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N U C L E A R PHYSICS A

ELSEVIER Nuclear Physics A 624 (1997) !-124

The NUBASE evaluation of nuclear and decay properties

G. Audi a, O. Bersillon u, J. Blachot h, A.H. Wapstra c a Centre de Spectromdtrie Nucldaire et de Spectromdtrie de Masse, CSNSM, IN2P3-CNRS, Batiment 108,

F-91405 Orsay Campus, France b Service de Physique Nucldaire, CEA, B.P. 12, F-91680 Bruydres-le-Ch~tel, France

c National Institute of Nuclear Physics and High-Energy Physics, NIKHEE PO Box 41882, I O09DB Amsterdam, The Netherlands

Received 27 August 1997; accepted 27 August 1997

Abstract

This paper presents the first version of the NUBASE evaluation of nuclear and decay properties of nuclides in their ground- and isomeric-states. All nuclides for which some experimental information is known are considered. NUBASE has basically been derived from the "Evaluated Nuclear Structure Data Files" and from the "Atomic Mass Evaluation" of 1995, but it also includes information from recent literature or literature missed in one of these two evaluations and is meant to cover all experimental data along with their references. In case no experimental data is available, whenever possible, trends in the systematics of neighboring nuclides have been used to derive estimated values (labeled in the database as non-experimental). Adopted procedures and policies are presented.

@ 1997 Elsevier Science B.V.

1. Introduct ion

We considered that the nuclear physics community from basic physics to applied

nuclear sciences would greatly benefit from a database which contains values for the

main basic nuclear properties such as masses, excitation energies of isomers, half-lives,

spins and parities, decay modes and their intensities. A requirement is that all the

information should be properly referenced in that database to allow checks on their validity.

One of the applications of such a database is the "Atomic Mass Evaluation" (AME)

in which it is essential to have clear identification of the states involved in a decay,

a reaction or a mass-spectrometric line. Furthermore, calculations requiring radioactive

0375-9474/97/$17.00 @ 1997 Elsevier Science B.V. All rights reserved. PII S0375-9474(97)00482-X

2 G. Audi et al./Nuclear Physics A 624 (1997) 1-124

parameters for nuclear applications (e.g. reactors, waste management, nuclear astro-

physics) need to access this basic information on any nuclide. In the preparation of a nuclear physics experiment, such a database could also be quite useful.

Most of the data mentioned above are in principle already present in two evaluated files: the "Evaluated Nuclear Structure Data Files" (ENSDF) [1] and the "Atomic Mass Evaluation" of 1995 (AME'95) [2]. The demand above could be thus partially fulfilled by combining them in a 'horizontal' structure (which exists in the AME, but not in ENSDF). NUBASE is therefore, at a first level, a critical compilation of these two

evaluations. In making this, we found it necessary to examine the literature, firstly, to revise

several of the collected results and insure that the mentioned data are presented in a more unique way; secondly, to have as far as possible all the available experimental data included, not only the recent ones (updating requirement), but also those missed in ENSDF and/or in AME (completeness requirement). This implied some evaluation

work, which appears in the remarks added in the NUBASE table and in the discussions below. Full references are given for all of the added experimental information (cf. 2.7.

References). The cut-off date for the data from literature used in the present NUBASE'97 evaluation

was December 31, 1996. Some post cut-off date works, available before August 31, 1997, were also included, but only in remarks to the relevant data.

The contents of NUBASE are described below, along with some of the policies adopted

in this work. Updating procedures of NUBASE are presented in Section 3. Finally, the electronic distribution of NUBASE and an interactive display of its contents with a World Wide Web Java program or with a PC-program are described in Section 4.

2. Contents of NUBASE

NUBASE contains experimentally known nuclear properties together with some values estimated by extrapolation of experimental data for 3010 nuclides. NUBASE also contains data on those isomeric states that have half-lives greater than 1 millisecond; there are 669 such nuclides of which 58 have more than one isomeric state.

For each nuclide ( A , Z ) , and for each state (ground or isomeric), the following quantities have been compiled, and when necessary evaluated: mass excess, excitation energy of the isomeric states, half-life, spin and parity, decay modes and intensities for each mode, isotopic abundances of the stable nuclei, and references for all experimental values of the above items.

In the description below, references to works that are also quoted in the NUBASE table are given with the same Nuclear Structure Reference key number style [ 3 ]. They are listed at the end of the main table.

The names and the chemical symbols of the elements 104 to 109 as recommended recently by the Commission on Nomenclature of Inorganic Chemistry of the International Union of Pure and Applied Chemistry (IUPAC) were used: 104 dubnium (Db), 105

G. Audi et al./Nuclear Physics A 624 (1997) 1-124 3

joliotium (J1), 106 rutherfordium (Rf), 107 bohrium (Bh), 108 hahnium (Hn), and

109 meitnerium (Mt), while the provisional symbols Xa and Xb were used for the

elements 110 and 111. It is known to the present authors that a new set o f suggestions has been made. The choice mentioned above is made for convenience and does not

express a preference. As in the AME'95 evaluation, we took care in having continuity of the set of the

considered nuclides at the same time in N, in Z, in A and in N - Z.

As far as possible, one standard deviations ( 1 o-) are given to represent the uncertainties connected with the experimental values. Unfortunately, authors do not always define

the meaning of the uncertainties they quote; under such circumstances, the uncertainties

are assumed to be one standard deviations. In not a few cases, the uncertainties are not

given at all; we then estimated them on the basis of the limitations of the method of

measurement. Values and errors that are given in the NUBASE table have been rounded, even

if unrounded values were found in ENSDF or in the literature. In cases where the

two furthest-left significant digit in the error were larger than a given limit (30 for the energies, to maintain strict identity with AME'95, and 25 for all other quantities), values

and errors were rounded off (examples: 2345.67 + 2.28 ~ 2345.7 ± 2.3, 2345.67 +

4.68 ~ 2346 + 5, 2346.67 -4- 46.82 ~ 2350 + 50, 2345.6789 + 0.0068 ~ 2345.679 +

0.007). When we felt it necessary, and to allow traceability, we added a remark with

the original value. When no experimental data exist for a nuclide, values can often be estimated from

observed trends in the systematics of experimental data. In the AME'95, masses estimated

from systematic trends were already flagged with the symbol '#'. The use of this symbol

is being extended in the present work to all other quantities and has the same meaning of indicating non-experimental information.

2.1. M a s s excess

The mass excess is defined as the difference between the atomic mass (in mass units)

and the mass number, and is given in keV for each nuclear state together with its one standard deviation uncertainty. The mass excess values given in NUBASE are those of

the AME'95 evaluation [2]. No values were changed here, since a new evaluation of masses would have required a considerable extra effort.

It sometimes happen s that knowledge on masses can yield information on the decay modes, in particular regarding nucleon-stability. Such information has been used here, as can be seen in the table for 1°He, 19Na, 39Sc, 62As or 63As.

Fig. 1 complements the main table in displaying the precisions on the masses, in a color-coded chart, directly as a function of N and Z. NUBASE includes nuclides that were not in the AME'95. They appear in light grey in Fig. 1, and no mass values are

given in the table.

4 G. Audi et al. /Nuclear Physics A 624 (1997) 1-124

o R

C) (v)

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~ O ~

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w 4 i 0 ~

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e •

0 e

0

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2.2. ~ o m e ~

For this first version of NUBASE we have adopted a simple definition for the isomers: they are excited states that live longer than 1 millisecond. Isomers are given in order of

increasing excitation energy and identified by appending 'm' or 'n' to the nuclide name, e.g. 122Cs for the ground-state, 122Csm for the first isomeric state, and 122Csn for the

second isomeric state. It was not necessary to give a notation for more isomers, except

that for one nuclide, 178Ta, three isomers are known to exist. For this nuclide we give then, in a remark to 178Tan (the second isomer), the available data for this third isomer.

The definition of isomers as excited states that live longer than 1 millisecond is

a simple one, but does not go without drawbacks, particularly for alpha and proton

decaying nuclides. For fl-decay a limit of 1 millisecond is acceptable, since the shortest- lived known fl-decaying nuclide (35Na) has a half-life of 1.5 millisecond. But for alpha

or proton decay, several cases are known where an isomer with a half-life far below 1

millisecond lives still longer than the ground-state. In a future version, NUBASE will

certainly amend the rule above, but here we decided not to accept more than a few exceptions. One of them is the newly discovered proton emitter 185Bi" with 44/xs half-

life; the ground-state of 185Bi is yet unknown, with an estimated half-life of 2 seconds.

Another exception is 187Bim with a half-life of 0.8(0.6) millisecond compatible with the

1 millisecond limit. The excitation energy can be derived from a number of different experimental meth-

ods. When this energy is derived from a method other than y-ray spectrometry, the origin is indicated by a two-letter code and the numerical value is taken from AME.

Otherwise, the code is left blank and the numerical value is taken from ENSDF or from

literature update. When the existence of an isomer is under discussion (e.g. 141Tbm) it is flagged with

'EU' in the origin field to mean "existence uncertain". A comment is generally added to indicate why its existence is questioned, or where this matter has been discussed.

Depending on the degree of our confidence in this existence, we can still give a mass excess value and an excitation energy, or omit them altogether (e.g. 138pmn). In the

latter case, the mention "non-existent" appears in place of that excitation energy. When an isomer has been reported, and later proved not to exist (e.g. 184Lure), it is

flagged with 'RN' in the origin field. In such case we give of course no mass excess

value and no excitation energy, and, as in the case of the 'EU's above, they are replaced

by the same mention "non-existent". In several cases ENSDF gives a lower and a higher limit for an isomeric excitation

energy. A uniform distribution of probabilities has been assumed which yields a value at the middle of the range and a lo- uncertainty of 29% of that range [4]. An example is 136La for which it is known that the isomer lies above the level at 230.1 keV, but,

as explained in ENSDF, there are good experimental indications that the difference between these two levels cannot exceed 22 keV. We presented this information as E = 241 (7) keV. However, if that difference would have been derived from theory or

from systematics, the resulting E would have been considered as non-experimental and


the value flagged with the '#' symbol. In case that the uncertainty o- on the excitation energy E is relatively large compared

to the value, the assignment to ground state and isomeric state is uncertain. If o- > E l 2

a flag is added in the NUBASE table. As a result of this work, the orderings of several ground-states and isomeric-states

have been reversed compared to those in ENSDF. They are flagged in the NUBASE table

with the '&' symbol. In several cases we found evidence for a state below the adopted ENSDF ground-state. Also, in many other cases, the systematics of nuclides with the same parities in N and Z strongly suggest that such a lower state should exist. They have been added in the NUBASE table and can be located easily, since they are also flagged with the '&' symbol. In a few cases, new information on masses can also lead to reversal of the level ordering. However, following the policy defined above for this first release of NUBASE, in maintaining strict compatibility with AME'95, the exchange

of the two levels has then not been made. Instead, the information is given in an added

remark.

News on isomeric excitation energies

Interestingly, the rather new technique of investigating proton decay of very proton- rich nuclides has given new information on isomeric excitation energies. Thus, such work on 167Ir [97Da07] now showed that it has an isomeric excitation energy E = 175.3(2.2) keV rather than the AME'95 value 220#(90#) keV. In addition, study of the a-decay series of these activities not only showed that a number of a lines earlier assigned to ground-states belong in reality to isomers, but also allowed to derive values for their excitation energies. Notes in the table refer to several of these cases.

Another case of such a change is 181pb. The a decay half-life that was assigned to 181pb" in AME'95 is now assigned to the ground-state, following the work of [96To01 ]

who showed, first, that contrary to a previous work, there is no a line at higher energy than the one just mentioned, and second, that the observed a is in correlation with the decay of the daughter 177Hg, which is also most probably a 5 / 2 - state.

2.3. Half-life

For some light nuclei, the half-life (7"1/2) is deduced from the level total width (Ucm)

by the equation I'cm T1/2 ~- hln2 :

T1/2 (s) '~ 4.562 10-22/Fcm (MeV).

Quite often uncertainties for half-lives are given asymmetrically T_+~. If these uncertainties are used in some applications, they need to be symmetrized. In AME'95 a simple rough symmetrization was used: take the central value to be the mid-value between the upper and lower lo'-equivalent limits T + (a - b ) / 2 , and define the uncertainty to be the average of the two uncertainties (a + b) /2 . The validity [ 5] of this relatively simple procedure was further investigated and we found, from a more strict statistical derivation (see Appendix), that a better approximation for the central value is obtained by using

G. Audi et aL/Nuclear Physics A 624 (1997) 1-124

T ÷ 0.64 × (a - b). The more complex expression for the uncertainty is given in the

Appendix. In the case of experiments in which extremely rare events are observed, and where

the results are very asymmetric, we did not average directly the half-lives derived from different works, but instead, when the information given in the papers was sufficient (e.g. 264Hn or 267Hn), we combined [84Sc13] the delay times of the individual events.

Some measurements are reported as a range of values with most probable lower and upper limits. They were treated, as above (cf. 2.2. Isomers), as a uniform distribution

of probabilities with a value at the middle of the range and a lo- uncertainty of 29% of

that range. For some nuclides identified by using a time-of-flight spectrometer, an upper or a

lower limit on the half-life is given. For observed species, we just used for lower limit the time-of-flight of the nuclides in the spectrometer. The user of our table should be careful in that this limit can be very far below the eventually measured half-life.

Upper limits for undetected nuclides have been evaluated for NUBASE by E Pougheon [93Po.A], based on the time-of-flight of the experimental setup and the yields expected

from the trends in neighboring nuclides. When half-lives for nuclides with the same parities in Z and N are found to vary

smoothly (see Fig. 2), interpolation or extrapolation is used to obtain reasonable esti-

mates.

2.4. Spin and parity

As in ENSDF, values are presented without and with parentheses based upon strong and weak assignment arguments, respectively (see the introductory pages of Ref. [6] ). The latter include estimates from systematics or theory. Where we could distinguish them, we used parentheses if the so-called "weak" argument was an experimental one,

but the symbol '# ' in the other cases. The survey might have not been complete, and the reader might still find non-flagged non-experimental cases (the authors will gratefuly acknowledge mention of such cases that will help improve future versions of NUBASE).

If spin and parity are not known from experiment, they can be estimated, in some cases, from systematic trends in neighboring nuclides with the same parities in N and Z. This is often true for odd-A nuclides (see Fig. 3 and Fig. 4), but also, not so rarely, for odd-odd ones, as can be seen in Fig. 5. These estimated values are also flagged with the '# ' symbol. In several cases we replaced the ENSDF systematics by our own.

The review of nuclear radii and moments of Otten [ 89Ot. 1 ], in which the spins were compiled, was used to check and complete the spin values in NUBASE.

2.5. Decay modes and intensities

The most important policy, from our point of view, in coding the information for the decay modes, is in establishing a very clear distinction between a decay mode that is energetically allowed but not experimentally observed (represented by a question mark

8 G. Audi et al . /Nuclear Physics A 624 (1997) 1-124

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10 G. Audi et aLINuclear Physics A 624 (1997) 1-124

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G, Audi et al./Nuclear Physics A 624 (1997) 1-124 11

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alone, which thus refers to the decay mode itself), and a decay mode that is actually observed but for which no intensity could be determined (represented by '=?', the

question mark referring here to the quantity after the equal sign). As in ENSDF, no corrections have been made to normalize the primary intensities to

100%. Besides direct updates from the literature, we also made use of partial evaluations

by other authors (with proper quotation). They are mentioned below, when discussing

some particular decay modes.

The fl+ decay In the course of our work we refined some definitions and notations for the fl+ decay,

in order to present more clearly the available information. We denote with fl+ the decay process that includes both electron capture, denoted e, and the decay by positron emission, denoted e +. As is well known, for an available energy below 1022 keV, only electron capture is allowed; above that value both processes compete. This notation is not the same as the one implicitly used in ENSDF, where the combination of both modes

is denoted "EC+B+" . When both modes compete, the separated intensities are not always available from

experiment. Most of the time, separated values in ENSDF are calculated ones. In continuation of one of our general policies in which we retain whenever possible only experimental information, we decided not to retain ENSDF'S calculated separated values (which are scarce and moreover not always updated). Only in some very particular cases is the distinction of importance, like in the case of rare or extremely rare processes (e.g. 91Nb, 54Mn). Then, the use of our notation is useful.

Similarly, we give both electron capture e-delayed fission and the positron e+-delayed

fission with the same symbol fl+SE

The double-fl decay In the course of our work we found that half-lives for double-fl decay were not

always given in a consistent way in ENSDF. For NUBASE we decided to give only half-life values or upper-limits related to the dominant process, which is in general the 2 neutrino gs-gs transition (one exception may be 98Mo, for which the neutrinoless decay

is predicted to be faster, see [95Tr07] ). No attempt was made to convert to the same statistical confidence level (CL) upper limit results given by different authors.

The excellent recent compilation of Tretyak and Zdesenko [95Tr07] was of great

help in this part of our work.

The fl-delayed decays For delayed decays, intensities have to be considered carefully. By definition, the

intensity of a decay mode is the percentage of decaying nuclei in that mode. But traditionally, the intensities of the pure fl decay and of those of the delayed ones are summed to give an intensity that is assigned to the pure decay. For example, if the (A,Z)


nuclide has a decay described, according to the tradition, by 'fl-=100; f l -n=20' , this means that for 100 decays of the parent 80 (A ,Z+I ) and 20 (A -1 ,Z+I ) daughter nuclei are produced and that 100 electrons and 20 delayed-neutrons are emitted. A strict notation would have been in this case ' f l-=80; fl-n=20' . However we decided to follow

the long-lived tradition and give also 'fl-=100; fl-n=20' . This also holds for more complex delayed emissions. A decay described by: 'f l-=100;

fl-n=30; fl-2n=20; f l - a=10 ' corresponds to the emission of 100 electrons, 70 delayed- neutrons and l0 delayed-re particles; and in terms of residual nuclides, to 40 ( A , Z + I ) , 30 ( A - 1 , Z + I ) , 20 ( A - 2 , Z + I ) and 10 (A-4,Z-1) . More generally, Pn, the number of

emitted neutrons per 100 decays, can be written:

Pn = Z i x fl/~; i

and similar expressions for tr or proton emission. The number of residual fl daughter

(A , Z+I ) is:

e - - Ee:n - Ze; - i j

Another special remark concerns the intensity of a particular fl-delayed mode. The primary fl decay populates several excited states in the fl-daughter, that will further decay by particle emission. However, in the case where the daughter's ground state also decays by the same particle emission, some authors included its decay in the value for the concerned fl-delayed intensity. We decided not to do so for two reasons. Firstly, because the energies of the particles emitted from the excited states are generally much higher than that from the ground-state, implying different subsequent processes. Secondly, because the characteristic times for the decays of the excited states are related to the parent, whereas those for the decays of the daughter's ground state are due to the daughter. For example 9C decays through fl+ mode with an intensity of 100% of which 12% and 11% to 2 excited p-emitting states in 9B, and 17% to an c~-emitting state. We give thus fl+p=23% and fl+a=17%, from which the user of our table can derive a 60% direct feeding of the ground-state of 9B. In a slightly different example, 8B decays only to 2 excited states in 8Be which in turn decay by ce and 7 emission, but not to the 8Be ground-state. We write thus fl+=100% and fl+a=100%, the difference of which leaves

0% for the feeding of the daughter's ground state. Finally, we want to draw to the attention of the user of our table that the percentages

are, by definition, related to 100 decaying nuclei, not to the primary beta-decay fraction. An illustrative example is given by the decay of 2a8Np, for which the delayed-fission probability is given in the original paper as 0.020(9)% [94Kr13], but this number is relative to the • process, the intensity of which is 59(7)%. We thus renormalized the delayed-fission intensity to 0.012(6)% of the total decay.

In collecting the delayed proton and c~ activities, the remarkable work of Hardy and Hagberg [89Ha.l], in which this physics was reviewed and discussed, was an


appreciable help in our work. The review of Honkanen, ,~yst6 and Eskola [7] on delayed-protons has also been checked.

Similarly, the review of delayed neutron emission of Hansen and Jonson [89Ha.2] was carefully examined and used in our table, as well as the evaluation of Rudstam, Aleklett and Sihver [93Ru01].

Spontaneous fission The evaluation of Lorenz [ 86Lo.A] for spontaneous fission intensities has been used

here.

6H and multi-neutron emission In the very special case of 6H, we mention as possible decay channels 3-neutron and

4-neutron emissions. The reason is that, based on the observed mass values, both its Sn and S2n separation energies are positive, which makes it stable against 1-neutron and 2-neutron emission, but not against 3n or 4n emission. 6H decays with a half-life of 320(60) yoctoseconds. Its mass value is derived from two 7Li(7Li,8B) experiments and one 9Be(I1B,140). If this mass value is confirmed, 6H would be a unique laboratory for

searching for simultaneous 3n or 4n emission.

2.6. Isotopic abundances

Isotopic abundances are taken from Ref. [8] and are listed in the decay field with the symbol IS. They are displayed as given in the compilation of Holden, i.e. we did

not even apply our rounding policy.

2.7. References

The year of the archival file is indicated for the nuclides evaluated in ENSDF; other-

wise, this entry is left blank. References for all of the experimental updates are given by the NSR key number

[ 3 ], followed by one, two or three one-letter codes which specify the added or modified physical quantities (see the Explanation of Table). In cases where more than one reference is needed to describe the updates, they are given in a remark. No reference is given for systematic values. The ABBW reference key is used in cases where it may not appear unambiguously that re-interpretations of the data were made by the present authors.

3. Updating procedure

NUBASE is updated via two routes: from ENSDF after each new A-chain evaluation, and directly from the literature.


.o.!.

8,...:- ...... i ..... L IIOIUlln~

o

c)

. , . . . . . . , . . . . . . . , . . . . . ,

(o

8 F-- . . . . . ~ ° ~ . o g . J o o ~ o e e ~ m e e t o m m t . o o l , w o o . . . ~ w l i . n

ZD t 0 o~ . ° . ° ° °1 ° . ~ o ° ° ° . . ~ o ° . . . ° . ~ - . - . o - ~ - o ° o ° o ° p - o ° - ,

• mme . . , a . i . ~ . , imm.sg ea . . . . . . e . eoQ I o . l oo . o .m . . o eoo ,

.iSNiO±iO id e e e I o e e

e I t i i o o i i t J i i 0 i e 8 I I O I i e t e 0

I I I e e O O I O I O I I I e o i I i e o e e e o l l o l o I i i I i e l o l I e e I I I I e i i i e o e i

' I : I I i

0 0 0 0 0 0

o

4~

e -

C..2


ENSDF files are retrieved from NNDC using the on-line service [ 1 ] and transferred through Internet. Two of the present authors [9] developed programs to successively: • check that each Z in the A-chain has an 'adopted levels' data set; if not, a corresponding data set is generated from the 'decay' or 'reaction' data set, • extract the 'adopted levels' data sets from ENSDF, • extract from these data sets the required physical quantities, and convert them into a format similar to the NUBASE format.

The processed data are used to update manually the previous version of NUBASE. This step is done separately by the four authors and cross-checked until full agreement

is reached. The ENSDF is updated generally by A-chains, and, more recently, also by individual

nuclides. Its contents however is very large, since it encompasses all the complex nuclear structure and decay properties. This is a huge effort, and it is no wonder that some older

data (including annual reports, conference proceedings, and theses) are missing, and that some recent data have not yet been included. Where we notice such missing data, they are analyzed and evaluated, as above, independently by the four authors and the proposed updatings are compared. Most often these new data are included in the next ENSDF evaluation and the corresponding references can be removed from the NUBASE

database.

4. Distribution and displays of NUBASE

An electronic ASCII file for the NUBASE table, for use with computer programs, is

distributed by the Atomic Mass Data Center (AMDc) [ 10] through anonymous f tp and through the World Wide Web. This file will not be updated, to allow stable reference data for calculations. Any work using that file should make reference to the present paper and not to the electronic file.

The contents of NUBASE can be displayed by a Java program JVNUBASE [ 11 ] through the World Wide Web and also with a PC-program called "Nucleus" [ 12]. Both can be accessed or downloaded from the AMDC. They will be updated regularly to allow the user to check for the latest available information in NUBASE.

5. Conclusions

A 'horizontal' evaluated database has been developed which contains some of the main properties of the nuclides in their ground and isomeric states. These data originate from a critical compilation of two evaluated datasets (ENSDF and AME) updated and completed from the literature. The guidelines in setting up this database were to cover as completely as possible all the experimental data, and to provide proper reference for those used in NUBASE and not already included in ENSDF; this traceability allows any user to check the recommended data and, if necessary, undertake a re-evaluation.


As a result of this 'horizontal' work, a greater homogeneity in data handling and

presentation has been obtained for all of the nuclides. Furthermore, isomeric assignments

and excitation energies have been reconsidered on a firmer basis and their data improved. It is expected to follow up this first version of NUBASE with improved treatments.

Among them, we plan to extend the definition of isomer to states with half-lives shorter

than 1 millisecond in order to better describe nuclides decaying by a or proton emission. Also, isomers with half-life as short as 1 microsecond are produced together with longer

lived ones in experiments at the large-scale facilities. Another foreseeable implementation would be to provide the main a, y, conversion and X-ray lines accompanying the decays. NUBASE could also be extended to other nuclear properties: radii, moments. . . An interesting feature that is already implemented, but not yet checked sufficiently to be included here, is to give for each nuclide, in ground or isomeric-state, the year of its discovery.

Acknowledgements

We wish to thank our many colleagues who answered our questions about their experiments and those who sent us preprints of their papers. Continuous interest, discussions and suggestions of C. Thibault were highly appreciated. Our thanks to F. Pougheon, C. Borcea, A. Gizon and C.E Liang for enlightening discussions. We appreciate the help provided by M. Martin and J.K. Tuli in solving some of the puzzles we encoun- tered. The help of the NNDC at Brookhaven laboratories is highly appreciated, more particularly from T.W. Burrows regarding the ENSDF library. Our thanks to E Bouvot and S. Audi for preparing the color figures in this paper and to P. Pearson at Elsevier for a particularly good cooperation in preparing the present publication. A.H.W. expresses his gratitude to the NIKHEF laboratory and J.B. to the ISN-Grenoble, DRFMC-Grenoble and CSNSM-Orsay laboratories for permission to use their facilities.

Appendix A. Symmetrization of asymmetric uncertainties

Experimental data are sometimes given with asymmetric uncertainties, X+_~. I f these data are to be used with other ones in some applications, their uncertainties may need to be symmetrized. A simple method (Method 1) consisted in taking the central value to be the mid-value between the upper and lower 1 o'-equivalent limits X + ( a - b ) /2 ,

and define the uncertainty to be the average of the two uncertainties (a + b) /2 .

An alternative method (Method 2) is to consider the random variable x associated with the measured quantity. For this random variable, we assume the probability density function to be an asymmetric normal distribution having a modal (most probable) value of x = X, a standard deviation b for x < X, and a standard deviation a for x > X (Fig. A.1 ). Then the average value of this distribution is

(x) = X + V/2/Tr (a - b),


I f _ "X, j b a N, x

X m

Fig. A.I. Simulated asymmetric probability density function (heavy solid line) and the equivalent symmetric one (dashed line).

with variance

0 -2 = ( 1 - 2/~r) ( a - b) 2 + ab. (A.1)

The median value m which divides the distribution into two equal areas is given, for

a > b, by

erf m - X a - - b (A.2)

and by a similar expression for b > a.

We define the equivalent symmetric normal distribution we are looking for as a

distribution having a mean value equal to the median value m of the previous distribution

with same variance 0-.

If the shift m - X of the central value is small compared to a or b, expression (A.2)

can be written [ 13] :

m - X -~ V/-#-/8 (a - b) -~ 0.6267 ( a - b).

In order to allow for a small non-linearity that appears for higher values of m - X, we

adopt for Method 2 the relation

m - X = O . 6 4 ( a - b ) .

Table A. 1 Examples of treatment of asymmetric uncertainties for half-lives. Method 1 is the classical method as used in AME'95 and in the present work for masses and excitation energies. Method 2 is the one developed here and used for half-lives and intensities of the decay modes.

Nuclide Original TI/2 Method 1 Method 2

65As 190+110-70 ms 210 4- 90 220 4- 90 222U 1.0+1.0-0.4 /.*s 1.3 + 0.7 1.4 4- 0.7 264Hn 80+400-40 /zs 260 4- 220 310 4- 250 266Mt 3.4+6.1-1.3 ms 5.8 4- 3.7 6.5 4- 4.0

G. Audi et al . /Nuclear Physics A 624 (1997) 1-124 19

Table A.1 i l lustrates the results f rom both methods. In NUBASE, Method 2 is used

for the symmet r i za t ion o f asymmetr ic half- l ives and o f asymmetr ic decay intensities.

References

References such as 86Lo.A, 89Ha.1 or 96To01 are listed under "References to the NUBASE table "(p.l lO).

[ 1 ] T.W. Burrows, Nucl. Instrum. Meth. 286 (1990) 595. [2] G. Audi and A.H. Wapstra, Nucl. Phys. A 595 (1995) 409. [3] Nuclear Structure Reference (NSR): a computer file of indexed references maintained by NNDC,

Brookhaven National Laboratory. [4] G. Audi, M. Epherre, C. Thibault, A.H. Wapstra and K. Bos, Nucl. Phys. 378 (1982) 443. [5] G. Audi, O. Bersillon, J. Biachot and A.H. Wapstra, Nucl. Instrum. Meth. A369 (1996) 511. [6] General Policies, Nuclear Data Sheets, 71 (1994) v. [7] J. Honkanen, J..~yst6 and K. Eskola, Phys. Scr. 34 (1986) 608. [8] N.E. Holden, Report BNL-61460 (1995) and private communication to J.K. Tuli (Nuclear Wallet

Cards). [91 O. Bersillon and J. Blachot, NEANDC(E) 246/L, INDC(FR) 071/L, September 1991.

[ 10] The NUBASE file in the electronic distribution can be retrieved from the Atomic Mass Data Center by anonymous ftp to: csnftp.in2p3.fr, in directory /pub/AMDC, or through the Web at the address http://csnwww.in2p3.fr/amdc/.

[ 11 ] E. Durand, Report CSNSM 97-09, July 1997. [12] B. Potet, J. Duflo and G. Audi, Proceedings ENAM'95 conference, Aries, June 1995, p. 151. [13] R.D. Evans, The Atomic Nucleus (McGraw-Hill, New York, 1955) p. 766.

20 G. Audi et aL/Nuclear Physics A 624 (1997) 1-124

NUBASE t a b l e

E X P L A N A T I O N O F T A B L E

D a t a a r e p r e s e n t e d in g r o u p s o r d e r e d a c c o r d i n g to i n c r e a s i n g m a s s n u m b e r A.

Nuclide Nuclidic name: mass number A = N + Z and element symbol (for Z > 103 see Section 2).

Mass excess Mass excess [M(in u ) - A ] , in keV, and its one standard deviation uncertainty as given in the most recent "'Atomic Mass Evaluation" (AME'95). No updatings have been made for mass-excesses or for isomeric excitation energies. When important new information exist, remarks have been added. The rounding policy is that of AME'95.

# in place of decimal point: value and uncertainty derived not from purely experimental data, but at least partly from systematic trends (cf. AME'95).

Energy difference, in keV, between levels adopted as higher level and ground state, and its one standard deviation uncertainty, as given in AME'95 (see explanation for "Mass excess" above).

# in place of decimal point: value and uncertainty derived from systematic trends (see above).

The excitation energy is followed by its origin code when derived from a method other than T-ray spectrometry:

MD Mass doublet RQ Reaction energy difference AD a energy difference BD fl energy difference p proton decay Nm estimated value derived with help of Nilsson model

When the existence of an isomer is questionable, the following codes are used: EU existence of isomer is under discussion (e.g. 141Tbm).

If existence is strongly doubted, no excitation energy and no mass are given. They are replaced by the mention "non-existent" (e.g. 138pmn).

RN isomer is proved not to exist (e.g. 18aLum). Excitation energy and mass are replaced by the mention "non-existent".

Isomeric assignment:

* In case the uncertainty o- on the excitation energy E is larger than half that energy (o- > E/2) an asterix has been added (e.g. i3°In and 13°Into).

& In case the ordering of the ground- and isomeric-states have been reversed compared to ENSDF, an ampersand sign has been added (e.g. 87Nb and 87Nbm).

Excitation energy

Half-life

j~r

Ens

Reference

G. Audi et al./Nuclear Physics A 624 (1997) 1-124

s = seconds; m = minutes; h = hours; d = days; y = years; 1 y (tropical year 1900) = 31 556 925.974 7 s

or 365.242 198 78 d STABLE = stable nuclide or nuclide for which no finite value for half-life

has been found.

# value estimated from systematic trends in neighboring nuclides with the same Z and N parities.

subunits: ms: l0 -3 s millisecond ky: l03 y kiloyear /.zs: 10 -6 s microsecond My: l0 6 y megayear ns: 10 - 9 s nanosecond Gy: 10 9 y gigayear ps; 10 -12 s picosecond Ty: 1012 y terayear fs : 10 -15 s femtosecond Py: l015 y petayear as: l0 -18 s attosecond Ey: l018 y exayear zs: I0 -21 s zeptosecond Zy: l021 y zettayear ys" 10 -24 s yoctosecond Yy: l024 y yottayear

Spin and parity: ( ) uncertain spin and/or parity. # values estimated from systematic trends in neighboring nuclides with the same Z

and N parities. high high spin. low low spin.

Year of the archival file of the ENSDF.

Reference keys: 92Pa05 Updates to ENSDF derived from regular journal. These keys are taken from

Nuclear Data Sheets. Where not yet available, the style 97Ya.l has been used. 95Am.A Updates to ENSDF derived from abstract, preprint, private communication, con-

ference, thesis or annual report.

The reference keys are followed by one, two or three letter codes which specifies the added or modified physical quantities:

T for half-life J for spin and/or parity E for the isomer excitation energy D for decay mode and/or intensity I for identification

21

22

Decay modes and

intensities


Decay modes followed by their intensities (in %), and their one standard deviation uncertainties. The special notation 1.8e-12 stands for 1.8 x 10 -12. The ordering is according to decreasing intensities.

Ot

p 2p n 2n E

e +

/3+ /3- 2/3- 2/3 + /3 -n /3-2n /3+p /3+2p /3-tr

/3-d IT SF fl+SF /3-SF 24Ne

a emission proton emission 2-proton emission neutron emission 2-neutron emission electron capture positron emission fl+ decay (/3+ = ~ + e + ) /3- decay double/3- decay double/3+ decay /3- delayed neutron emission /3- delayed 2-neutron emission /3+ delayed proton emission /3+ delayed 2-proton emission /3- delayed a emission /3+ delayed a emission /3- delayed deuteron emission internal transition spontaneous fission /3+ delayed fission /3- delayed fission heavy cluster emission list is continued in a remark, at the end of the A-group

For long-lived nuclides: IS Isotopic abundance

A remark on the corresponding nuclide is given below the block of data corresponding to the same A.

Remarks. For nuclides indicated with an asterix at the end of the line, remarks have been added. They are collected in groups at the end of each block of data corresponding to the same A. They start with a code letter, like the ones for the "Reference" above, indicating to which quantity the remark applies. They give:

(i) Continuation for the list of decays. In this case, the remark starts with three dots. (ii) Information explaining how a value has been derived.

(iii) Reasons for changing a value or its uncertainty as given by the authors or for rejecting it. (iv) Complementary references for updated data. (v) Separate values entering an adopted average.

(vi) The original value and its upper and lower uncertainties in the case of an asymmetric result (see Section 2.3 and Appendix).

(vii) New data on masses that were not included in the most recent "Atomic Mass Evaluation" (AME'95) but that are of importance in determining the isomeric ordering or the isomeric excitation energy.

(viii) Post cut-off date (December 31, 1996) information.


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities (keV) euergy(keV ) (%)

In 8071.323 0.002 614.6 s 1.1 1/2 + 94 96By03 T /3 -=100 IH 7288.969 0.O01 STABLE 1/2 + 94 IS=99.985 1

*In T : mean life 96By03=889.2(4.8) s combined with 7 other values, see 96By03

2H 13135.720 0.001 STABLE 1 + 94 IS=0,015 1

3H 14949.794 0.001 12.33 y 0.06 1/2 + 96 fl-=100 3He 14931.204 0.001 STABLE 1/2 + 87 IS=0.000137 3

4H 25930 110 4He 2424.911 0.001 4Li 25320 210

*4H T : from 91Go19 *4Li T : from 65Ce02

100 ys 20 2 - 82 92Ti02 D n=100 STABLE 0 + 94 IS--99.999863 3

91 ys 9 2 - 94 92"fi02 D p=100

5H 36830 950 5He 11390 50 5Li 11680 50 5Be 38000# 4000#

*SH T : average 91Go19=66(25) 95AI.A=l10

80 ys 30 1/2+# 84 95AI.A TD n=100 760 ys 30 3/2-- 84 n=100 300 ys 3 / 2 - 84 p=100

1/2+# 84 p ?

6H 41860 260 6He 17594.1 1.0 6Li 14086.3 0.5 6Be 18374 5

*6H T : from 86Be35

320 ys 60 ( 2 - ) 84 88Aj01 DJ 3n ?; 4n ? 806.7 ms 1.5 0 + 84 90Ri01 D /3-=100; fl--d---0.00028 5

STABLE 1 + 94 IS=7.5 2 5.0 zs 0.3 0 + 84 2p=100

D : see discussion in the text

7He 26110 30 2,9 zs 0.5 (3/2) -- 89 7Li 14907.7 0.5 STABLE 3/2-- 89 7Be 15769.5 0.5 53,29 d 0.07 3 / 2 - 89 7B 27870 70 350 ys 50 ( 3 / 2 - ) 89

*TBe T : average of 3 values in ENSDF. See also 96Ja10=53.12(0.07)

n=100 IS=92.5 2 *=100 p=100

8He 31598 7 119.0 ms 1.5 0 + 89 88Aj01 D 8Li 20946.2 0.5 838 ms 6 2 + 89 88.~i01 D 8Be 4941.66 0.04 67 as 17 0 + 94 8B 22921.0 1.1 770 ms 3 2 + 89 88A j01 D 8C 35094 23 2,0 zs 0.4 0 + 89

*8He D : f l - n intensity is from 88Aj01; / ~ - t intensity from 86Bo41 *SLi D : /3-- decay to first 2 + state in 8Be. which decays 100% in 2 a *SB D : fl+ to 2 excited states in 8Be, then a and 7, but not to 8Be ground-state

/3-=100; /3--n=16 1 ; /3 - t=0 .9 1 * /3-=100; ~ - a=lO0 . a=lO0 #%100; /~+ a=10o . 2t~100

9He 40820 60 7 zs 4 1 / 2 - # 89 88Aj01 D n=100 9Li 24953.9 1.9 178.3 ms 0.4 3/2-- 89 95Re.A D fl--=100; /3--n=50.8 2 9Be I IM7.6 0.4 STABLE 3/2-- 89 IS= 100. 9B 12415.7 1.0 800 zs ~ 0 3/2-- 94 p=100

9C 28913.7 2.2 126.5 ms 0.9 ( 3 / 2 - ) 89 88Aj01 D /5+=100; fl+p=23; f l+a=17 *gHe T : derived from width 100(601 keV in 95Bo.B *gLi D : also 92Te03 •--n=51(1)%, outweighed -9C D : fl+=12% and 11% to 2 excited p-emitting states in 9B, and 17% to a emitter

10He 48810 70 2.7 zs 1.8 0 + 94Os04 T 2n=100 10Li 33050 15 2.0 zs 0.5 ( 1 - , 2 - ) 89 94Yo01 TJ n=100 10Be 12606.6 0.4 1.51 My 0.06 0 + 88 f l - =100 t0B 12050.8 0.4 STABLE 3 + 94 IS=19.9 2 10C 15698.6 0.4 19.290 s 0.012 0 + 94 90Ba02 T /5'+=100 10N 39700# 400# 1 - # p ?

* 10He D : most probably 2 neutron emitter from $2n=-1070(70) keV


Nuclide Mass excess Excitation Half-life jcr Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

l lL i 40796 27 8.59 ms 0.14 3 / 2 - IIBe 20174 6 13.81 s 0.08 1/2 + 11B 8668.0 0.4 STABLE 3/2-- I I c 10650.5 1,0 20.39 m 0.02 3/2-- I tN 24960 180 500 ys 80 I /2 +

* l l L i D : . . . ; f l - 3n=1.9 2; /3-- not=l.00 6; ,8-- t--0.014 3; , 8 - d=0.013 5 .11Li D : , 8 - n, , 8 - 2n and /3 - 3n intensities are from 89Ha.2's evaluation; * l lLi D : ,8-not intensity is from 84La27; / 3 - d intensity from 96Mu19; * l lL i D : , 8 - t : average 84La27--0.010(4)% 96Mu19=0.020(5)% *dl lLi T : average 96Mu19=8.2(0.2) 95Re.A=8.4(0.2) 81Bj01=8.83(0.12) 74Ro31=8.5(0.2)

92 96Mu19 T 92 81A103 D ,8-=100; , 8 - a = 2 . 9 4 92 1S=80.1 2 92 ,8+=100 92 96Ax01 TJ p=100

12Li 50100# 1000# < 10 ns 74Bo05 T 12Be 25076 15 21.3 ms 0.1 0 + 94 95Re.A TD 12B 13368.9 1.4 20.20 ms 0.02 1 + 92 66Sc23 D 12C 0.0 0,0 STABLE 0 + 94 12N 17338.1 1.0 11.0130 ms 0.016 1 + 92 66Sc23 D 120 32048 18 580 ys 30 0 + 92 95Kr03 T

13Be 33660 500 2.7 zs 1.8 ( 1 / 2 - ) 95Pe12 T 13B 16562.2 1.1 17.36 ms (}.16 3/2-- 94 13C 3125.011 0.001 STABLE 1/2-- 94 13N 5345.46 0.27 9.965 m 0.004 1/2-- 94 130 23111 10 8.58 ms 0.05 ( 3 / 2 - - ) 93 70Es03 D

*13Be T : an upper limit of 10 ns was previously obtained by 74Bo05

14Be 39880 110 4,35 ms 0.17 0 + 93 14B 23664 21 12.3 ms 0.3 2 - 93 95Re.A TD 14C 3019,892 0.004 5.73 ky 0.1/4 0 + 94 14N 2863.417 0.17101 STABLE 1 + 94 140 8006.46 0.07 70.606 S 0.018 0 + 93 14F 33610# 400# 2 - #

ISB 28967 22 9.87 ms 0.07 3/2-- 93 95Re.A TD 15C 9873.1 0.8 2.449 s 0.005 1/2 + 94 tSN 101.438 0.001 STABLE 1 / 2 - 94 150 2855.4 0.5 122.24 s (I.16 1/2-- 94 ISF 16780 130 460 ys 90 (1/2 + ) 93

*ISB D : , 8 - 2 n intensity is from 89Re.A J : given in 91Aj01

I6B 370811 6(I < 19(I ps 0 - 96Kr05 T 16C 13694 4 747 ms 8 0 + 94 89Re.A D I6N 5683.4 2.6 7.13 s 0.02 2 - 94 74Ne10 D 160 --4736.998 0.001 STABLE 0 + 94 16 F 10680 8 11 z~s 6 0-- 93 16Ne 23992 20 9 zs 0 + 93

17B 4372(I 140 5.08 ms 0.05 ( 3 / 2 - ) 93 88Du09 D I7C 21037 17 193 ms 5 (3/2, 5/2) + 93 95Ba28 J 17N 7871 15 4.173 s 0,004 1/2-- 94 94Do08 D 170 --809.011 (I.2l STABLE 5/2 + 94 17F 1951.70 0.25 64.49 s 0.16 5/2 + 94 17Ne 1649(I 50 109.2 ms 0.6 I /2- - 93 88Bo39 D

*17B D : . . . ; ,8-- 3n=3.5 7; , 8 - 4n=0.4 3 * lTc T : avel'age 95Sc03=193(6) 95Re.A=I88(10) 86Cu01=202(17) *17C D : /3--n intensity is from 95Re.A

,8-=100; f l -n=84 .9 8; ,8-2n=4.1 4; . . . *

n ? ,8 -=100; , 8 - u=0.52 9 , 8 - = t 00 ; ,8-o t=l .6 3 IS=98.89 1 /6'/-=100; /3+0t=3.5 5 2p=60 30;/3'~ ?

n ? /3-=100; B-n--0.28 4 IS=I.II 1 fi t =100 ,8+=100; fl+p=10.9 20

f l - = 100 ; /3-n=81 4 ; / 3 - 2n=5 2 /3-=100; , 8 - n=6.04 23 / 3 - =100 IS=99.634 9

/3+=100 p ?

/3-=100; /3-n=93,6 12; / 3 - 2n--0.4 2 B - = 1 0 0 1S--0.366 9 /3+=100 p=100

n ? /3-=100; /3-n--97.9 23 ,8-=100; , 8 - a=O.O0100 7 1S=99.762 15 p=100 2p=100

fl-=lO0; , 8 - n--63 1; , 8 - 2u=ll 7; . . . /3-=100; ,8-n=28.4 13 /3-=100; /3-n--95 1; /3-a=0.0025 4 IS=0.038 3 / ~ = 1 0 0 /3+=100; /3+1~:96.0 9; /3+ot=2.7 9


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities (keV) energy(keV) (%)

18B 52320# 800# < 26 ns 4 - # 93Po.A T n ? 18C 24920 30 92 ms 2 0 + 96 95Sc03 T .8-=100; .8-n=31.5 15 * 18N 13117 20 624 ms 12 1 - 96 95Re.A D . 8 - =100; / 3 - n=10.9 9; . 8 - ot=12.2 6 *

180 --782.1 0.8 STABLE 0 + 96 IS=0.200 12 18F 873.4 0.6 109.77 m 0.05 1 + 96 ~ - = 1 0 0 18Ne 5306.8 1.5 1.672 s 0.008 0 + 96 fl+ =100

18Na 25320# 400# 1 - # p ?; 15 '+ ? • 18C D : .8--n intensity is from 95Re.A ** • 18N D : . 8 - n intensity is from 95Re.A; .8 - -a intensity from 89Zh04 **

19B 59360# 400# > 200 ns 3 / 2 - # 86Po13 T . 8 - ? 19C 32830 110 46.2 ms 2.3 (1/2 + ) 88Du09 TD .8-=100; .8-n--47 3; f l - 2 n = 7 3 * 19N 15860 16 271 ms 8 (1/2, 3/2, 5 / 2 ) - 96 95Re.A TD .8-=100; .8-n=54.6 14 *

190 3334 3 26.464 s 0.009 5/2 + 96 94It.A T .8--=100 19F --1487.40 0.07 STABLE 1/2 + 96 1S=100. 19Ne 1751.1 0.6 17.296 s 0.005 1/2 + 96 94Ko.A T .8+=100 19Na 12929 12 < 40 ns 5 /2+# 93 93Po.A T p=100 *

• 19C T : average 88Du09=49(4) 95Re.A=44(4) 95Oz02--45.5(4.0) J : from 95Ba28 **

• 19N J : from 95Oz02 ** • 19Na D : most probably prou~n emitter from Sp=-333(12) keV **

20C 37560 200 16 ms 3 0 + 90Mu06 TD .8-=100; .8--n=72 14 * 20N 21770 50 130 ms 7 93 95Re.A TD . 8 - =100; . 8 - n=57.0 25 200 3796.9 1.2 13.51 s 0.05 0 + 93 . 8 - =100 20F --17.40 0.08 11.163 s 0.008 2 + 95 96Ti.1 T .8--=100 20Ne --7041.930 0.002 STABLE 0 + 94 IS=90.48 3 20Na 6845 7 447.9 ms 2.3 2 + 94 89(2102 D fl+=100; ff~-a=25.0 4 20Mg 17571 27 90 ms 6 0 + 94 95Pi03 T fl+=100; fl+p=3 2 *

• 20C T : average 90Mu06=14(+6--5) 95Re.A 16.7(3.5) ** • 20Mg T : average 95Pi03=95(3) 92Go10=82(4) D : .8+p intensity is from 8lAy01 **

21C 45960# 500# < 30 ns 1 /2+# 93Po.A T n ? 21N 25230 90 87 ms 6 1 / 2 - # 90Mu06 TD .8-=100; . 8 - n=80 6 * 210 8062 12 3.42 s 0.10 (1/2, 3/2, 5/2) + 93 , 8 - = 100 21F --47.6 1.8 4.158 s 0.020 5/2 + 94 fl-- =100 21Ne --5731.72 0.04 STABLE 3/2 + 94 IS=0.27 1 21Na --2184.3 0.7 22.49 s 0.04 3/2 + 94 fl+=100 21Mg 10912 16 122 ms 3 (5/2, 3/2) + 93 73Se08 D .8+=100; .8+t,=32.6 10; .8+a<0.5 * 21A1 26120# 300# < 35 as 1/2+# 93Po.A T p ?

• 2IN T : average 90Mu06--95(+15-11) 95Re.A=83.6(6.7) ** • 2IN D : . 8 - n : average 90MufKa=84(9)% 95Re.A=78(7)% ** ,21Mg J : from mirror 211::, tbare is a preference for 5/2 + **

22C 52580# 900# > 200 ns 22N 32080 200 18 ms 5 220 9280 60 2.25 s 0.15 22F 2794 12 4.23 s 0.04 22Ne --8024.34 0.22 STABLE 22Na --5182.1 0.5 2.6019 y 0.0004 22Mg --396.8 1.4 3.857 s 0.009 22A1 18180# 90# 80 ms 40 22Si 32160# 200# 29 ms 2

• 22N T : average 90Mu06=24(+7-6) 95Re.A=I4(5.6) • 22A1 T : symmetriz~d from 70(+50-35)

0 + 93 86Po13 T . 8 - ? 90Mu06 TD f l - = 100 ; . 8 -n=35 5

0 + 93 95Re.A D .8-=100; . 8 - n < 2 2 4 + , ( 3 + ) 94 95Re.A D . 8 - =100; . 8 - n<11

0 + 94 IS=9.25 3 3 + 94 /5+=100

0 + 94 #'+=100 4 + 93 ABBW D .8+=100; .8+2p~2.5; .8+p~0.8 o + 96Bnl TD #+=100;/~+p=32 4

• 22A1 D : .8+p,,~0.8% and #~-2p~2.5% deduced from #~+p+fft-2p~.2.9(+2.1-1.5)% • 22A1 D : in 82Ca16 and from ~+2p/ .8+p~,3.7 (average of 1.9 and 5.5) in 84Ca29 • 22A1 D : ~+2p=0.9(0.5)%. fl+a--0.31(0.09)%, T=59(3) ms and fn '= (3+) in post cut-off date 97B103

2 6 G. Audi et al./Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life . f f Eas Reference Decay modes and intensities (keV) energy(keV) (%)

23N 37740# 710# 230 14620 100 23 F 3330 80

23Ne --5153.64 0.25 23Na --9529.49 0.21 23Mg --5472.7 1.3 23 AI 6767 25 23Si 23770# 200#

*230 T : symmetdzed from 82(-t-45-28)

> 200 ns 1 / 2 - # 85La03 T .0-- ? 90 ms 40 1/2+# 93 90Mu06 T .0--=100; .0--n=31 7

2.23 s 0.14 (3/2, 5/2) + 93 95Re.A T .0--=100; . 0 - n < 1 4 37.24 s 0.12 5/2 + 94 . 0 - = 100

STABLE 3/2 + 94 IS=I00. 11.317 s 0.011 3/2 + 94 .0+=100

470 ms 30 5 /2+# 93 952q08 D .0+=100; .0+p=8 4 > 200 ns 3 /2+# 86La17 T .0+ ?

• 23A1 D : ~+p=3.5(1.9)% from the IAS. Total=3.5×4.8/2.2=7.6% • 23Si T : 42.3(0.4) ms; .0+=100%; .0+p~88%; ~+2p=3.6(0.31% in post cut-off date 97B104

24N 47040# 500#

240 18970 310 7~F 7540 70 24Ne --5948 10 24Na -8417 .60 0.22 24Na"f --7945.39 0.22 472.207 0.009 24Mg -- 13933.38 0.19 24A1 --55 4 24A1 m 371 4 425.8 0.1 24Si 10755 19 24p 32000# 500#

*240 T : symmetrized from 61(+32-19)

3.38 m 0.02 14.9590 h 0.0012 20.20 ms 0.07

STABLE 2.053 s 0.004 131.3 ms 2.5 100 ms 40

• 24F T : average 95Re.A=440(70) 86Du07=340(80) • 24A1 D : f l+p derived from ~-p / .0+a=0.047(2) ; 94Ba54 uses fl+a=O.026%, no mason given • 24Si D : symmeWized from .0+p=7(+6-4)% T : post cut-off date 97Cz02=140(8) and .0+p=37.6(2.5)%

< 52 ns 93Po.A T n ?

70 ms 30 0 + 93 90Mu06 T .0 -=100; .0 -n=58 12 * 400 ms 50 (1 ,2 ,31 + 93 95Re.A TD .0-=100; . 0 - n < 5 . 9 *

0 + 93 . 0 - =100 4 + 94 , 8 - =100 1 + 94 I T ~ 100; .0---0.05 0 + 94 1S=78.99 3 4 + 93 94Ba54 D .0+=100; .0+a=0.035 6; .0+p--0.0016 3 * 1 ~- 93 1T=82 3; .0+=18 3; .0+a=0.028 6 0 + 93 8lAy01 D .0+=100; .0+p=8 5 *

1+# p ?; .0+ ?

250 27140# 370# 25F 11270 80 25 Ne -- 2060 40 25Na --9357.5 1.2 25Mg --13192.73 0.19 25A1 --8915.7 0.7 25Si 3825 10 25p 18870# 200#

< 50 ns 3 /2+# 93Po.A T n ? 87 ms 16 5 /2+# 95Re.A TD .0-=100; . 0 -n=24 5

602 ms 8 (1/2, 3/2) + 93 . 0 - =100 59.1 s 0.6 5/2 + 93 . 0 - = 100

STABLE 5/2 + 94 IS=I0.00 1 7.183 s 0.012 5/2 + 94 .0+=100 220 ms 3 5/2 + 93 93Ro06 D /3+=100; .0+p=36.81 5

< 30 ns 1/2+# 93Po.A T p ?

260 35160# 430# 26F 18290 120 26Ne 4~1 511 26Na --6902 14 26Mg -- 16214.48 0.19 26A1 -- 12210.34 0,20 26A1" --11982.03 0.20 228.305 0.013 26Si --7145 3 26p 10970# 200# 26S 25970# 300#

< 40 ns 0 + 93Po.A T n ?; .0----0 190 ms 110 95Re.A TD .0-=100; . 0 - n < 3 2 197 ms 1 0 + 93 92Te03 TD .0-=100; .0-n--0.13 3

1.077 s 0.005 3 + 93 92Te03 T . 0 - =100 STABLE 0 + 94 IS=l 1.01 2

740 ky 30 5 + 94 fl+=100 6.3452 s 0.0019 0 + 94 .0+=100

2.234 s 0.013 0 + 94 .0+=100 30 ms 25 (3 + ) 93 ABBW D .0+=100; .0+2p~1; .0+p~0.9 10# ms 0 ~ 2p ?

*260 D : in 96Fa01 experiment, several hundred of 260 events expected, none observed *26Na T : average 92Te03=1.074(0.006) 73A113=1.087(0.0121 .26p T : symmetrized from 20(+35-15) . 26p D : .0+ p~-,0.9% and .0+2p~1% deduced from .0+ p+.0+2p,,~,l.9% in ENSDF .26p D : and .0+2p/f l+p,~l .2 (average of 0.9 and 1.4) in 84Ca29

27 F 25050 420 27 Ne 7090 90 27Na --55811 40 27Mg -- 14586.50 0.20 27A1 --17196.83 0.13 27Si --12384.43 0.16 27p --750 40

27S 17510# 20(1#

> 200 ns 5 /2+# 93 85La03 T . 0 - ? 32 ms 2 3 /2+# 93 92Te03 TD .0-=100; .0 -n=2.0 5

301 ms 6 5 /2 + 93 84Gu19 D .0-=100; p - n = 0 . 1 3 4 9.458 m 0.012 1/2 + 93 .0--=100

STABLE 5/2 + 94 IS=100. 4.16 S 0.02 5/2 + 94 .0+=100 260 ms 80 1/2 + 93 96Og01 D ff~=100; fl+p---0.07 21 ms 4 (5/2 + ) 93 91B032 TJD ,8+=100; .0+2p=2.0 10; .0+p=?

G. Audi et al./Nuclear Physics A 624 (1997) 1-124 2 7


28F 33230# 510# 28 Ne 11280 110 28Na -- 10311 80 28Mg -- 151118.8 2.0 28A1 --16850.55 0.14 28Si --21492.793 0.002 28p --7161 4 28S 4070 160 28C1 26560# 500#

*28Ne T : average 95Re.A=8.2(2.5) 92Te03=17(4) . 28p D : . . . ; /3+a--0.00086 25

< 40 ns 11 m s 4

30.5 ms 0.4 20.91 h 0.03

2.2414 m 0.0012 STABLE

270.3 ms 0.5 125 ms 10

93Po.A T n ? 0 + 93 92Te03 TD / 3 - =100; / 3 - n=22 3 14 93 /3-=100; /3-n--0.58 12 0 + 93 / 3 - =100 3 + 94 /3 -=100 0 + 94 IS=92.23 1 3 ¢ 93 79Ho27 D /3+=100; /3+p=0.0013 4; . . . 0 + 93 89Po10 D /3+=100; /3+p=20.7 19 t+# p ?

29F 40300# 580# 29 Ne 18020 300 29 Na 2620 90 29Mg -- 10661 29 29At -- 18215.5 1.2 29Si --21895.025 0.028 29p -- 16951.9 0.7 29S --31611 50 29C1 13140# 200#

> 200 ns 5 /2+# 89Gu03 T / 3 - ? 200 ms 100 3 /2+# 92Te03 TD /3 -=100 44.9 ms 1.2 3/2 I+#) 93 90En08 J / 3 - = 100 ; / 3 - n= 25 .9 23 1.30 s 0.12 3/2 + 94 /3 -=100 6.56 m 0.06 5/2 + 93 / 3 - =100

STABLE 1/2 ~- 96 IS=4.67 21 4.142 s 0.015 1/2 + 96 /3+=100

187 ms 4 5 /2" 93 79Vi01 D /3+=100; /3+p=46.4 10 < 20 ns 3 /2+# 93Po.A T p ?

*29Na D : /3--n : average 95Re.A=27.1(I.6)% 84La03=21.5(3.0)%

30Ne 22240 8211 30 Na 8590 90

3°Mg --8880 70 3°AI -- 15872 14 3°Si --24432.88 0.04 ~ P --20200.6 0.4 3°S -- 14063 3 3°CI 4440# 200# 30 Ar 20080# 300#

* ~ N a D : . . . ; /3--a=5.5e-5 20

> 200 ns 0 + 85La03 T /3 - ? 48 ms 2 2 + 93 ,8-=100; /3 -n=30 4; /3-2n=1.17 16; . . . *

335 ms 17 0 + 93 84La03 D /3--=100; /3 -n<0 .06 3.60 s 0.06 3 ÷ 93 /3 - =100

STABLE 0 + 94 IS=3.10 1 2.498 m 0.1104 1 + 94 /3+=100 1.178 s 0.005 0 + 94 /3+=100 < 30 ns 3+# 93Po.A T p ? < 20 ns 0 + 93 93Po.A T p ?

31Ne 30840# 900# 31Na 12660 160 31Mg --3220 80 31AI -- 14954 20 31Si --22948.96 0.07 31p --24440.99 0.18 31S -19044 .9 1.5 31C1 --706t) 50 31Ar 1 1 3 1 1 0 # 210#

*31Na D : . . . ; /3-- 3n<0.05 .31AI J : from systematics there is a preference for 5/2 + *31Ar D : . . . ; /3+3p=2.1 10 D : all from 92Ba01. /3+a and /3+po, not found

> 260 ns 7 / 2 - # 96Sa34 T / 3 - ? ; / 3 - n ? 17.0 ms 0.4 (3/2 + ) 93 93K102 J /3-=100; /3-n=37 5; /3-2n--0.9 2; . . . * 230 ms 20 3/2 + 96 90En08 D /3-=100; /3-n=1.7 3 644 ms 25 (5/2, 3/2) + 93 95Re.A D /3-=100; /3--n<1.6 •

157.3 m 0.3 3/2 + 93 / 3 - =100 STABLE 1/2 + 94 IS=100.

2.572 s 0.013 1/2 + 93 /3+=100 150 ms 25 3/2 + 93 85Ay02 D /3+=100; /3+p=0.7 15 ms 3 (5/2 + , 3/2 + ) 87Bo36 TJ /3+=100; /3+p=55 7;/3+2p=2.48 15; . . . *

D : all from 84Gu19 **

32Ne 37180# 880# 32Na 18300 480 32Mg --800 100 32A1 --11060 90 32Si --24080.9 2.2 32p --24305.32 0.19 32S --26015.98 0.11 32C1 -- 13331 7 32Ar --2180 5(I 32K 20420# 500#

*32Mg T : average 95Re.A=85(13) 84La03=120(201

> 200 ns 0 + 90Gu02 T /3-- ?; /3-- n ? 13.2 ms 0.4 ( 3 - - , 4 - ) 93 93K102 J /3--=100; /3--n=24 7; f l--2n=8 2 95 ms 16 0 + 93 95Re.A T /3-=100; /3-n=2.4 5

31.7 ms 0.8 l + 96 95Re.A TD /3-=100; /3-n--0.7 5 132 y 13 0 + 93 93Ch10 T /3 -=100

14.262 d 0.014 1 + 94 /3 -=100 STABLE 0 + 94 1S--95.02 9

298 ms 1 1 + 93 79Ho27 D /3+=100; /3+ot=0.054 8;/3+p--0.026 5 98 ms 2 0 + 93 /3+=100; /3+p=43 3

1+# p ?

2 8 G. Audi et al . /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life J~ Ens Reference Decay modes and intensities (keV) energy(keV) (%)

33Ne 7 / 2 - # n ? * 33Na 25510 1490 8.2 ms 0.4 3 /2+# 93 ,8 -=100; ,8 -n=52 20; ,8 -2n=12 5 33Mg 5200 150 90 ms 20 7 / 2 - # 96 ,8-=100; ,8 -n=17 5 33Al --8500 70 40.5 ms 2.8 5 /2+# 93 95Re.A TD ,8--=100; ,8-n=8.5 7

33Si --20492 16 6.18 s 0.18 3 /2+# 93 , 8 - = 100 33p --26337.7 1.1 25.34 d 0.12 1/2 + 94 , 8 - = 100 33S --26586.24 0.11 STABLE 3/2 + 94 IS=0.75 1 33CI --21003.5 0.5 2.511 s 0.003 3/2 + 93 ,8+=100 33At --9380 30 173.0 ms 2.0 1/2 + 93 /3+=100; ,8+p=38.7 10 33K 6760# 2(10# < 25 ns 3 /2+# 93Po.A T p ?

*33Ne I : clue for particle unstability obtained in post cut-off date 97Sa14

34Na 32510# 1050# ~4 Mg 8450 260 34 AI -- 2860 90

MSi --19957 14 34p --24558 5 34S --29931.85 0.10 34CI --24440.57 0.12 34C1"~ --24294.21 0.12 146.36 0.03 34At -- 18378 3 34 K -- 1480# 300#

MCa 13150# 300#

5.5 ms 1.0 1 + 93 ABBW D , 8 - MOO; f l - 2n~50; , 8 - n,~,15

20 ms 10 0 + 93 f l - = 100 ; , 8 - u ? 42 ms 6 4 - # 93 95Re.A TD ,8--=100; /3-n=12.5 25

2.77 s 0.20 0 ~ 93 fl-- =100 12.43 s 0.08 1 I- 93 fl--=100

STABLE 0 + 94 IS--~-.21 8 1.5264 s 0.0014 0 + 94 ,8+=100 32.00 m 0.04 3 ~ 94 ,8+ =55.4 6; IT=.~.6 6 845 ms 3 0 + 94 ,8+ = 100

< 4(I ns 1+# 93Po.A T p ? < 35 ns 0 + 93Po.A T p ?

*34Na D : , 8 - u,~, 15%, f l - 2n~50% estimated from P,, = 13- n + 2 X f l - 2n=115(2(I1% in 84La03 *34Na D : assuming ,8-n/,8--2n--0.3 from trends in the 30Na-33Na series: 26 41 3 4

.34A1 D : , 8 - u=27(5)% in ENSDF, not used

35Na 41150# 1550# 35Mg 16290# 440# 35AI --60 140 35 Si -- 1436(I 4(1 35p --24857.6 1.9 35S --28846.37 0.09 35C1 --29013.51 0.04 35Ar --23(148.2 0.8 35K --11167 20 35Ca 4440# 70#

1.5 ms 0.5 3 /2+# 93 ,8-=100; 0 - n = ? 70 ms 40 7 / 2 - # 95Re.A TD ,8-=100; f l - n = 5 2 46 30 ms 4 5 /2+# 93 95Re.A TD ,8--=100; f l - n = 2 6 4

780 ms 120 7 / 2 - # 93 95Re.A D f l -=100 ; f l - n < 5 . 2 6 47.3 s 0.7 1/2 ~ 93 , 8 - = 100 87.51 d 0.12 3/2 + 94 , 8 - = 100

STABLE 3/2 + 94 IS=75.77 5

1.775 s 0.004 3/2 + 94 ,8+ =100 190 ms 30 3/2 + 94 ,8+=100; ,8+p=0.37 15 50 ms 30 1/2+# 94 ,~' =100; ,8+2p=?

• 35Ca D : ,8'~p=20%# to the IAS, estimated by 85Ay01

36Mg 20910# 900# 36A1 5920 270 36Si -- 12400 100 36p --20251 13 36S --30663.96 0.23 36CI --29521.89 0.08 36At -- ~12~1.44 0.25 36K -- 17425 8 36Ca --6440 40 36 Sc 139(10# 500#

• 36K D : . . . ; ,8+a---0.0034 13

> 200 ns 0 + 89Gu03 T , 8 - ? 90 ms 40 95Re.A TD f l - = 100 ; , 8 - n< 31

450 ms 60 0 + 93 95Re.A D ,8-=100; ,8 -n=12 5 5.6 s 0.3 93 , 8 - =100

STABLE 0 + 93 IS=0.02 1 301 ky 2 2 + 94 ,8----98.1 1; ,8+=1.9 1

STABLE 0 + 94 IS=0.3365 30; 2,8 + ? _'342 ms 2 2 + 93 /8+=100; fl+p=0.048 14; . . . 102 ms 2 0 ~ 93 95Tr02 TD ,8+=100; ,84-p=56.8 13

p ?

37Mg 29100# 900# 37A1 9600 540 37Si --6520 130 37p -- 18990 40 37S --26896.22 (I.25 37CI --31761.52 0.05 3TAr --30948.11 0.3 37K --24799.24 0.27 37Ca -- 13161 22 37 Sc 284(1# 300#

> 260 as 7 /2 - -# 96Sa34 T fl-- ?; f l - -n ? > 1 ,us 3 /2+# 91Or01 T fl-- ? 90 ms 60 7 /2 - -# 95Re.A TD f l -=100 ; fl--n=17 13

2.31 s 0.13 1/2+# 93 ,8-- =100 5.05 m 0.02 7/2-- 94 fl-- =100

STABLE 3/2 "I- 94 IS=24.23 5 35.04 d 0.04 3/2 + 94 e=100 1.226 s 0.007 3/2 + 94 ,8+=100 181.1 ms 1.0 3/2 + 93 95Tr03 TD /3+=100; ,8+p=74.5 7

7 / 2 - # p ?


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

38Mg 0 + , 8 - ?

38A1 15740# 560# 89Gu03 T , 8 - ? 38Si --3740 270 0 + 91Zh24 T , 8 - ?; , 8 - n ? 38p --14470 140 93 95Re.A D ,8-=100; , 8 - n= 12 5 38S --26861 7 0 + 94 , 8 - =100 38C1 --29797.98 0.11 2 - 93 , 8 - = 100 38C1m --29126.62 0.11 671.361 0.008 5 - 93 11"--100 38Ar --34714.8 0.5 0 + 94 IS=0.0632 5 38K --28801.7 0.7 3 + 94 ,8+=100 38Kin --28671.3 0.8 130.4 0.3 0 + 94 ,8+=100 38Ca --22059 5 0 + 93 fl+=100 38Sc --4940# 300# 2 - # 94B110 T p ? 38Scm --4240# 320# 700# 100# 5 - # p ? 38"I~ 9100# 250# < 120 ns 0 + 96B121 T 2p ?

*38Mg I : 18 events reported in post cut-off date 97Sa14. Then T>260 ns

1# ms > 200 as

> 1 ,us 640 ms 140

t70.3 m 0.7 37.24 m 0.05 715 ms 3

STABLE 7.636 m 0.018 923.9 ms 0.6 440 ms 8

< 300 n s

39A1 20400# 600# 39Si 2140# 400# 39p -- 12650 150 39S --23160 50 39CI --29800.7 1.7 39At --33242 5 39K --33806.84 0.28 39Ca --27276.3 1.8 39Sc --14168 24 39Ti 1230# 100#

• 39Sc D : most probably proton emitter from Sp=~602(24) keV • 39Ti D : f l+2p decay observed by 92Mo15 • 39Ti T : symmetrized from 26(+8-7)

> 200 ns 3 /2+# 89Gu03 T , 8 - ? > 1 /~s 7 / 2 - # 90Au.A T /3 - ?

190 ms 50 1/2+# 93 95Re.A TD ,8--=100; ,8--n=26 8 :'~.5 s 0.5 ( 3 / 2 , 5 / 2 , 7 / 2 ) - 93 ,8-=100 55.6 m 0.2 3/2 + 93 , 8 - =100 269 y 3 7 / 2 - 94 , 8 - =100

STABLE 3/2 + 94 IS=93.2581 44 859.6 ms 1.4 3/2 + 94 ,8+=100 < 300 ns 7 / 2 - # 93 94B110 T p=100

26 ms 8 3/2 + # 92 90De43 TD ,8+=100; ,8+p=85 15; /~-2p=? *

40AI > 260 ns

40Si 5400# 500# > 200 ns 0 + 40p --8340 200 290 ms 80 'IOs --22850 230 8.8 s 2.2 0 +

40C1 --27560 30 1.35 m 0.02 2 - 4°At --35039.890 0.004 STABLE 0 + 40K --33535.02 0.27 1.277 Gy 0.008 4 - 40Ca --_34846.11 0.29 STABLE 0 + 40Sc --20526 4 182.3 ms 0.7 4-- 40Ti --8850 160 60 ms 15 0 + 40V 10330# 500# 2 - #

*40AI I : tentative. Only one event has been observed. 34 events in post cut-off date 97Sa14 .40p T : symmetrized from 260(+100410) *40K D : . . . ; B+=10.72 13 .40Sc D : . . . ; f l+a=0.017 5 .40"11 T : symmetrized from 56(-I-18-12); post cut-off date 97Li.1=55(2) ms *40Ti T : post cut-off date 97Po.A=51.8(0.4) ms and ,8+p=100.5(2.7)%. In the work *40Ti T : of 90De43, not all the fl+ p activity was observed

96Sa34 T , 8 - ?; , 8 - n ? * 89Gu03 T , 8 - ?

93 89Le16 T ,8-=100; , 8 - n= 30 10 * 93 , 8 - = 100 93 , 8 - =100 93 IS--99.6003 30 94 IS--0.0117 1; ,8---89.28 13; . . . * 94 IS--96.941 18; 2/~- ? 93 fl+=100; fl+p--0.44 7; . . . * 93 90De43 TD ,8+=100; ,8+p---43 6 *

p ?

41AI 1# ms 3/2 + # 4 l s i 11830# 600# > 200 ns 7 /2 - -# 41p --4840 470 120 ms 20 1/2+# 93 41S --18600 210 2.6 s 1.4 7 /2 - -# 41C1 --27340 60 38.4 s 0.8 (1/2, 3/2) + 93 41At --33067.3 0.7 109.34 m 0.12 7/2-- 94 41 K --35558.87 0.26 STABLE 3/2 + 94 41Ca --35137.5 0.4 103 ky 4 7/2-- 94 41Sc --28642.2 0.3 596.3 ms 1.7 7 / 2 - 94 41Ti --15710# 40# 80 ms 2 3/2 + 93 41V -- 240# 250# 7/2 - #

.41AI 1 : 4 events mpotmd in post cut-off date 97Sa14. Then T>260 ns

p - ?

89Gu03 T , 8 - ? ,8-=100; , 8 - n=30 10

95Re.A TD , 8 - = 100; , 8 - n ? ,8--=100 ,8--=100 IS=6.7302 44 ~=100 ~+ =I00 #'+ =100; ~+ p~,~ 100 p ?


Nuclide Mass excess Excitation Half-life ftr Ens Reference Decay modes and intensities (keV) energy(keV) (%)

42Si 15000# 700# > 200 ns 0 + 90Le03 T 8 - ? 42p 8(1# 500# 120 ms 30 93 89Le16 T /3-=100; /3 -n=50 20 * 42S --17240 330 560 ms 60 0 + 95So03 TD /3-=100; / 3 - n < 4

42C1 --24990 110 6.8 s 0.3 93 /3 -=100 42 Ar -- _M420 40 32.9 y 1.1 0 + 93 / 3 - = 100 42K --35021.3 0.3 12.360 h 0.003 2-- 94 /3--=100 42Ca --38546.8 0.4 STABLE 0 + 94 IS=0.647 9 42Sc --32120.9 0.4 681.3 ms 0.7 0 + 94 /3+=100 42Scm --31504.6 0.4 616.28 0.06 61.7 s 0.4 7 +, (5 +, 6 + ) 94 /3+=100 42Ti --25121 5 199 ms 6 0 + 93 /3+=100 42V --8170# 200# < 55 ns 2 - # 92Bo37 T p ? 42Cr 5990# 300# > 350 ns 0 + 96B121 T /3+ ?; 2p ? *

.42p T : symmetrized from 110(+40-20) ** • 42Cr T : 20 ms expected from systematics of/3+ half-lives **

43Si 15# ms 3 / 2 - # / 3 - ? 43p 3080# 500# 33 ms 3 l / 2 + # 95So03 TD /3-=100; /3-n=100 43S --12480 840 240 ms 70 7 / 2 - # 93 89Le16 T /3-=100; /3-n-M0 10 *

43CI --2403,0 160 3.3 s 0.2 3 /2+# 93 /3-=100; / 3 - n ? 43Ar --31980 70 5.37 m 0,06 (5/2, 3/2) ~-#) 93 f l - = 1 0 0 * 43 K -- 36593 9 22.3 h 0.1 3/2 + 93 / 3 - = 100 43Ca --384118.4 0.5 STABLE 7/2-- 94 IS=0.135 6

43Sc --36187.6 1.9 3.891 h 0.012 7 / 2 - 94 /3+=100 43"15 --29320 7 509 ms 5 7/2-- 93 /3+=100 43V --18020# 230# > 80/) ms 7 /2 - -# 92Bo37 T /3+ ? * 43Cr --2140# 90# 22 ms 4 (3/2 + ) 92Bo37 TJD /3+=100; /3+p=23 6; /3+2p=6 5; /3+a ? *

• 43S T : symmetrized from 220(+80-50) ** ,43Ar J : from systematics, there is a preference for 5 / 2 - ** • 43V T : te be confirmed. 80 ms expected from systematics of/3+ half-life ** • 43Cr T : symmetrized from 21(+4-3) ** • 43Cr D : from /3+p(1/2-1 )=1714)% and/3+p+/3+2p(IAS)=12(4)%, as analyzed with 96Po.A **

44p 9200# 700# > 200 ns 89Gu03 T / 3 - ? 44S --10880# 501/# 123 ms 10 0 + 93 93So06 TD /3-=1011; /3-n=18 3 44C1 --19990 220 434 ms 60 95So03 TD /3-=100; / 3 - n < 8 44Ar --32262 20 11.87 m 0.05 0 + 93 /3--=100 44K --35810 40 22.13 m 0.19 2-- 93 /3--=100 44Ca --41469.1 0.9 STABLE 0 + 94 IS=2.086 12 44Sc --37815,8 1.8 3.927 h 0.008 2 ¢ 94 /3+=100 44Sc" --37544.7 1.8 271.13 0.11 58.6 h 0.1 6 ÷ 94 IT=98.80 7; /3+=1.20 7 44Ti --37548.3 0.8 64.8 y 2.2 0 + 94 96No.A T e=100 44V --23850# 80# 1l l ms 7 (2 +) 93 97Ha04 TJ /3+=100; /3+a=? 44V" --23550# 130# 300# 100# 15(I ms 3 (6 + ) 97Ha04 TJD /3+=100 44Cr -- 135411# 130# 54 ms 4 0 + 96Fa09 D /3+=100; /3-I p=7 3 4"4Mn 641111# 5011# < 105 ns 2 - # 92Bo37 T p ?

• 44Ti T : average 96No.A=62(2) 90A111=66,6(1.6); post cut-off date 97No.1=63(3) supersedes 96No.A • 44"15 T : beth strongly disagree with earlier results, see discussion in 96No.A • 44Ti T : T-~9(3) yea,~ is, in ENSDF, the average of 3 earlier measurements

• 44Cr T : 53(+4-3) from 92Bo37

45p 14100# 800# > 21/11 ns 1/2+# 93 90Le03 T f l - ? 45S --4830# 601/# 82 ms 13 3 / 2 - # 95So03 TD /3-=100; /3--n=54 45CI --18910 650 400 ms 40 3 /2+# 95 /3 =100; /3 -n=24 4 45AT --29720 60 21.48 s 0.15 (1/2, 3/2, 5 /2) - - 95 /3--=100 45K --36608 10 17.3 m 0.6 3/2 + 95 /3 -=100 45Ca --40812.5 0.9 162.67 d 0.25 7/2 95 94Lo04 T /3-=1011 45Sc --411169.3 1.1 STABLE 7/2-- 95 IS=I00. 45Sc m --411156.9 1.1 12.40 0.05 318 ms 7 3/2 + 95 IT= 100

. . . A-group is cominued on next page . . .


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensifies (keV) energy(keV ) (%)

. . . A-group continued . . . 45Ti --39006.9 1.2 184.8 m 0.5 7 / 2 - 95 45V --31874 17 547 ms 6 7 / 2 - 95 45Cr --19410# 100# * 50 ms 6 7 / 2 - # 95 45Cr0~ --19310# 120# 100# 70# * 1# ms 3 /2+# 45Mn --5110# 300# < 70 ns 7 / 2 - # 45Fe 13560# 400# > 350 ns 3 /2+#

• 45Ar J : 7 /2 - - is expected from theory and from systematics. See ENSDF. • 45Fe T : but not observed by 92Bo37, with <250 ns; T=I0 ms expected from • 45Fe T : systematics of ,8+ half-lives

92Bo37 T 96B121 T

,8+=100 ff~ =100 ,8+=100; ,8+p>27 IT ?; ,8+ ? p ?

p ?; 2p ?

46p 22200# 900# > 200 ns 46S --400# 700# > 200 ns 46C1 - 14790# 500# 220 ms 40 46Ar --29720 40 8.4 s 0.6 46K --35419 16 105 s 10 46Ca --43134.9 2.4 STABLE 46Sc --41758.6 l . l 83.79 d 0.04 46 Sc"~ --41616.1 1.1 142.528 0.007 18.75 s 0.04 46"1"i --44125.3 l . l STABLE 46V --37073.9 1.5 422.37 ms 0.20 46vm --36272.4 1.5 801.52 0.10 1.02 ms 0.07 46Cr --29471 20 260 ms 60 46Mn --12370# 110# 42 ms 7 46Mn" --12220# 120# 150# 50# 1# ms 46Fe 760# 350# 28 ms 15

*46Mn T : symmetrized from 41(+7-6) *46Fe T : symmetdzed from 20(+20-8)

90Le03 T , 8 - ? 0 + 89Gu03 T , 8 - ?

93So06 TD , 8 - =100; , 8 - n=60 9

0 + 93 , 8 - =100 2 ( - ) 93 82To02 J , 8 - = 1 0 0

0 + 93 IS=0.004 3; 2 ,8 - ? 4 + 93 , 8 - = 100 1 - 93 IT= 100

0 + 93 IS=8.25 3 0 + 93 fl+ =100 3 + 93 IT=I00 0 + 93 /5'+=100

(4 + ) 93 92Bo37 TDJ `8+=100; fl+p=22 2; ~ - 2 p ?; ,8+or ? *

1 - # ,8+ ? 0 + 93 92Bo37 TD ,8+=100;, ,8+p=? *

47S 7100# 800# 47C1 --11230# 600# 47At --25910 100 47 K -- 35697 8 47Ca --42339.7 2.3 47Sc --44331.6 2.1 47Ti --44931.7 1.0 47V --42003.9 1.1 47Cr --34552 14 47Mn --22260# 160# 47Fe --6620# 260# 47C0

*47Ar D : from 95So03 *47Fe T : symmetfized from 27(+32-10)

> 200 ns 3 / 2 - # 95 89Gu03 T `8- ? > 200 ns 3 /2+# 95 89Gu03 T /3-=100; `8--n<3

580 ms 120 3 / 2 - # 95 89Ba.B T `8- =100; , 8 - -n< l 17.50 s 0.24 1/2 + 95 , 8 - =100 4.536 d 0.003 7 / 2 - 95 fl-- =100

3.3492 d 0.0006 7 / 2 - 95 fl-- =100 STABLE 5/2-- 95 IS=7.44 2

32.6 m 0.3 3 / 2 - 95 ~+ =100 500 ms 15 3 / 2 - 95 fl+ =100 100 ms 50 5 /2 - -# 95 96Fa09 TD ,8+=100; fl+p=3.4 9 41 ms 22 7 /2 - -# 92Bo37 TD fl+=100; fl+p=?

7 / 2 - # p ?

48S 12100# 900#

48CI - 4 8 0 0 # 70O# 4BAr --23220# 300# 48K --32124 24 48Ca --44215 4 48 Sc -- 44493 5

48Ti --48487.0 1.0 48V --44474.7 2.6 48Cr --42815 7 48Mn --29000# 70# 48Fe --18110# 100# 48Co 1640# 400#

> 200 ns 0 + 90Le03 T , 8 - ?

> 200 ns 89Gu03 T , 8 - ? 500# ms 0 + , 8 - ? 6.8 s 0.2 ( 2 - - ) 95 , 8 - =100; f l - -n=l .14 15 51 Ey 23 0 + 95 96Ba80 TD 1S--0.187 4; 2`8-=?; , 8 - ?

43.67 h 0.09 6 + 95 , 8 - =100 STABLE 0 + 95 IS=73.72 3 15.9735 d 0.0025 4 + 95 `8+=100 21.56 h 0.03 0 + 95 ,8+=100 158.1 ms 2.2 4 + 95 87Se07 D ,8+=100; ,8+p=0.28 4; f l + a = 6 e ~

44 ms 7 0 + 95 96Fa09 TD fl+=100; ,8+p=3.6 11 6+# p ?

• 48Ca T : symmetdzed from 43(+24-11 statistics + 14 systematics) • 48Ca T : also T>36Ey from 70Ba61. Single f l - decay: T>6Ey (95% CL). from 85A117 • 48Mn D : one `8+t~ event was observed, versus 437 fl+p, in fig.4 of 87Se07



49S 20500# 1000# < 200 ns 3 / 2 - # 90Le03 T n ? 49C1 --100# 800# > 170 ns 3 /2+# 95 /3-- ? 49Ar --16600# 500# > 170 ns 3 / 2 - # 95 /3-- ? 49K --30320 70 1.26 s 0.05 (3/2 + ) 95 /3-=100; /3 -n=86 9 49Ca - 4 1 2 9 0 4 8.718 m 0.006 3 / 2 - 95 /3-=100 49Sc -46552 4 57.2 m 0.2 7 / 2 - 95 f l - =100 49Ti --48558.0 1.0 STABLE 7/2-- 95 IS=5.41 2 49V --47956.2 1.3 3~1 d 15 7 / 2 - 95 e=100

49Cr --45325.4 2.6 42.3 m 0.1 5 / 2 - 95 /3+=100 49Mn --37611 24 382 ms 7 5 / 2 - 95 /3+=100 49Fe --24580# 160# 70 ms 3 ( 7 / 2 - - ) 95 96Fa09 TJD /3+=100; /3+p=52 10 49Co --9580# 260# < 35 ns 7 / 2 - # 94B110 T p 7; /3+ ? 49Ni > 350 ns 7 / 2 - # 96B121 T p ?; /3+ ?

• 49S I : statistics precludes any conclusion, say authors

5°C1 7200# 900# 5°At -- 13100# 700# 5°K --25350 280 50Ca --39571 9 50Sc --44538 16 50Sc m --44281 16 256.895 0.010 50"15 --51425.8 1.0 50V --49217.5 1.3

~ C r --50254.5 1.3 50Mn --42621.5 1.4 50Mnm --42393 7 229 7 5O Fe -- 34470 60 50Co -- 17200# 170# 50Ni --3790# 260#

*50V T : symmetrized from 140(+40-30)

20# ms > 170 ns 0 + 95

472 ms 4 ( 0 - - , 1, 2 - ) 95 13.9 s 0.6 0 + 95

102.5 s 0.5 5 + 95 350 ms 40 2 +, 3 + 95

STABLE 0 + 95 150 Py 40 6 + 95

STABLE >lSOPy 0 + 95 283.9 ms 0.5 0 + 95 1.75 m 0.03 5 + 95 150 ms 30 0 + 95 44 ms 4

> 300 ns

f l - - ? / 3 - - ? /3-- =100; /3-- n=29 3 /3--=100 /3--=100 1T>97.5; f l - <2.5 IS=5.18 2 1S=0.250 2;/3+=83 11; f l - = 1 7 11 *

1S=4.345 13; 2fl + ? /3+=100 fl+=100 /3+=100; O+pm0

(6 + ) 95 96Fa09 TJD fl+=100; fl+p=54 12

0 + 94B110 T fl+ ?

51CI 1260(1# 1000# 51Ar -- 6.'300# 700# 5( K --22000# 500# 51Ca --35890 911 51Sc --43219 20 51Ti --49726.9 1.3 5IV --52197.5 1.3 51Cr --51444.8 1.3 51Mn --48237.0 1.3 51Fe --40217 15 51 Co -- 27270# 150# 51Ni --11440# 260#

> 200 ns 3 /2+# 90Le03 T , 8 - ? > 200 ns 3 / 2 - # 91 89Gu03 T / 3 - ?

365 ms 5 3/2 + # 92 fl-- =100; / 3 - n=47 5 10.0 s 0.8 3 / 2 - # 91 /3 - =100; / 3 - n ? 12.4 s 0.1 (7 /2 ) - - 91 /3 - =100 5.76 m 0.01 3 / 2 - 91 /3-- =100

STABLE 7/2-- 91 IS=99.750 2 27.702 d 0.004 7 / 2 - 91 ~=100 46.2 m 0.1 5 / 2 - 91 /3+=100 305 ms 5 ( 5 / 2 - ) 91 /3+=100

> 200 ns 7 /2 - -# 87Po04 T ill- ? > 200 ns 7 /2 - -# 87Po04 T B + ?

52At --1710# 900# 52K -- 16200# 700# 52Ca --32510 470 52Sc --40380 230 52q~ --49464 7 52V --51437.4 1.3 52Cr --55412.8 1.4 52Mn --50701.1 2.4 52Mnm --50323.4 2.4 377.749 0.005 52Fe --48329 10 52Fe nl --41510 130 6820 130 52Co --33920# 71)# 52Co m --3355(1# 1211# 370# 100# 52Ni --226511# 811# 52Cu -- 26~t# 260#

10# ms 105 ms 5 4.6 s 0.3 8.2 s 0.2 1.7 m 0.1

3.743 m 0.005 STABLE

5.591 d 0.003 21.1 m 0.2

8.275 h 0.008 45.9 s 0.6 I 15 ms 23 104 ms 11 38 ms 5

0 + f l - ? 2 - # 94 ABBW D f l - = 100 ; f l - n ~ 6 4 ; / 3 - 2 n ~ 2 1 * 0 + 94 83La23 D f l - = 100 ; / 3 - n < 2 3 + 94 f l - =100 0 + 94 fl--=lO0 3 + 94 f l - =100 0 + 94 IS=83.789 18 6 + 94 fl+ =1130 24 94 fl÷ =98.25 5; IT=1.75 5 0 + 94 fl+ =100

( 12 + ) 94 ,/3+=100 (6 + ) 97Ha04 TJD 13 +=100 2+# 97Ha04 'I'D /3+=?; IT ? 0 + 94Fa06 TD /3+=100; /3+p>17

34# p ?

• 52K D : /3- -n~64%. f l - -2n~21% estimated from P, = / 3 - n + 2 × f l -2n=107(20)% in 83La23 • 52K D : and assuming f l - n / f l - 2n=3 as in 32Na • 52CC" I : Tentative: no specific evidence for 52Com, say authors in 97Ha04

~tg(

G. Audi et al . /Nuclear Physics A 624 (1997) 1-124 3 3


53Ar 5800# 1000# 3# ms 5 / 2 - # ' 8 - ?; ' 8 - n ? 53K --12000# 700# 30 ms 5 3 /2+# 90 ABBW D '8 -=100; '8 - -n~67; ' 8 - 2 n ~ 1 7 * 53Ca --27900# 500# 90 ms 15 3 / 2 - # 90 '8 -=100; ' 8 - n > 3 0 * 53 Sc --37970# 300# 900 ms 900 7 / 2 - # 95So.A TD f l - =100; ' 8 - n ? 53Ti --46820 100 32.7 s 0.9 ( 3 / 2 ) - 90 ' 8 - = 1 0 0 53V --51845 3 1.61 m 0.04 7 / 2 - 90 ' 8 - = 1 0 0 53Cr --55280.6 1.4 STABLE 3/2-- 90 1S=9.501 17 53Mn --54683.6 1.4 3.74 My 0.04 7 / 2 - 96 ~=100 53Fe --50941.3 2.1 8.51 m 0.02 7 / 2 - 90 '8+=100 53Fe m - 4 7 9 0 0 . 9 2.1 3040.4 0.3 2.526 m 0.024 1 9 / 2 - 90 96Ge.A T IT=I00 53C0 --42639 18 240 ms 20 7 / 2 - # 90 '8+=100 53Co'~J --39445 24 3194 30 p 247 ms 12 ( 1 9 / 2 - ) 90 '8+~98.5; p ~ l . 5 53Ni --29380# 160# 45 ms 15 7 / 2 - # 90 76Vi02 D '8+=100; ' 8+p~45 53Cu --13460# 260# < 300 ns 3 / 2 - # 93BI.A T p ?; '8+ ?

• 53K D : ' 8 - n ~ 6 7 % . ' 8 - 2 n ~ 1 7 % estimated from Pn = ' 8 - n + 2 X '8-2n=100(30)% in 83[a23 • 53K D : and assuming '8--n/fl-2n=4 as in 33Na • 53Ca D : ' 8 - n=40( 10)% is given as a lower limit, see ENSDE • 53Fern T : average 96Ge.A=2.48(0.05) 68De27=2.51(0.02) 67Es06=2.58(0.03)

54 K -- 5600# 900#

54Ca --23590# 700# 54 Sc -- 34470 470 54-fi --45760 230 54V --49887 15 54Cr --56928.3 1.4 54Mn --55551.3 1.7 54Fe --56248.4 1.3 54Co - 4 8 0 0 5 . 3 1.3 54Com --47806 4 199 4 54Ni --39210 50 54Cu --21690# 210# 54Zn --6570# 400#

10 ms 5 2 - # 95 '8 -=100; ' 8 - n=? 80# ms 0 + 95 ' 8 - ?; ' 8 - n ? 230 ms 70 3+# 95 95So.A TD '8 -=100; ' 8 - n ? 1.5 s 0.4 0 + 95 96Do23 'IT) ' 8 - = 1 0 0

49.8 s 0.5 3 + 95 ' 8 - = 1 0 0 STABLE 0 + 95 1S=2.365 7

312.3 d 0.4 3 + 95 e=100; ' 8 - < 2 . 9 e - 4 ; e+<5.Te-7 STABLE 0 + 95 1S=5.845 35; 2'8 + ? 193.23 ms 0.14 0 + 95 '8+=100

1.48 m 0.02 (7) + 95 '8+=100 143 ms 23 0 + 95 95Re.B T /3+=100

< 75 ns 3+# 94B110 T p ? 0 + 2p ?

55K --570# 1000# 55Ca -- 18120# 700# 55Sc --30340# 1030# 55Ti --41810 240 55V --49150 t00 55Cr --55103.3 1.4 55Mn --57706.4 1.3 55Fe --57475.0 1.3 55Co --54023.7 1.4 55 Ni -- 45330 11 55Cu --31620# 300# 55Zn -- 14920# 250#

3# ms 3 /2+# / 3 - ?; '8--n ? 50# ms 5 /2 - -# ,8-- ? 130 ms 40 7 /2 - -# 95So.A TD '8 -=100 ; ' 8 - n ? 570 ms 70 3 / 2 - # 96Do23 'I'D ' 8 - = 1 0 0 6.54 s 0.15 7 / 2 - # 95 ' 8 - = 1 0 0

3.497 m 0.003 3/2 - 95 ' 8 - = 100 STABLE 5/2-- 95 IS=100.

2.73 y 0.03 3/2-- 95 e=100 17.53 h 0.03 7 / 2 - 95 ~6+ =IG0 207 ms 5 7 /2-- 95 95Re.B T fl+ =100

> 200 ns 3 / 2 - # 95 ~+ ?; p ?

20# ms 5 / 2 - # '8+ ?; 2p ? • 55Ii T : average 96Do23=600(40) 95Am.A=400(100) • 55Ni T : average 95Re.B=209(3) 87Ha.A=212.1(3.8) 84Ay01=208(5) 77Ho25=189(5) • 55Ni T : and 76Ed.A=219(6)

Z C a - 1 3 2 4 0 # 900# 10# ms 0 + 56Sc - 2 5 4 7 0 # 700# 80# ms 3+# 56"11 - 3 9 1 3 0 280 150 ms 30 0 + 56V - 4 6 2 4 0 240 230 ms 25 3~-# 56Cr - 5 5 2 8 9 10 5.94 m 0.10 0 + 93 56Mn --56905.6 1,4 2.5785 h 0.0002 3 + 93 56Fe --60601.0 1.4 STABLE 0 + 93 56Co --56035.0 2.4 77.27 d 0.03 4 + 93

Ni -- 53900 11 5.9 d 0.1 0 + 93 56Cu --38600# 140# > 200 ns 4+# 56Zn --25730# 260# 36 ms 10 0 + 56Ga --4740# 260# 3+#

*56Zn T : half-life is derived from experimental (p.n) cross sections

' 8 - ? ' 8 - 7

96Do23 TD , 8 - =100; , 8 - n ? 96So.A TD ' 8 - =100; ' 8 - n ?

' 8 - = 1 0 0 ' 8 - =100 IS---91.754 36 0+=100 '8+=100

87Po04 T '8+ ? 95Wa.A T '8+ ?

p ?


Nuclide Mass excess Excitation Half-life j,,r Ens Reference Decay modes and intensities (keV) energy(keV) (%)

57Ca --7120# 100(1#

57Sc --21390# 700#

57,fi - M560# 9 ~ #

57V --44380 2511

57Cr - 5 2 3 9 0 911

57Mn --57485 3

57Fe --60175.7 1.4

57Co --59339.7 1.4

57Ni --56075.5 2.9

57Cu --47305 16

57Zn --32690# 1411#

57Ga -- 15900# 260#

• 57Ti T : average 96Do23=56(20) 95Am.A=180(40)

5# ms 5 / 2 - # / 3 - ? ; / 3 - n ?

30# ms 7 / 2 - # / 3 - ?

80 ms 50 5 / 2 - # 96Do23 TD / 3 - = 1 0 0 ; / 3 - n ?

320 ms 30 7 / 2 - # 96So.A TD / 3 - =lif0; / 3 - n ?

21.1 s 1.0 3 / 2 - - , 5 / 2 - , 7 /2 93 / 3 - =100

85.4 s 1.8 5 /2-- 93 / 3 - =100

STABLE 1/2-- 93 IS=2.119 10

271.79 d 0.09 7 / 2 - 93 e=100

35.60 h 0.06 3 / 2 - 93 /3+=1011

196.3 ms 0.7 3 / 2 - 93 96Se01 T /3+=100

40 ms 10 7 / 2 - # 93 76Vi02 D /3+=100; /3+p~65

1 / 2 - # p ?

58 Sc -- 15770# 80{)# 3 + #

58 -fi -- 31570# 70(1# 0 +

58V --40380 260 3 ~ #

58Cr --51930 240 0 +

58 Mn -- 55900 30 0 +

58Mnm --55830 30 71.78 0.05 3 ~

58Fe --62148.8 1.4 0 +

58Co --59841.4 1.7 2 +

58Com --59816.5 1.7 24,889 0.021 5 +

58Ni --60223.0 1.4 0 +

58Cu --51660.0 2.5 1 -~

58Zn --422911 50 0 +

58Ga --23990# 210# * 2+#

58Gain --23960# 210# 30# 30# * 5+#

58Ge --8370# 320# 0 ~

• 58V T : average 95Am.A=270(40) 96So.A=205(20)

• 58Mn J : 1 + in post cut-off date ENSDF'97

• 58Mn m J : (4) +, T=65.210.5) s and IT=20%# in post cut-off date ENSDF'97

• 58Co T : 70.86(0.07) d in post cut-off date ENSDF'97

• 58Co m T : 9.04(0.11) d and E=24.9510,06) in post cut-off date ENSDF'97

• 58Zn T : from estimated 7'--50-80 ms, from ENSDF

10# ms /3-- ?

> 150 ns 92We04 T /3-- ?

218 ms 26 96So.A TD /3-=100; / 3 - n ?

7.11 s 0.3 90 /3 - = 100

3.(I s 0.1 96 / 3 - = 1 0 0

65.3 s 0.7 96 92Sc.A E / 3 - ,,~ 100; IT=?

STABLE 90 1S=0.282 4

70.82 d 0.03 90 /3+=100

9.15 h 0.10 90 IT=I00

STABLE >700Ey 96 93Va19 T IS=68.077 9; 2/3 ~ ?

3.204 s 0.007 90 /3+=100

65# ms 911 /3~ =1011; /3+ p=60# p ?

p ?

2p ?

D : /3+p=50-70%# estimated in ENSDF

59 Sc -- 11140# 900# 10# ms

59Ti --26120# 700# 50# ms

59V --37910 330 140 ms 70

59Cr --47850 250 460 ms 50

59Mn --55473 29 4.6 s 0.l

59Fe --60658.4 1.4 44,503 d 0.006

59Co --62223.6 1.4 STABLE

59Ni --61151 .I 1.4 80 ky i1

59Cu --56351.5 1.7 81.5 s 0.5

59Zn --47260 40 182.0 ms 1.8

59Ga --34120# 170#

59Ge -- 17000# 280#

7/2 # / 3 - ?; / 3 - n ?

5/2- # /3 - ? 7 / 2 - # 93 95So.A TD /3-=100; / 3 - n ?

5 / 2 - # 93 96Do23 T / 3 -=100

3 / 2 - , 5 / 2 - 94 / 3 - =100

3/2-- 93 / 3 - =10(I

7 /2-- 93 IS=100.

3/2-- 93 94Ru.1 T /3+=1011

3/2-- 93 /3+=1011

3/2-- 93 /3+=100; /3~-p---0.10 3

3 / 2 - # p ?

7 / 2 - # 2p ?

• 59Ti I : discovered by time-of-flight spectrometry, in post cut-off date 97Be12, thus T>150ns

. 5 9 V T : average 95Am.A=200(30) 95So.A=70(40)

• Y~Ni T : average of discrepant 94Ru.1=108(13) 81Ni08=76(5)

G. Audi et al. /Nuclear Physics A 624 (1997) 1-124 35

Nuclide Mass excess Excitation Half-life j,r Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

6011 -- 22690# 800# 60V --33070 560 60Cr --46830 260 60Mn --52910 270 60Mnm --52640 270 271.90 0.10 60Fe --61407 4 60Co --61644.2 1.4 60Co'~ --61585.6 1.4 58.59 0.01

~Ni --64468.1 1.4 60Cu --58341.2 2.5 60Zn --54183 11 60Ga --40000# 110# 60Ge --27770# 230#

6°As --6400# 600# 60As" --6340# 600# 60# 20#

30# ms 0 + ,O- ? 220 ms 30 3+# 95Am.A TD 8-=100; ' 8 - n ? 490 ms 60 0 + 93 96Do23 T 8 - =100

51 s 6 0 + 94 f l -=100 1.77 s 0.02 3 + 94 92Sc.A E '8-=88.5 8; 1T=ll.5 8 1.5 My 0.3 0 + 93 '8-=100

5.2714 y 0.0005 5 + 93 '8-=100 10.467 m 0.006 2 + 93 IT,~,100; fl----0.24 3

STABLE fl+ 96 IS=26.223 8 23.7 m 0.4 2 + 93 '8+=100 2.38 m 0.05 0 + 93 '8+=100

> 1.2 /zs 2+# 95B106 T '8+ ? .'K)# ms 0 + '8+ ?; 2p ?

5+# p ? 2+# p ?

,60,fi I : discovered by time-of-flight spectrometry, in post cut-off date 97Be12, thus T>150es *60Cr T : average 96Do23=510(150) 95Am.A=380(30) and 88Bo06=570(60)

61Ti -- 16750# 900# 6Iv --30360# 700# 61Cr --42760 280 61Mn --51740 260 61Fe --58917 20 61Co --62895.0 1.6 61Ni --64216.8 1.4 61Cu --61979.6 1.8 61Zn --56342 16 61Ga --47350# 200# 61Ge --33730# 300# 6lAs --18050# 600#

10# ms 1 / 2 - # ' 8 - ?; '8--n ? > 150 es 7 / 2 - # 92We04 T ' 8 - ?

260 ms 20 5 / 2 - # 93 95Am.A TD '8-=100; ' 8 - n ? 710 ms 10 ( 5 / 2 ) - 93 '8-=100 5.98 m 0.06 3 / 2 - , 5 / 2 - 93 '8-=100 1.650 h 0.005 7 / 2 - 93 ' 8 - =100

STABLE 3/2-- 93 IS=1.140 1 3.333 h 0.005 3 / 2 - 93 '8+=100 89.1 s 0.2 3 / 2 - 93 '8+=100 150 ms 30 3 / 2 - # 93 93Wi03 TD '8+=100 4(I ms 15 3 / 2 - # 93 '8+=100; '8+ p~80

3 / 2 - # p ? • 61"[i | : discovered by time-of-flight spectrometry, in post cut-off date 97Be12, thus T>150ns

62V -25020# 700# > 150 ns 62Cr --41170 370 160 ms 10 62Mn --48470 260 880 ms 150 62Fe --58898 15 68 s 2 62Co --61428 20 1.51) rn 0.04 62Co m --61406 21 22 5 13.91 m 0.05 62Ni --66742.7 1.4 STABLE 62Cu --62795 4 9.74 m 0.02 62Zn --61167 l0 9.186 h 0.013 62Ga --51996 28 116.12 ms 0.23 62Ge --42240# 140# > 150 ns 62 As --24960# 300#

*62Ge I : T=113(+6-5) ms in 93Wi03 (table 1) is a misprint for 62Ga *62As D : p-unstable from estimated Sp=-1476#(422#) keV

3+# 95Cz.A T ,0-- ? 0 + 95Am.A TD fl--=100; f l - n ?

(3 + ) 90 fl-- =100; ' 8 - n ? o + 90 ,8-=100 2 + 90 '8-=100 5 + 90 ' 8 - >99; IT< 1 0 + 90 IS=3.634 2

1 + 90 '8+=100 0 + 90 '8+=100 fl+ 90 fl+=100 0 + 91Mo10 T '8+ ? 1+# p ?

63V --21660# 900# 63Cr --35530# 700# 63Mn --46750 280 63Fc --55780 190 63Co --61837 20 63Ni --65509.2 1.4 63Cu --65576.2 1.4 63 Zn -- 62209.3 2.1 63Ga --56690 100 63Ge --46910# 200# 63 As -- 33820# 500#

> 150 ns 7 / 2 - # 95Cz.A T f l - ? 70 ms 10 1 / 2 - # 95Am.A TD '8-=100; f l - n ? 282 ms 18 5 / 2 - # 91 85Bo49 T f l - =100 6,1 s 0.6 ( 5 / 2 ) - 91 fl--=lO0 26.9 s 0.4 ( 7 / 2 ) - 91 941t.A T fl--=100 100.1 y 2.0 1 /2- 91 f l -=100

STABLE 3/2-- 91 IS=69.17 3 38.47 m 0.05 3 / 2 - 91 fl+ =100 32.4 s 0.5 3 / 2 - , 5 / 2 - 91 /~=100 97 ms 22 3 / 2 - # 93Wi03 TD '8+ =100

3 / 2 - # p ? *63Mn T : average 95Am.A=290(20) 85Bo49=250(40) .63Co T : average 941t.A=26.4110.27) 721008=27.5(0.3) 69Wa15=26(11 *63Ge T : symmetrized from 95(+23-20) *63As D : p-unstable from estimated Sp=-1132#(522#) keV

ag~

36 G. Audi et aL/Nuclear Physics A 624 (1997) 1-124


64 V

64Cr --33350# 700# 64Mn --43100 330

64Fe --550811 280 64Co --59789 20 64Ni --67095.9 1.4 64Cu --65420.8 1.4 64Zn --65999.5 1.7 64Ga --58835 4 6aGe --54420 250 64 As -- 39520# 360#

> 150 as 95Cz.A T / 3 - ? > 1 ~ 0 + 89Ar.A T / 3 - ? 240 ms 30 3+# 96 95Am.A TD /3-=100; / 3 - n ?

2.0 s 0.2 0 + 96 /3 - =100 300 ms 30 I + 96 /3 - =100

STABLE 0 ~ 96 IS=0.926 1 12.700 h 0.002 l + 96 fl+=61.0 3; /3-=39.0 3

STABLE >2.3Ey O ~ 96 85No03 T IS=48.6 3; 2/3 + ? 2.627 m 0.012 01+#1 96 fl~=100 63.7 s 2.5 11 + 96 /3+=100 > 1.2 ,us 0+# 95B106 T 13 + ?

65Cr --27600# 900# 65Mn --41/8911 560 6SFe --51290 280 65Co --59164 13 65Ni --65122.6 1.5 65Cu --67259.7 1.7 65Zn -65907 .8 1.7 65Ga -62652 .9 1.8 65Ge --56410 100 65 As -- 47060# 390# 65Se -- 32920# 600#

> 150 ns 1 / 2 - # 95Cz.A T /3 - ? 160 ms 30 5 / 2 - # 93 95Am.A TD /3-=100; / 3 - n ? 760 ms 50 1 / 2 - # 93 95Am.A T / 3 - =100 1.20 s 0.06 (7 /2 ) - - 93 / 3 - = 100

2.5172 h 0.01103 5 / 2 - 93 / 3 - =100 STABLE 3/2-- 93 IS=30.83 3 244.26 d 0.26 5 / 2 - 93 1~ =100

15.2 m 0.2 3 / 2 - 93 /3+=100 311.9 s 0.5 ( 3 / 2 ) - 93 87Vi01 D fl+=100; /3+p--0.011 3 19(I ms 11 3 / 2 - # 93 95Mo26 T /3 I~ =100

< 50 ms 3 / 2 - # 93 94Mo.A T /3'~=100; fl~-p=? *65Fe T : supersedes 94Cz02=450(150) from same group ,65Sc D : from 92Ba.A

66Cr

66Mn -- 36500# 700# 66Fe --50320 330 66Co --56050 270 66Ni --66029 16 66Cu --66254.3 1.7 66Zn --68896.3 1.5 66Ga --63721 3 66Ge --61620 30 66As --51820# 200# 66Se --41720# 300#

> 150 ns 11 ~ 95Cz.A T /3 ? 220 ms 40 95Am.A TD /3--=100; / 3 - n ? 600 ms 60 0 + 92 95Am.A TD /3-- =100; / 3 - n ? 230 ms 20 3+# 91 /3 - =100 54.6 h 0.4 0 + 92 /3-- = 100

5.088 m 0.011 1 "~ 92 / 3 - =100 STABLE 0 ~ 92 IS=27.9 2

9.49 h 0.07 0 + 91 /3+=100 2.26 h 0.05 0 + 92 fl+=100

95.77 ms 0.23 91 fl~=100 > 1.2 /zs 0 + 95B106 T /3+ ?

67Cr 50# ms 1 / 2 - # f l - ? 67Mn --337110# 8110# > 150 ns 5 / 2 - # 95Cz.A T fl-- ? 67Fe --46570 470 500 ms ll30 1 / 2 - # 91 95Am.A TD /3--=100; / 3 - n ? 67C0 --55320 280 320 ms 30 7 / 2 - # 91 85Bo49 T f l - =100 67Ni --63742 19 21 s I 1 /2- -# 94 ,0--=100 67Nim --63060# 100# 680# 100# 9 /2+# fl-- ?; IT ? 67Cu --67300 8 61.83 h 0.12 3 / 2 - 91 f l - =100 67Zn --67877.2 1.6 STABLE 5/2-- 91 IS=4.1 1 67Ga --66876.7 1.8 3.2612 d 0.01306 3 / 2 - 96 e=100 67Ge --62654 5 18.9 m 0.3 1 / 2 - 91 fl+=100 67As --56640 100 42.5 s 1.2 ( 5 / 2 - ) 91 fl~=100 67Se --46490# 200# 69 ms 15 5 / 2 - # 95B123 TD fl+=100; /3+p=0.5 1 67Br --32800# 500# 1 / 2 - # p ?

• 67Cr 1 : discovered by time-of-flight spectrometry, in post cut-off date 97Be12, thus T>150ns • 67Co T : average 95Am.A=310(20) 85Bo49=420170) • 67NilUs E : estimated from 9/2 ÷ level in isotones 71Ge=19810) 69Zn=438(0) • 67Se T : average 95B123--601+17-11) 94Ba50=-10"/135) • 67Se T : post cut-off date 97Oi01: values from 95B123 for 67Se and 71Kr questioned


Nuclide Mass excess Excitation Half-life j,n- Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

68Mn

68Fe --44240# 700# 68Co --51830 330 68Ni --63486 17 68Cu --65540 50 68Cure --64820 50 721.6 0.7 68Zn --70004.0 1.6 68Ga --67082.9 2.0 68Ge --66977 6 68As --5888O 100 68Se --54150# 300# 68Br --38890# 540#

> 150 ns 95Cz.A T / 3 - ? 100 ms 60 0 + 96 /3-=100; / 3 - n ? 310 ms 30 96 95Am.A T / 3 - = 100

17 s 5 0 + 96 / 3 - = 100 31.1 s 1.5 1 + 96 /3--=100 3.75 m 0.05 ( 6 - ) 96 1T=84 1 ; / 3 - = 1 6 1

STABLE 0 + 96 1S=18.8 4 67.629 m 0.024 1 + 96 /3+=100 270.8 d 0.3 0 ÷ 96 e=lO0 151.6 s 0.8 3 + 96 /3+=100 35.5 s 0.7 0 + 96 fl+ =100

< 1.2 /.Ls 3+# 95B106 T p ?

• 68Co T : supersedes 91Be33=180(100) from same group

• 68Ni T : symmetrized from 19(+3-6)

69Mn

69Fe --39400# 800# 69Co --51050 370 69Ni --60380 140 69NinJ --59990# 170# 390# 100# 69Cu --65740 8 69Zn --68414.9 1.7 69Znm --67976.3 1.7 438.64 0.02 69Ga --69321 3 69Ge --67094 3 69As --63O80 3O 69Se --56300 30 69Br --46410# 310# 69Kr --32300# 500#

> 150 as 5 / 2 - # 95Cz.A T /3-- ? 90 ms 10 1 / 2 - # 95Am.A TD ,8 -=100; / 3 - n ?

270 ms 50 7 / 2 - # 90 91Be33 TD /3-=100; / 3 - n ?

11.4 s 0.3 1 / 2 - # 90 / 3 - = 100 9 /2+# / 3 - ?; IT ?

2.85 m 0.15 3/2-- 90 / 3 - =100 56.4 m 0.9 1 / 2 - 90 / 3 - =100 13.76 h 0.02 9 /2 + 90 1T~100; /3---0.033 3

STABLE 3/2-- 90 IS=60.108 6 39.05 h 0.10 5 / 2 - 90 /3+=100 15.2 m 0.2 5 / 2 - 90 /3 + =100 27.4 s 0.2 ( 1 / 2 - ) 90 95Po01 J /5'+=100; /3+p--0.045 10 < 24 ns 1 / 2 - # 90 96Pf01 T p ?

> 1.2 bts 5 /2 - -# 95BI06 T 13 + ? • 69Ni" E : estimated from 9/2 + level in isotones 73Ge=-66(0) 71Zn=157(1) • 69Kr T : 32(10) ms ft'om /3+p in pest cut-off date 97Xu01

70Fe

70Co --46750# 700# 70Ni --59490 330 70Cu --62960 15 * 70Cu m --62820 80 140 80 BD * 70Zn --69559 3 70Ga --68905 3

7°Ge --70560.3 1.7 7°As --64340 50 7°Se --61940# 210# 70Br --51590# 360# 70Brm --51590# 370# 0# 100# 70Kr --40980# 400#

> 150 ns 230 ms 20 > 1 /.ts 4.5 s 1.0 1 + 93 47 s 5 3 - - . 4 - - , 5 - - 93

STABLE 0 + 93 21.14 m 0.03 1 + 93

STABLE 0 + 93 52.6 m 0.3 4 (+#~ 93 41.1 m 0.3 0 + 93

* 7 9 . 1 ms 0.8 93 * 2 . 2 s 0.2 93

> 1.2 /.ts 0 +

0 + 95Cz.A T / 3 - ? 93 95Am.A TD /3-=100; / 3 - n ?

0 + 93 93Se.A T / 3 - ? / 3 - =100 / 3 - = 100 IS=0.6 1; 2 /3 - ? / 3 - ~100; e=0.41 6 IS=21.23 4 /3+=100 /3+=100 /3+=100

/3+=?; IT ? 95B106 T /3+ ?

*70Zn T : >500 Ty in ENSDF is for 0~,-2/3-- decay alone

71Fe

71Co --44960# 800# 71Ni --55890 370 71Cu --62760 40 71Zn --67322 11 71Znm --67164 11 157.7 1.3 71Ga --70136.8 1.8

. . . A-group is continued on next page . . .

> 150 ns 7 /2+# 95Cz.A T /3-- ? 270 ms 50 7 / 2 - # 93 95Am.A TD /3-=100; / 3 - n ? 1.9 s 0.4 1 / 2 - # 93 / 3 - = 100

19.5 s 1.6 ( 3 / 2 - ) 93 / 3 - = 100 2.45 m 0.10 1 / 2 - 93 / 3 - =100 3.96 h 0.05 9 /2 + 93 / 3 - ~ 100; IT<0.05

STABLE 3/2-- 93 IS=39.892 6



. . . A-group continued . . . 71Ge --69904.9 1.7 71Ge"* -69706 .5 1.7 198.367 0.010 71 As -- 67892 4 71Se -- 63090# 200# 71Br --56590# 300# 71Kr --46100# _'~0# 71Rb --32300# 500#

.71Kr T : average 95BI23=64(+8-5) 81Ew01=97(9)

11.43 d 0.03 1 / 2 - 93 e=100 20.40 ms 0.17 9/2 + 93 IT= 100

65.28 h 0.15 5 / 2 - 93 /3+=100 4.74 m 0.05 5 / 2 - 93 /3+=I00 21.4 s 0.6 ( 5 / 2 ) - 93 /3 I =100 81 ms 16 5 / 2 - # 93 95B123 TD /3;=100; /3+ p=5.2 6

5 / 2 - # p ?

.71Kr T : post cut-off date 97Oi01: T=100(3) ms and/3+p=2.1(7)% at variance with 95BI23 and

.71Kr T : J ~ = ( 5 / 2 - ). Values fi'om 95B123 for 67Se and 71Kr questioned by 97Oi01

72 Fe

72Co --40600# 800# 72Ni --54680 470 72Cu --60060# 200# 72Zn --68128 6 72Ga -68586 .5 2.0 72Gain -68466 .8 2.11 119.66 0.05

72Ge -72585 .6 1.5 72As --68229 4 72Se --67894 12 72Br --59150 260 72Br nJ --59050 260 100,92 0.03

72 Kr -- 54110 270 72Rb --38120# 500# 72Rbm --38020# 500# 100# 50#

> 150 ns 0 + 100 ms 50 1.30 s I1.111 0 ~- 6.6 s 0.1 ( i + ) 95

46.5 h 0.1 0 q- 95 14.10 h 0.02 3 - 95 39.68 ms 0.13 (0 + ) 95

STABLE 0 + 95 26.0 h 0.1 2 - 95 8.40 d 0.08 0 + 95 78.6 s 2.4 3 + 95 10.6 s 0.3 1 - 95

17.2 s 0.3 0 + 95 < 1.2 ,us 3+#

1 - #

• 72Ni T : supersedes 92Be.A=2.06(0.30) from same group

95Cz.A T /3 - ? 95Am.A TD /3-=100; / 3 - n ? 95Am.A TD /3-=1110; / 3 - n ?

/3- =lOO / 3 - =100 / 3 - =100 IT=I00

I8=27.66 3 /3+=100 ~=100 /3+=100 I T ~ I00; /3+='?

/3~ =100 95B106 T p ?

p ?

73 Co

73 Ni -- 50230# 600# 73Cu - 5 9 1 6 0 # 300# 73Zn --65410 40 73Zn" --65220 40 195,5 2.0 73Ga --69704 6 73Ge --71297.1 1.5 73Ge m --71230.4 1.5 66.716 0.019 73 As -- 70956 4 73Se --68216 11 73Se m --68190 11 25.71 0.04 73Br --63530 1311 73Kr --56890 141.1 73Rb --46230# 480# 73Sr --31700# 600#

> 150 ns 7 / 2 - # 95En07 T 800 ms 100 7 /2+# 93 95Am.A T 3.9 s 0.3 3/2 # 93

23.5 s 1.0 1 1 / 2 ) - 93 5.8 s 0.8 17/2 + ) 93

4.86 h 0.03 3 / 2 - 93 STABLE 9/2 + 93

499 ms l 1 1/2 -- 93 80.30 d 0.06 3 / 2 - 93 7.15 h 0.08 9/2 ~ 93 39.8 m 1.3 3/2-- 93 3.4 m 0.2 1/2-- 93

27.0 s 1.2 5/2-- 93 < 30 ns 5/2-- # > 25 ms 1 /2- -#

• 73Ni T : supersedes 90Be13--900(150) from same group

/3 ? /3-=100; / 3 - n ? /3-=100; / 3 - n ? /3-=1110 IT=?; / 3 - =?

/3 =100 IS=7.73 1 1T=100 e=100 /3+ =100 IT=72.6 3; 139 =27.4 3 /3+ =100 /3+ =100; /3+ p=0.68 12

96Pf01 T p ? 93Ba61 TD /3+=100; /3+ p=?

74Co

74Ni --48520# 700# 74Cu --55700# 400# 74Zn --65710 50 74Ga --68050 70 74Gain --67990 70 59.571 0.014 74Ge --73422.0 1.5 74As --70859.6 2.2 74Sc --72212.6 1.5 74Br --65306 15 74Brm --65292 15 13.58 0.21 74Kr --62170 60 74Rb --51730 720 74Sr --40700# 500#

> 150 ns 95En07 T 500 ms 200 11 + 95 95Am.A T

1.594 s 0.010 1+# 95 95.6 s 1.2 0 + 95 8.12 m 0.12 ( 3 - ) 95 9.5 s 1.0 (0) 95

STABLE 0 + 95 17.77 d 0.02 2-- 95

STABLE 0 ~ 95 25.4 m 0.3 ( 0 - ) 95 46 m 2 4 (÷#) 95

11.50 m 0.11 0 + 95 64.9 ms 0.5 (0 + ) 95

> 1,2 ,o,s 0 + 95B106 T • 74Ni T : supersedes 90Be13=1100(500) from same group

13- ? /3-=100; B - n ? /3 - =100 B - = 1 0 0 /3 - =100 IT=?; /3 -=25# IS=35.94 2 /3+=66 2; f l - = 3 4 2 IS--0.89 2; 2/3 '+ ? /3+=100 ,8+=100 /3+=100 B ~ =1110 /3 + ?


Nuclide Mass excess Excitation Half-life fir Ens Reference Decay modes and intensities (keV) energy(keV ) ( % )

75Co > 150 ns 7 / 2 - # 75Ni --43810# 800# 700 ms 400 7/2+# 75Cu --54310# 500# 1.224 s 0.003 3 / 2 - # 90 91Kr15 T 75Zn --62470 70 10.2 s 0.2 (7/2 + ) 90 75Ga --68464 7 126 s 2 3 / 2 - 90 75Ge --71855.9 1.5 82.78 m 0.04 1 /2 - 96 75Ge"r -71716.2 1.5 139.69 0.03 47.7 s 0.5 7/2 + 96 75As --73032.5 1.6 STABLE 3/2-- 96 75Asm --72728.6 1.6 303.9243 03~011 16.79 ms 0.15 9/2 + 96 75Se --72168.8 1.5 119.79 d 0.04 5/2 + 96 75Br --69139 14 96.7 m 1.3 3/2-- 90 75Kr --64242 15 4.3 m 0.2 5/2 + 90 95Ke04 J 75Rb --57222 8 19.0 s 1.2 ( 3 / 2 - , 5 / 2 - ) 90 75Sr --46650# 300# 100 ms 50 3 / 2 - #

• 75Ni D : .8-n=1.6%# estimated by 85Re01

95En07 T .8- ? 95Am.A TD .8-=100; .8-n=1.6#

.8-=100; .8 - n=3.5 6

.8-=100 /3- =100

f l -=100 IT~ 100; .8 - =0.030 6 lS=100. 13"--100 e=100 /3+=100 /3+=100 ~+=10o

95BI23 TD .8+=?; .8+p=6.5 33

• 75Se T : see 75As decay data set of ENSDF: 80Hol7's weight decreased hy LWM method • 75Sr T : symmetdzed from 71(+71-24)

76Ni --41610# 900# 440 ms 400 04 76Cu -50310# 600# * 641 ms 6 (3, 5) 95 90Wi12 J 76Cure --50310# 630# 0# 200# * 1.27 s 0.30 (1, 3) 95 90Wi12 J 76Zn --62040 120 5.7 s 0.3 0 + 95 76Ga --66200 90 32.6 s 0.6 (2 + , 3 + ) 95 76Ge --73212.9 1.5 1.09 Zy 0.13 0 + 95 94Ba15 T 76As --72289.6 1.6 1.0778 d 0.0020 2 - 95 76Se --75251.6 1.5 STABLE 0 + 95 76Br --70289 9 16.2 h 0.2 1 -- 95 76Brn' --70186 9 102.58 0.03 1.3l s 0.02 (4) + 95 76Kr --68979 11 14.8 h 0.1 0 + 95 76Rb --60481 8 36.5 s 0.6 1 ( - ) 95 78Ha08 D 76Sr --54390# 300# 8.9 s 0.3 0 + 95

• 76Ni T : symmetdzed from 240(+550-240) • 76Ge T : average 94Ba15=1.42(0.13) 90Val8=0.90(0.10) • 76Ge T : 93Br22--0.84(+0.104).08)(2(r) and 90Mi23=l.l(+0.6-0.3)(2cQ • 76Ge T : also 96Gu.1=1.77(+0.13-0.11) not used yet

95Am.A TD .8-=100; . 8 - n ? .8-=100; /3--n=3 2 .8-=100 O-=100 B - =100 IS=7.44 2; 2.8-=100 .8- ~100; ~<0.02 IS=9.36 11 /3+=100

1T>99.4; .8+ <0.6 .8+=100 .8+=100; .8+a=3.8e-7 10 .8+=100

77Ni --36490# 1000# > 150 ns 9/2+# 95En07 T .8-- ? 77Cu --48480# 700# 469 ms 8 3/2--# 89 91Kr15 T .8-=100 77Zn --58600 130 2.08 s 0.05 (7/2 + ) 94 B-- =100 77 Zn" --57830 1.'30 772.39 0.12 1.05 s 0.10 ( 1 / 2 - ) 94 IT>50; . 8 -<50 77Ga --65870 6(1 13.2 s 0.2 ( 3 / 2 - ) 89 .8-=100 77Ge --71214.1 1.8 11.30 h 0.01 7/2 + 89 ,8-=100 77Gem --71054.4 1.8 159.7 0.1 52.9 s 0.6 1 /2 - 89 .8--=79 2; IT=21 2 77As --73916.2 2.2 38.83 h 0.05 3 / 2 - 89 .8-=100 77Se --74599.0 1.5 STABLE 1/2-- 89 IS=7.63 6 77Sere --74437.1 1.5 161.9200 0.0013 17.36 s 0.05 7/2 + 89 IT=I00 77Br --73234 3 57.036 h 0.006 3/2-- 89 .8+=100 77Brn~ --73128 3 105.85 0.09 4.28 m 0.10 9/2 + 89 IT=100 77Kr --70171 9 74.4 m 0.6 5/2 + 89 /3+=100 77Rb --64826 8 3.80 m 0.04 3 / 2 - 89 93A103 T fl+=100 77Sr --57970 150 9.0 s 0.2 5/2 + 89 92Lill J .8+=100; /3+p<0.25 77y --46930# 300# < 1.2 #s 5/2+# 95B106 T p ?; fl+ ?

*77Rb T : average 93A103=3.78(0.04) 72At02=3.90(0.10)

78Ni --33720# 1100# > 150 es 0 + 95En07 T f l - ? 78Cu --43960# 800# 342 ms 11 91Kr15 T f l - =100 78Zn --57220 16(1 1.47 s 0.15 0 + 91 f l -=100 78Ga --63660 80 5.09 s 0.05 (3 + ) 91 f l - =100 78Ge --71862 4 88 m 1 0 + 91 .8- =100 78As --72816 10 90.7 m 0.2 2 - 91 .8-=100 78Se --77025.7 1.5 STABLE 0 + 91 IS=23.78 9


g t ~ ¢

4 0 G. Audi et al./Nuclear Physics A 624 119971 1-124

Nuclide Mass excess Excitation Half-life ,fir Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

. . , A-group continued . . . 78Br --73452 4 6,46 m 0.04 1 + 91 78Kr --74160 7 STABLE > l l 0 E y 0 + 91 94Sa31 T 78Rb --66936 8 17.66 m 0.08 0 (+) 91 78Rb m --66825 8 111.211 0.10 5.74 m 0.05 4 ! - ) 91 91Mc.A E 78Sr --63175 8 159 s 8 0 + 91 92Gr09 T 78y --52630# 400# > 150 ns 92Ye04 T

*78Br D : , 8 - branch is uncertain. See ENSDF *78Kr T : limit given here is for the K-e + decay (theoretically faster)

/3 + ~ 100; , 8 - <0.01 1S=0,35 2; 2,8 + ? ,8+=100 ,8+--90 2; IT=I0 2 /3+=100

/3+ ?

79Cu --41660# 900# 79Zn -- 5M00# 270# 79Ga --62490 120 79Ge --69490 911 79Gem --69300 90 185.95 0.04 79As --73636 6 79Se --75916.9 1.5 79Sere --75821.1 1.5 95.77 0.03 79Br --76068.0 t.9

79Brm --75860.5 1.9 207.52 0.10 79Kr --74442 4 79Ktan --74312 4 129.78 0.05 79Rh --70797 7 79Sr --65477 9

7') y -- 58360 450 79Zr --47360# 400#

188 ms 25 3 / 2 - # 94 995 ms 19 (9/2 + ) 94

2.847 s 0.003 ( 3 / 2 - ) 94 18.98 s 0.03 ( 1/2 ) - 94

39.0 s 1.0 (7/2 + ) 94 9.01 m 0.15 3 / 2 - 94

< 650 ky 7/2 + 94 3.92 m 0.01 1 / 2 - 94

STABLE 3/2 - 94 4.86 s 0.04 9/2 + 94 35.04 h 0,10 1 / 2 - 94

50 s 3 7/2 + 94 22.9 m 0.5 5/2 + 94 2.25 m 0.10 3/2 ( - I 94

14.8 s 0.6 (5/2 + ) 94 200# ms 5/2 ~ #

/3-=100; , 8 - n=55 17 ,8-=100; B - n=l.3 4 ,8 -=100; , 8 - n=0.089 19 , 8 - =100 , 8 - = 9 6 1; IT=4 1 , 8 - =100 fl-- =100 IT~,-"~100; ,8-=0.056 11 IS=50.69 7 1T=100

B+=100 IT=100 /3+=100 3+=100 ,8': =100; #+p ? ,8+ 7; fl+ p ?

80Cu --35500# 900# 80Zn --51780 170

8°Ga --59070 1211 80Ge -69448 23 80As --72118 21 80Se --77759.4 1.9 80Br --75888.8 1.9 80Bi ~n --75803.0 1.9 85.843 0.004 80Kr --77893 4 80Rb --72173 7 80Sr --70?,05 8 80y --61170# 400# 8°Zr - 5 5 3 8 0 #

*8°Zr T : > 10 us in post cut-off date 97Is.A

> 150 ns 95En07 T 545 ms 16 0 + 92

1.697 s 0.011 (3) 92 93Ru01 D 29.5 s 0.4 0 + 92 15.2 s 0.2 1 + 92

STABLE 0 + 92 17,68 m 0.02 1 + 92

4.4205 h 0.11008 5 - 92 STABLE [)+ 92

33.4 s 0.7 1 + 92 93A103 T 106.3 m 1.5 0 + 92

35 s 2 13,4,51 92 > 150 ns 04 92 92Ye04 T

, 8 - - ? 3--=100; ,8--n=l .0 5 /3--=100; , 8 - n=0.89 6 , 8 - =100 , 8 - =100 IS-~9.61 10; 2 ,8- ? ,8---91.7 2; ,8+=8.3 2 1T=100 IS=2.25 2 /3+=100 ,8+ =100 ,8'~ =lID

,8+ ?

81Zn --46130# 400# 81Ga - 5 7 9 8 0 190 81Ge --66.°,00 120

81Gem --65620 1211 679.13 0.04 81As --72533 6 81Se --76389.I 2.0 81Se m --76286.1 2.0 102.99 0.06 81Br --77974.4 2.8 8tKr --77693.6 2.9 81Kr n, --77503.1 2.9 190.62 0.04 81Rb --75456 6 81Rbm --75370 6 86.31 0.07 81Sr --71527 8 81y --66020 60 81Zr -- 58860 300 81Nb -- 47460# 400#

290 ms 50 5/2 + # 97 1.217 s 0.005 ( 5 / 2 - ) 97

8 s 2 9 /2+# 97

8 s 2 11/2 + ) 97 33.3 s 0.8 3/2 - 97 18.45 m 0.12 1 / 2 - 97 57.28 m 0.02 7/2 + 97

STABLE 3/2 - 97 229 ky 11 7/2 + 97

13.10 s 0,03 1 / 2 - 97 4.576 h 0.005 3 / 2 - 97 30.5 m 0.3 9 /2 + 97 22.3 m 0.4 1 / 2 - 97 70.4 s 1.0 (5/2 + ) 97

15 s 5 3 / 2 - # 97 800# ms 3 / 2 - # 97

,81Go T : derived from 7.6(0.6), for mixture of ground-state and isomer with almost same half-life *81Nb T : estimated half-life is for 13 + decay; p-decay would be much shorter

,8--=100; ,8--n=7.5 30 /3--=100; fl-- n=l l .9 7 ,8-- =100 ,8-- ,-~ 100; r r < l B - =ICO , 8 - =100 ITm.100; ,8----0.052 14 1S=49.31 7 e=100 IT~,,~ 100; ,e--0,0025 4 ,8+=100 1T=97.6 6; 13 + =2.4 6 ,8+=100 /3+=100 /3+=100; /3+ p=? /3+ ?; 134 p ?; p ?

8t~

go*


Nuclide Mass excess Excitation Half-life fir Ens Reference Decay modes and intensifies (keV) energy(keV ) (%)

82Zn --42070# 400# > 150 ns 0 + 95Cz.A T /3- ?

82Ga --52950# 300# 599 ms 2 (1,2, 3) 95 93Ru01 D ,8-=100; /3-n=21.5 23 82Ge --65620 240 4.6 s 0.4 0 + 95 /3-=100 82As --70320 200 * 19.1 s 0.5 (1 +) 95 /3-=100 82Asm --70075 25 250 200 BD * 13.6 s 0.4 ( 5 - ) 95 /3-=100

82Se --77593.4 2.1 121 Ey 17 (I + 95 IS=8.73 6; 2,8-=100 82Br --77495.9 2.8 35.30 h 0.02 5 - 95 /3-- =100 82B~mJ --77450.0 2.8 45.9492 0.0010 6,13 m 0.05 2 - 95 IT=97.6 3; /3-=2.4 3 82Kr --80588.6 2.6 STABLE 0 + 95 IS=I 1.6 l 82Rb --76189 7 1.273 m 0.002 l + 95 /3+=100 82Rbn' --76121 7 68.9 1.5 6.472 h 0.006 5-- 95 fl+~100; IT<0,33 82Sr --76009 6 25.55 d 0.15 0 + 95 ~=100 82y --68190 100 9.5 s 0.3 1 + 96 /3+=100 82Zr --64190 510 32 s 5 0 + 95 fl+=100 82Nb --52970# 300# > 150 ns 92Ye04 T 13 + ?

• g2Se T : symmetrized from 108(+26~5)

83Zn > 150 as 5/2+# 95Cz.A T /3- ?

83Ga --49490# 500# 308 ms 1 3 / 2 - # 92 91Kr15 T /3--=100; f l -n=40 14 83Ge --61000# ~ 1.85 s 0.06 (5/2 + ) 92 /3-=100 83As --69880 220 13.4 s 0.3 ( 5 / 2 - , 3 / 2 - ) 92 /3-=100 83Se --75340 4 22.3 m 0.3 9/2 + 92 /3-=100 83Se m --75112 4 228.50 0,20 70.1 s 0.4 1/2-- 92 /3--=100

83Br --79009 4 2.40 h 0.02 3 / 2 - 92 fl-- =100 83Kr --79982 3 STABLE 9/2 + 92 IS=I 1.5 1 83Kr" --79940 3 41.543 0,007 1.83 h 0.02 1 /2 - 92 IT=100 83Rb --79073 6 86.2 d 0.1 5 / 2 - 92 ~=100 83Rb m --79031 6 42.11 0,04 7.8 ms 0.7 9/2 + 6SEt01 T IT=100 83Sr --76797 9 32.41 h 0.03 7/2 + 96 /3+=100 8351 'm --76538 9 259.15 0.09 4.95 s 0.12 1/2-- 96 IT=I00 83y --72330 40 7.08 m 0.06 (9/2 + ) 92 /3+=100 83y,~ --72270 40 62.00 0.20 2.85 m 0.02 (3/2--) 92 /3+=60 5; IT--40 5 83Zr --66460 100 44 s 1 1/2--# 92 /3+=100; /3+ p=? 83 Zrn, non existent RN 8 s 1 high 87Ra06 1 83Nb --58960 310 4.1 s 0.3 (5/2 + ) 92 /3+=100 83Mo --47750# 500# 400# ms 3 / 2 - # ff~ ?; ~+p ?

*83Ga D : / 3 - n intensity is from 93Ru01

84Ga --44400# 600# 85 ms 10 91Kr15 TD ,8-=100; .t3--n=70 15 84Ge --58400# 400# 954 ms 14 0 + 89 93Ru01 TD ,8-=100; /3--n=10.8 6 84As --66080# .300# * 4.02 s 0.03 0 ( -1 . 1 ~-) , 2 - 89 93Ru01 TD fl-=100; fl-n=0.28 4 84Ash' --66080# 320# 0# 100# * 650 ms 150 89 f l -=100 84Se --75950 15 3.1 m 0.1 0 + 89 /3-=100

84Br --77776 25 31.80 m 0.08 2 - 89 fl--=100 84Br" --77460 100 320 100 BD 6.0 m 0.2 ( 5 - , 6 - ) 89 f l -=100 84Kr --82431 3 STABLE 0 + 89 IS=57.0 3 84Rb --79750 3 32.77 d 0.14 2 - 89 ,B+--96.2 5; /3-=3.8 5 84Rbm --79285 3 464.62 0.09 20.26 m 0.04 6 - 89 IT=I00; /3+ ? 8'lSr --80644 3 STABLE 0 + 89 1S=0.56 1; 2/~- ? 84y --74160 90 * 4.6 s 0.2 1 + 89 fl+=100 84ym --74240 170 --80 190 BD * 40 m 1 ( 5 - ) 89 /3+=100 84Zr --71490# 200# 25.9 m 0.8 0 + 96 fl+=100 84Nb --61880# ~ 12 s 3 (3 +) 89 /3+=100; fl+p ? 84Mo --55810# 400# > 150 ns 0 + 94He28 T fl+ ?

• 84Ge T : average 93Ru01=947(11) 91Krl5--984(231

4 2 G. Audi et al. /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life fir Ens Reference Decay modes and intensities (keV) energy(keV) (%)

85Ga > 150 ns 3 / 2 - # 95Cz.A T , 8 - ? 85Ge --53380# 500# 540 ms 50 5 /2+# 91Kr15 TD ,8-=100; /3 -n=14 3 85As --63520# 300# 2.022 s 0.009 ( 3 / 2 - - ) 91 93Ru01 DT ,8-=100; / 3 - n=59.4 24 85Se --72429 30 31.7 s 0.9 (5/2 ~ ) 91 `8 -=100 85Br --78611 19 2.90 m 0.06 3 / 2 - 91 /3 -=100 85Kr --81480.6 3.0 10.756 y 0.018 9/2 ~ 91 f l - =100 85Krm --81176 3 304.871 0.02(I 4.480 h (I.008 1 / 2 - 91 /3-=78.6 4; IT=21.4 4 85Rb --82167.7 2.3 STABLE 5/2 91 IS=72.165 20 85Sr --81103 3 64.84 d 0.02 9 /2 + 91 ~r=100 85Srm --80864 3 238.66 0.116 67.63 m 0.04 1 / 2 - 91 IT=86.6 4; f i t =13.4 4 85 y -- 77848 25 2,68 h 0.05 ( 1/2 ) 94 `8+ = 100 85y,~ --77828 25 19.8 0.5 4.86 h 0.13 9/2 + 94 `8+ ~ 100; IT<0.002 85Zr --73150 100 7.86 m 0.04 7/2 + 94 fl~ =100 85Zrm --72860 100 292.2 0,3 10.9 s 0.3 ( 1 / 2 - ) 94 IT<92; ,8+>8 85Nh --67150 220 20.9 s 0.7 (9/2 + ) 91 /3+=100 85Mo --5907(1# 400# > 150 ns 9 /2+# 92Ye04 T fl~ ? 85Te --47560# 500# 500# ms 9 /2~# ,.6 + ?; `8~p ?; p ?

*85As T : average 93Ru01=2.002(0.013) 91Kr15=2.032(0.012) 68To19=2.028(0.0121 ,85Tc T : estimated half-life is for `8+ decay; p-decay would be much shorter

,,g

86Ga

86Ge -- 50050# 600# 86As --59400# 40(~ 86Se --70541 16 86Br --75640 11 86Kr --83265.9 l . l 86Rb --82747.3 2,3 86Rbm --82191.2 2.3 556.0 0.2 86Sr --84521.6 2.2 86y --79282 14 86ynr --79(164 14 218.30 0.20 86Zr --77810 30 86Nb --69830 90 * 86Nbm --69580# 180# 250# 160# * 86Mo --64560 440 86Tc --53210# 300#

• 86Rbm E : 556.05(0.18) in post cut-off date ENSDF'97 • 86Nb J : 6 ~ in post cut-off date 97Ta10

> 150 ns 95Cz.A T , 8 - ? > 150 ns 0 + 94Be24 T , 8 - ?; / 3 - n ?

945 ms 8 88 93Ru01 TD `8 =100; , 8 -n=33 4 15.3 s 0.9 0 + 88 /3 - =100 55. I s 0.4 ( 2 - ) 88 , 8 - =100

STABLE 04 88 IS=17.3 2; 2 ,8- ? 18,631 d 0.018 2 - 94 , 8 - ~100; ~=0.1X152 5 1.017 m 0.003 6 94 IT=100

STABLE 0 + 88 1S=9.86 l 14.74 h 0.02 4 88 ,8+ =100

48 m 1 (8 ~ ) 88 1T=99.31 4; ,8+ --0.69 4 16.5 h (I.l 0 + 88 ,8+ =100 88 s 1 (5 + ) 88 ,84 =100

56 s 8 high 94Sh07 TD fl" =i(~q 19.6 s 1.1 (1~ 94Sh07 TD /3 I- =100

> 150 ns 92Ye04 T /3+ ?

87Ge

87 As -- 56280# 50,)# 87Se --665811 40 87Br --73857 18 87Kr --80710.0 1.3 87Rb --84595.0 2.5 87Sr --84878.4 2.2 87 SiJ" --84489.9 2.2 388.532 I).003 87y --83016.8 2.6 87ynr --82636.0 2.6 380.79 0.07 87Zr --79348 8 87Zrm --79012 8 335.73 (I.24 87Nb --74180 6(1 87Nbm --74180 611 3.9 0.1 87Mo --67690 220 87Tc --59120# 300# 87Ru -- 47_'M0# 600#

> 150 ns 5 /2+# 95Cz.A T , 8 - ? 560 ms 110 ( 3 / 2 - ) 91 93Ru01 DT ,8-=100; ,8-n=15.4 22 5.50 s 0.14 (5/2 + ) 91 93Ru01 DT ,8-=100; f l - n=0,36 8

55.60 s 0.15 3 / 2 - 91 93Ru01 D 76.3 m 0.6 5/2; 91 47.5 Gy (1.4 3 / 2 - 9l

STABLE 9/2 + 96 2.803 h 0.003 1 / 2 - 96 79.8 h 0.3 1/2-- 96 13.37 h 0.03 9/2 ~ 96 1.68 h 0.01 (9/2) + 91 14.0 s 0.2 (1 /2 ) - - 91

& 3.7 m 0,1 (1/2 ) 96 & 2.6 m 0.I (9/2 ~ ) 96 91Ju05 E

13.4 s 0.4 7 /2+# 91 83Ha06 D > 150 ns 9 /2+# 92Ye04 T > 1.5 #s 9 /2+# 95Le14 T

,8--=100; ,8-- n=2.52 7 , 8 - =100 1S=27.835 20; , 8 -=100 IS=Z00 l IT~I00; E---0.~l 8 ,8~ =100 IT=98.43 10; ,8+=1.57 10 /3 + =IC0 IT=I00 ,8+=100 ,8~=100 ,8+=100; ,81-p=15 8

,8+ ? ,8+ ?

*87As T : average 93Ru01=485(40) 78Cr03=730(60) .87Sc T : average 93Ru01=5.29(11) 70Kr05=5.85(15) 70De08=5.90(20) 71T013=5.41(101 .87Mo D : given ,84 p value corresponds to transition only through the first 2 ; state ,87Mo D : post cut-off date 97HUO7 `8÷ p=15(6)% (through 3 levels) and T=13.6(I.1) s


Nuclide Mass excess Excitation Half-life ./rr Ens Reference Decay modes and intensities (keV) encrgy(keV ) (%)

88Ge > 150 ns 88As --51640# 600# > 150 ns 88Se --63880 50 1.52 s 0.03 88Br --70730 40 16.36 s 0.07 88Kr --79692 13 2.84 h 0.03 88Rb --82606 4 17.78 m 0.11 88St --87919.7 2.2 STABLE 88y --84297.1 2.7 106.65 d 0.04 88ym --83622.6 2.7 674.55 0.04 13.9 ms 0.2 88Zr --83624 10 83.4 d 0.3 88Nb --76420# 200# * 14.5 m 0.1 88Nb m --76030 100 390# 220# BD * 7.8 m 0.1 88Mo --72701 20 8.0 m 0.2 88Tc --62570# 300# * 5.8 s 0.2 88Tcm --62570# 420# 0# 300# * 6.4 s 0.8 88Ru --55500# 500# > 150 ns

*88Br T : average 93Ru01=16.3410.08) 74Gr29=16.510.21

0 + 95Cz.A T , 8 - ? 94Be24 T , 8 - ?; , 8 - n ?

0" 88 93Ru01 D , 8 - =100; , 8 - n=0.99 10 ( 1 - ) 88 93Ru01 TD ,8-=100; ,8-n=6.58 18

0 + 88 ,8-- =100 2 - 88 , 8 - = 1 0 0 0 + 88 IS=82.58 1 4 - 88 ,8+=100

(8) + 88 IT=I00 0 + 88 e=lO0

(8 ~ ) 88 ,8+=100 ( 4 - ) 88 ,8+=100

0 + 88 .8+=100 3 + 96Od01 TJD ,8+=100

(6 + ) 96Od01 TJD .8+=100 0 + 94He28 T .8+ ?

89Ge

89As --47290# 600# 89Se --59600# 300# 89Br --68570 611 89Kr --76720 50 89Rb --81711 6 89Sr --86207.0 2.2 89y --877112.1 2.3 89ym --86793.1 2.3 908.96 89Zr --84869 3 89 Zr m -- 84281 3 89 Nb -- 80580 40 89Nb m -- 80580# 50# 89Mo --75003 15 89Mo m --74616 15 89Tc --67490 210 89Tc m --67490# 370# 89Ru --59510# 500# 89Rh --47150# 5(30#

0.04

587.84 0.09

0# 30#

387.5 0.3

0# 300#

> 150 ns 3 /2+# 95Cz.A T ,8-- ? > 150 ns 3 / 2 - # 94Be24 T . 8 - ?

410 ms 40 (5/2 + ) 90 93Ru01 D ,8 -=100; ,8 -n=7.8 25 4.40 s 0.03 ( 3 / 2 - , 5 / 2 - ) 90 93Ru01 D ,8 -=100; ,8-n=13.8 4 3.15 m 0.04 3/2 ( ) ) 90 95Ke04 J . 8 - = 100 15.15 m 0.12 3 / 2 - 90 , 8 - = 1 0 0 50.53 d 0.07 5/2 + 96 , 8 - =100

STA~LE l /2 - - 96 IS=100. 15.663 s 0.005 9/2 + 96 941t.A T IT=100 78.41 h 0.12 9/2 + 90 ,8+=100 4.18 m 0.01 1 / 2 - 90 IT=93.77 12; ,8+=6.23 12 1.9 h 0.2 (9/2 + ) 90 ,8+=100

1.18 h 0.10 ( 1 / 2 - - ) 90 13+=1(10 2.04 m 0.11 (9/2 + ) 90 /3+=100 190 ms 15 ( 1 / 2 - ) 90 IT=100 12.8 s 0.9 (9/2 + ) 91He04 TDJ .8+=100 12.9 s 0.8 ( 1 / 2 - ) 91He04 TDJ ,8+=100

> 150 ns 9 /2+# 92Ye04 T ,8+ ? > 1.5 gs 9 /2+# 95Le14 T ,8+ ?

*89Br T : ENSDF averages 8 values. Also 93Ru01-~.348(0.022)

90As

90Se --56430# 400# 90Br --64610 80 90Kr --74963 19 90 Rb -- 79355 8 90Rbm --79248 8 106.90 0.03 90Sr --85941.9 2.7 90y --86487.9 2.3 90ym --85805.9 2.3 682.03 0.06 90Zr --88767.9 2.2 90 Zr" --86448.9 2.2 2319.000 0.010 90Nb --82657 5

90 Nb" --82532 5 124.67 0.25 ~ N b " --82275 5 382.01 0.25 90Mo --80168 6 90Tc --71210 24(1 90To'" --70901 ,'3011 310 390 90Ru --65410# 400# 90Rh --532211# 5011#

> 150 ns 95Cz.A T , 8 - ? > 150 ns 0 + 94Be24 T , 8 - ?; , 8 - n ? 1.910 s 0.010 93 93Ru01 TD ,8 -=100; ,8-n=25.2 9 32.32 s 0.09 0 + 93 , 8 - =100

158 s 5 0 - 93 , 8 - =100 258 s 4 3 - 93 , 8 - -----97.4 4; IT=2.6 4

28.84 y 0.05 0 + 93 96Wo06 T , 8 - =100 64.10 h 0.08 2 - 93 , 8 - =100 3.19 h 0.01 7 + 93 IT~I00 ; .8---0.0018 2

STABLE 0 + 93 1S=51.45 3 809.2 ms 2.0 5 - 93 IT=100 14.60 h 0.05 8 + 93 ,8+=100 18.81 s 0.06 4 - 93 IT=100 6.19 ms 0.08 1 + 93 IT=100 5.56 h 0.09 0 + 96 ,8+=100

* 8.7 s 0.2 1 + 93 ,8+ =100 BD * 49.2 s 0.4 (8 + ) 93 93Ru03 J .8+=100

11 s 3 0 + 93 94-Zh26 T /3'+=100 > 150 ns 94He28 T ,81- ?

*90Br T : supel~sedes 80A115=1.92(0.02) from same group -90Sr T : average 96Wo06=28.79(0.06) 92Sc.B=28.78(0.04) 94Ma50=28.915(0.038) .90Tc m E : arguments are given in 93Ru03 for the (8+) level to be the ground-state *90Ru T : updates 91Zh29=13(5) from same authors

, , i (~


Nuclide Mass excess Excitation Half-life ./n Eas Reference Decay modes and intensities (keV) energy(keV) (%)

91 AS

91 Se --50890# 500#

91Br --61510 711

91Kr --71310 60

91Rb --77748 8

91Sr -- 83639 6

91y --86346.3 2.8

9lyre --85790.7 2.8 555.58

91Zr --87891.1 2.2

91Nb -- 86638 3

91Nbm --86534 3 104.49

91Mo --82204 11

91Mo m --81551 11 653.01

91Tc --75980 200

91Tcm --75800 220 180

91Ru - 6 8 5 8 0 500

91Rum --68180# 580# 400# 300#

91Rh --59100# 4(k')#

91Pd --47060# 600#

*91Tcm E : less than 350 keV, from ENSDF

0 . ~

0.09

0.09

100

> 150 ns 3 / 2 - # 95Cz.A T

270 ms 50 1/2 + # 90 541 ms 5 3 / 2 - # 90 93Ru01 D

8.57 s 0.04 5t2 (+1 90 95Ke04 J

58.4 s 0.4 3/2 ( -~ 90

9.63 h 0.05 5/2 + 90

58.51 d 0.06 1 / 2 - 90

49.71 m 0.04 9/2 ~ 90

STABLE 5/2 + 9~)

680 y 130 9/2 + 90 91Hi.A D

60.86 d 0.22 l / 2 - 90 91Hi.A D

15.49 m 0.01 9/2 + 90

65.0 s 0.7 1 / 2 - 90

3.14 m 0.02 (9 /2) + 90

3.3 m 0.1 ( 1 / 2 1 - 90 ABBW E

9 s 1 (9/2 + ) 9(I

7.6 s 0.8 ( 1 / 2 - ) 90

> 150 ns 9 / 2 - # 94He28 T

> 1.5 #s 9 /2~# 95Le14 T

/ 3 - ? /3-=100; /3-n=21 10

/3-=100; B - n=20 3

/3 - =100

/ 3 - =100

/ 3 - =100

/3-=10(I

IT>98.5; / 3 - <1.5

IS=I 1.22 4

e~, ~ 100; e +---0.0138 25

IT=93 4; ~=7 4; e+--0.0028 2

/3+=100

IT=50.1 12; /3+--49.9 12

/3+=100

/3+>99; IT<I

/3+=100

/3+~100; /3~-p=?; IT ? /3 + ?

/3~ ?

92 As

92Se --47200# 600#

92Br --56580 50

92Kr --68788 12

92Rb --74775 7

92Sr --82875 7

92y --84815 9

92Zr --88454.6 2.1

92 Nb -- 86449.0 2.7

92 Nbn' --86313.5 2.7 135.5

92 Mo -- 86805 4

92Tc --78935 26

92Ru --74410# 300#

92Rh --63360# 40(1#

92 Pd -- 55500# 50(1#

0.4

> t50 ns 95Cz.A T

> 1511 ns 0 + 95Cz.A T

343 ms 15 ( 2 - ) 92 93Ru01 D

1.840 s 0.008 0 + 94

4.492 s 0.020 0 - 94

2.71 h 0.01 0 + 92

3.54 h 0.01 2 - 95

STABLE 0 b 94

34.7 My 2.4 (7) + 94

10.15 d 0.02 (2) 4 94

STABLE >300Py 0 + 94 85No03 T

4.23 m 0.15 (8) + 94

3.65 m 0.05 0 + 94

> 150 ns 64# 94He28 T

> 15(I ns 0 + 94He28 T

• 92Mo T : T>I90 Ey (2 o') in post cut-off date 97Ba35

• 92Rh J : (6 + ) in post cut-off date 97Ka07

/ 3 - ?

/ 3 - ? /3-=100; / / - n=33.1 21

/3-=100; B - n=0.033 3

/3 -= I00 ; / 3 - n=0.0107 5

/3 -=100

~ - =100

IS=17.15 2

f14 ~--,100; /3-- <0.05

/3~=1~1 IS=14.84 4; 2/3 + ? /3+=100

/3+ =100 6 "~ ?

/3+ ?


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities ( keV ) energy(keV ) (%)

93 Se

93Br --53000# 300#

93 Kr -- 64030 100

93Rb --72626 8

935r --80088 8

93 y -- 84224 11

93ym --83465 11 758.721 0.021

93Zr --87117.4 2.1

93Nb --87208.7 2.2

93Nbm --87177.9 2.2 30.82 0.17

93 Mo -- 86804 4

93Mo m --84379 4 2424.89 0.03

93Tc --83603 4

93Tc m --83211 4 391.84 0.08

93Ru --77270 90

93Rum --76540 90 734.40 0.10

93Rh --69170# 400#

93pd --59700# 400#

*93Br D : symmetrized from / 3 - n = 1 0 ( + 5 - 3 ) %

.93Kr D : /3--n intensity is from 93Ru01 J : 1/2 + in post cut-off date ENSDF'97

*93Rb D : f l - -n=l .39(7)% in post cut-off date ENSDF'97

.93ym E : 758.719(0.021) in post cut-off date ENSDF'97

*93Ru n' D : . . . ; /3+1)--0.027 5 D : jff+p----0.010(2)% in ENSDF is not correct

*93Rh J : from 95Ro06

*93pd I : f l+p precursor with T--60(20): not trusted

> 150 as 1/2+# 95Cz.A T / 3 - ?

102 ms 10 3 / 2 - - # 93 88Kr10 TD /3-=100; / 3 - n = l l 4

1.286 s 0.010 1/2 TM 93 95Ke04 J

5.84 s 0.02 5/2-- 93

7.423 m 0.024 5/2 + 93

10.18 h 0.08 1 / 2 - 93

820 ms 40 7/2 + 93

1.53 My 0.10 5/2 + 93

STABLE 9/2 + 93

16.13 y 0.14 1/2-- 93

4.0 ky 0.8 5/2 + 93

6.85 h 0.07 21/2 + 93

2.75 h 0.05 9 /2 + 93

43.5 m 1.0 1 / 2 - 93

59.7 s 0.6 (9/2) + 93

10.8 s 0.3 ( I / 2 ) - 93 83Ay01 D

> 150 ns (9/2 + ) 94He28 T

3# s 9 /2+# 93

/3-=100; /3-n=1.95 11 *

fl-=lO0; f l - n = l . 3 5 7 *

/3- =1oo / 3 -=100

IT=I00 *

/3- =1oo 1S=100.

IT=I00

~=100

IT~I00 ; /3+---0.12 1

/3'+=100

IT=76.7 11; /3+=23.3 11

/:=1oo B+=78.0 23; IT=22.0 23; . . . * ~ ? * B + ? .

945e

948r --47800# 400#

94Kr --61140# 300#

94Rb --68551 9

945r --78842 7

94 y -- 82350 8

94Zr --87266.3 2.3

94Nb --86364,9 2.2

94NbnJ --86324.0 2.2 40.902 0.012

94Mo --88410.3 1.8

94Tc --84155 4

94Tcm --84080 4 75.5 1.9

9'lRu --82568 13

94Rh --72940# 450#

94Rhm --72640 400 300# 200#

94pd --66350# 400#

94Ag -- 53_'~0# 500#

94Agm --51950# 640# 1350# 400#

*94Ag J : as plgdicted by 945c35

> 150 ns 0 + 95Cz.A T

70 ms 20 92

200 ms 10 0 + 92

2.702 s 0.005 3 ~ - ) 92 93Ru01 D

75.3 s 0.2 0 + 92

18.7 m 0.1 2-- 92

STABLE >6Py 0 + 92 90Ba.A T

20.3 ky 1.6 (6) + 92

6.263 m 0.004 3 + 92

STABLE 0 + 92

293 m 1 7 + 92

52.0 m 1.0 (2) + 92

51.8 m 0.6 0 + 92

* 70.6 s 0.6 (2 + , 4 + ) 92 96.Io06 J

* 25.8 s 0.2 ( 8 + ) 92

9.0 s 0.5 0 + 92

1# s 0+#

420 ms 50 (9 + )

/ 3 - ? /3-=100;/3-n=30 10

/3-=100; /3-n=5.7 22

/3-=100; /3-n=10.01 23

/3- =1oo f l - = l O 0

IS=17.38 4; 2/3/-- ?

/3- =I00

IT=99.50 6; /3----0.50 6

15=9.25 3

/3+=100

/3+ ~, 100; IT<0.1

/3+=100

a~=lOO; a%=18 5 B+=lOO

/3+=1oo a+?

945c35 TJD /3+=100; /3+p=?

4 6 G, Audi et al. /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life j~r Ens Reference Decay modes and intensities (keV) energy(keV) (%)

95Br > 150 ns 3 / 2 - # 95Cz.A T /3 ?

95Kr --56040# 400# 780 ms 30 1/2 !+) 95 95Ke04 J / 3 - =100

95Rb --65839 19 377.5 ms 0.8 5 / 2 - 95 /3-=1/10; /3 n=8.73 20

~JSSr --75117 8 23.90 s 0.14 1/2 ~ 94 / 3 - = 100

95y --81204 8 10.3 m 0.1 1 / 2 - 94 /3 =10(1

95Zr --85657.6 2.3 64.02 d 0.(15 5/2 + 95 / 3 - =100

95Nb --86782.5 1.9 34.975 d 0.007 9/2 + 95 /3 - =100

95Nb'~ --86546.8 1.9 235,68 0.02 86.6 h 0.8 1 / 2 - 95 IT=94,4 6 ; / 3 - =5.6 6

95Mo --877118.1 1.8 STABLE 5/2 I- 95 IS=15.92 5

95Tc --86017 5 20.0 h 0.1 9/2 + 95 /3+=100

95Tc" --85978 5 38.89 0.05 61 d 2 1 / 2 - 95 /3+=96.12 32; IT=3,88 32

fJSRu --83450 12 1.643 h 0.014 5/2 + 94 /3~ =100

95Rh --78340 150 5.1/2 m 0.10 (9/2) + 94 /34 =100

"~SRhm --778~10 150 543.3 0.3 1.96 m 0.04 ( t / 2 ) 94 1T=88 5;/34 =I2 5

95pd --70150# 40(1# 10# s 9 /2+# 95 /3~ ?

95pdm --68280 3/00 1870# 500# 13.3 s 0.3 (21/2 + ) 95 /3+=?; IT=5#; /3+p---0.90 16

9SAg --60100# 400# 2.0 s 0.1 (9/2 + ) 94Sc35 TJD /31 =100; /3+p=?

*95pd T : 1.35(I).261 s in post cut-off date 97Sc.I, if the 1219.3 keV 7 originates from ground-state

*95pdm E : Q(/3 ~p)=4300(300) to 2644,85 level in 94Ru from figures in 82Ku15 and 82No06

*9SAg T : to be replaced by post cut-off date 97Sc.1=1.74(0.13), for/3t 7 activity, same authors

%Br > 150 ns 95Cz.A T f l - ?

96Kr --53030# 500# > 50 ms 0 ~ 95Ke04 T f l - ?

96Rb --61214 26 203 ms 3 24 95 93Ru01 D /3-=100; /3 n=13.4 4

96Rhm --61210# 200# 0# 200# > 1 ms 1 ( -#1 81Bo30 JT / 3 - ?; IT ?; f l - n ?

%Sr --72954 25 1.07 s 0.01 0 + 93 / 3 - = 100

%Y --78341 22 5.M s 0.05 0 - 93 / 3 - =100

%ym --77204 21 1140 30 BD 9.6 s 0.2 (8) + 93 / 3 - =l t l )

96Zr --85441 3 39 Ey 9 0 + 93 93Ka12 T 1S=2.80 2; 2 /3- =llg~

96Nb --85604 4 23.35 h 0.05 6 ~ 93 /3 - =1/~)

%Mo --88791./I 1.8 STABLE 0 + 93 IS=16.68 5

%To --85818 5 4.28 d 0.07 7 F 93 /3+=11.10

%Tc" --85784 5 34.28 0.(17 51.5 m 1.0 4 + 93 IT=98.0 5; /3+=2.0 5

96Ru --86(172 8 STABLE >67Py 0 + 93 85No03 T IS=5.52 6; 2/3 ~ ?

%Rh --79626 13 9.90 m 0.10 (6 + ) 93 /3+=10(I

%Rh" --79574 13 52.0 0.1 1.51 m 0.02 (3 + ) 93 IT--~) 5; /3~ =40 5

96pd --76180 150 122 s 2 0 + 93 /3+=100

t~6Ag --64570# 40)# 5.1 s 0.4 (8 ~ , 9 + ) 93 96He25 D /3+=10(I; /3+p=3.7 9

%Cd --561t)0# 500# 1# s 0 + /3+ ?

*%Rb T : ENSDF average of 8 values. See also 201(1) of 93Ru01

*96Rbm 1 : non-observation by 81Th04 is not in contradiction with 81Bo30 experiment

*%Rb" 1 : existence of this isomer is discussed in ENSDF

*%Zr T : observation of 2/3-- decay by 93Ka12 questionned by 96Ba37

*%Zr T : and 94Ar29 reports limit for single /3 - decay: T>38Ey (90% CL)

*C~6Ag T : post cut-off date 97Sc.1=4.50(0.06) s and discl'epant /3+p=l 1.9(2.6)%


Nuclide Mass excess Excitation Half-life frr Ens Reference Decay modes and intensities (keV) energy(keV) (%)

97Br > 150 ns 3 / 2 - # 95Cz.A T /3- ? 97Kr --47920# 500# > 150 ns 3/2+# 94Be24 T /3- ?; /3 -n ? 97Rb --58365 28 169.9 ms 0.7 3/2 + 93 93Ru01 D /3-=100; /3-n=25.7 8

97Sr --68792 19 429 ms 5 1/2 + 93 /3-=100; /3- n<0.05 97y --76260 12 3.75 s 0.03 ( 1 / 2 - ) 93 93Ru01 D /3-=100; /3-n=0.058 7 97ym --75592 12 667.51 0.23 1.17 s 0.03 (9/2) + 93 ,8->99.3; IT<0.7; /3-n<0.08 97yn --72737 12 3523.3 0.4 142 ms 8 ( 2 7 / 2 - ) 93 1T>80; /3- <20 97Zr --82949 3 16.90 h 0.05 1/2 + 93 ,8- =100

97Nb --85606.9 2.6 72.1 m 0.7 9/2 + 93 /3- =100 97Nb m --84863.5 2.6 743.35 0.03 52.7 s 1.8 1 /2 - 93 IT=I00 97Mo --87540.8 1.8 STABLE 5/2 + 93 IS=9.55 3 97Tc --87221 5 2.6 My 0.4 9/2 + 93 e=100 97Tcm --87124 5 96.56 0.06 90.1 d 1.0 1/2-- 93 IT~I00; ~<0.34 97Ru --86112 8 2.9 d 0.1 5/2 + 93 /3+=100 97Rh --82590 40 30.7 m 0.6 9/2 + 93 /3+=100 97Rh m --82330 40 258.85 0.17 46.2 m 1.6 1 /2 - 93 /3+=94.4 6; IT=5.6 6 97pd --77800 300 3.10 m 0.09 (5/2 + ) 93 /3+=100 97Ag --70790# 400# 25.3 s 0.3 (9/2 + ) 93 95Sc.A T /3+=100 97Cd --60600# 400# 2.8 s 0.6 9/2+# 93 95Sc.A T /3+=100; /3+p=?

99Kr > 150 ns 3/2+# 95Cz.A T /3- ? ~'X)Rb --50840 150 50.3 ms 0.7 (5/2 + ) 95 93Ru01 D /3-=100; /3--n=15.9 20 99Sr --62120 140 269 ms 1 3/2 + 95 /3-=100; /3-n=0.100 19 99y --702112 24 1.470 s 0.007 (5/2 +) 95 /3- =100; /3-n=1.9 4 99Zr --77769 20 2.1 s 0.1 (1/2 + ) 95 /3- =100 99Nb --82327 13 15.0 s 0.2 9/2 + 95 /3- =100 99Nbm --81962 13 365.29 0.14 2.6 m 0.2 1 /2 - 95 f l -=? ; 1T<3.8 99Mo --85966.1 1.8 65.94 h 0.01 1/2 + 95 /3-=100 99Tc --87323.3 1.9 211.1 ky 1.2 9/2 + 95 /3-=100 99Tcm --87180.6 1.9 142.6833 0.0011 6.01 h 0.01 1/2-- 95 IT~,I00; /3--=0.0037 6 99Ru --87617.0 2.0 STABLE 5/2 + 95 IS=12.7 1 99Rh --85574 7 16.1 d 0.2 1/2-- 95 /5'+=100 ~Rh m --85510 7 64.3 0.4 4.7 h 0.1 9/2 + 95 /3+~t00; IT<0.16 ~Pd --82188 15 21.4 m 0.2 (5/2) + 95 /3+=100 99Ag --76760 150 124 s 3 (9/2) + 95 /3+=100 99AgnS --762511 150 506.1 0.4 10.5 s 0.5 ( 1 / 2 - ) 95 IT=100 99Cd --69850# 210# 16 s 3 (5/2 +) 95 /3+=100; fl+p=0.21 8; /3+tr<le~- * 991n --60910# 500# > 150 ns 9/2+# 94Sc22 T /3+ ?

• 99Cd D : symmetrized from /3+1::.--0.17(+11-5)% **

98Kr > 150 ns 0 + 95Cz.A T 13- ? 98Rb --54300 30 114 ms 5 (1,0) (-#) 93 93Ru01 D fl-=100; /3--n=13.8 6; . . . *

~Rb m --53920 120 380 120 BD 96 ms 3 (4, 5) (+#1 93 fl--=100 98Sr --66629 26 653 ms 2 0 + 93 93Ru01 D fl-=100; /3-n--0.25 5 98y --72452 24 548 ms 2 ( 0 ) - 93 93Ru01 D /3-=100; /3-n=0.331 24 98y,,~ --72040 30 410 30 BD 2.0 s 0.2 (5 +) 93 94St31 J /3-=?; IT=10#; /3-n=3.4 10 98Zr --81276 20 30.7 s 0.4 0 + 93 /3- =100 98Nb --83526 6 2.86 s 0.06 1 + 93 /3- =100 98Nbn' --83442 7 84 4 51.3 m 0.4 (5 +) 93 /3 -~100; IT--0.1# 98Mo --88112.0 1.8 STABLE >100Ty 0 + 93 52Fr23 T 1S=24.13 7; 2/3- ? * 98Tc --86428 4 4.2 My 0.3 (6) + 93 /3- =100 98Ru --88224 6 STABLE 0 + 93 IS=1.88 6 98Rh --83167 12 * 8.7 m 0.2 (2) + 93 /3+=100 98Rh m --83110# 50# 60# 50# * 3.5 m 0.3 (5 +) 93 /3+=?; 1T ? 98pd --81300 21 17.7 m 0.3 0 + 93 /3+=100 9SAg --72880 150 46.7 s 0.9 (5 +) 93 96He25 D /3+=100; /3+p=0.0012 5 * 98Cd --67460# 210# 9.2 s 0.3 0 + 93 96He25 D /3+=100; /3+p<0.025 98In --53800# 500# > 1.5 /zs 95Le14 T /3+ ?

• 98Rb D : . . . ; /3-2n=0.051 7 ** • 98Rb T : Several other results reported in ENSDF. See also 109(1) of 93Ru01 ** • 98Mo T : limit given here is for 0v-2/3-- decay (theoretically faster, see text) ** • 9SAg D : symmetrized from /3+p=0.0011(+5~:~)% **


Nuclide Mass excess Excitation Half-life j,,r Ens Reference Decay modes and intensities (keV) energy(keV) (%)

100Kr > 150 ns 0 + 95Cz.A T

100Rb --46700# _'3(10# 51 ms 8 (3 + ) 90 93Ru01 D

100Sr --60220 130 202 ms 3 0 + 90 93Ru01 D

100y --67290 80 * 735 ms 7 1 - , 2 - 90 93Ru01 D

100ym --67090# 220# 200# 200# * 94(I ms 30 ( 3 , 4 , 5 ) (+#1 90

100Zr --76600 40 7.1 s 0.4 0 + 90

100Nh --79939 26 1.5 s 0.2 14 90

100Nbm --79471 28 470 40 BD 2.99 s 0.11 ( 4 + , 5 + ) 90

100Mo --86184 6 10.2 Ey 0.8 0 + 90 95Da37 T

100To --86016.4 2.2 15.8 s 0.1 1 + 90 93Ga09 D

100Ru --89218.8 2.0 STABLE 0 + 90

100Rh --85589 20 20.8 h 0.1 1 - 90

IOORhm -85481 20 107.6 0.2 4.6 m 0.2 (5 + ) 90

100pd --85227 11 3.63 d 0.09 0 + 90

100Ag --7818(I 80 2.01 m 0.09 (5) + 90

100Agm --78160 80 15.52 0.16 2.24 m 0.13 (2) + 90

l°°Cd --74310 100 49.1 s 0.5 0 + 90

l°°ln --64130 380 6.2 s 0.7 6+# 96 95Sz01 TD

100Sn --56860# 430# 1.1 s 0.4 0 + 95Fa.A TD

• 100Rb T : ENSDF average of 3 values. See also 53(2) of 85Pf.A J : from 95PRO4

• l°°Rb D : f l - 2 n intensity is derived from / 3 - 2 n / / 3 - n=0.027(7), in 81Jo.A

• 10°Sr D : /3--n=0.78(13)% in post cut-off date ENSDF'97

.100y D : /3--n---0.92(8)% in post cut-off date ENSDF'97

• 100Mo T : average 95Da37=9.5(0.9) 91Ej02=11.5(+3-2) and 9tEl04=11.6(+3.4-0.8)

• 100Mo T : and post cut-off date 97A102=7.6(+2.2-1.4) not used yet

• 100Mo T : 10.0(1.0) in post cut-off date ENSDF'97 with 97A102 included

• 100ln T : average 95Sz01=6.1(0.9) 95Fa.A=6.3(+I.04).9); 95Fa.A supersedes 95Sc33=7.8(8)

• 100Sn T : symmetrized from 0.94(+0.544).27) D : from /3+p//3+ <20%

• 100Sn T : results from 95Fa.A are now in post cut-off date 97Su06

/ 3 - ? /3-=100; /3-n=5.6 12:/3-2n--0.15 5

/3-=100; /3-n=0.98 23

]3-=100; /3-n=1.02 7

13- =100

/3- =100

/ 3 - =100

/ 3 - =100

IS--9.63 3; 2 3 - = l O 0

/ 3 - ~-,"~100; e=0.0018 9

IS=12.6 1

/3+=100

1T~98.3; /3+ ~ 1.7

e=100

fl + =100

/3+ =?; 1T ?

/3' =100

/3~- = 100; /3+ p>3.9

/3+=100; f l+p<17

101Rb --43600 170 32 ms 4 3 /2+# 94

101Sr --55410 120 118 ms 3 ( 5 / 2 - ) 94 95Lh04 J

101y --64910 100 426 ms 20 (5/2 ~-) 94 96Me09 T

101Zr --73460 30 2.1 s 0.3 (3/2 + ) 94

10lNb --78943 19 7.1 s 0.3 (5/2#) + 94

101Mo --83512 6 14.61 m 0.03 1/2 + 94

101Tc --86336 24 14.22 m 0.01 (9/2) + 94

101Ru -- 87949.6 2.0 STABLE 5/2 + 94

10lRh --87408 17 3.3 y 0.3 1 / 2 - 94

101Rhm --87251 17 157.32 0.04 4.34 d 0.01 9 /2 + 94

101pd --85428 18 8.47 h 0.06 (5/2 + ) 94

10lAg --81220 100 11.1 m 0.3 9 /2 + 94

101Agm --80950 100 274.1 0.3 3.10 s 0.10 1/2-- 94

101Cd -75750 150 1.2 m 0.2 (5/2 + ) 94

101In -68410# ~ 16 s 3 9 /2+# 94

101Sn --59560# 500# 3 s l 5 /2+# 95Ja16 TD

.101y T : average 96Md)9=400(20) 86Wa17-~40(20) and 83Wo10=500(50)

.101y T : 93Ru01=279(9) at variance, not used

,8-=100; /3-n=31 6

f l -=100 ; R-n=2.37 14

/3-=100; /3-n=1.94 18

R - =100

/3 -=100

3-=I00 /3 -=100

1S=17.0 l

e=100

~=93.6 2; IT--6.4 2

fl+ =100

/3+=100

IT= 100

/3+=100

/3+ =lO0; ~ -p=7

/3+=100; /~+ p=?


Nuclide Mass excess Excitation Half-life f r Ens Reference Decay modes and intensities (keV) energy(keV) (%)

102Rb --38000# 500# 37 ms 5 91 /3-=100; /3 -n=18 8 102Sr --53080 110 69 ms 6 0 + 91 93Ru01 D /3-=100; /3-n=5.5 15 102y --61890 90 * 300 ms 10 low 91 96Me09 D /3-=100; f l -n- -4 .9 11

102ym --61690# 220# 200# 200# * 360 ms 40 high 91 /3-=100; /3--n=6.0 17 102Zr --71740 50 2.9 s 0.2 0 + 91 /3-=100 102Nb --76350 40 1.3 s 0.2 1 + 91 /3-=100 102 Nb m --76220 50 120 50 BD 4.3 s 0.4 high 91 / 3 - =100 102Mo --83558 21 11.3 m 0.2 0 + 91 /3 -=100 102Tc --84568 9 * 5.28 s 0.15 1 + 91 /3 -=100 102Tc m --84548 13 20 10 * 4.35 m 0.07 (4 ,5 ) 91 fl----98 2; 1T=2 2 102Ru --89097.9 2.0 STABLE 0 + 91 IS=31.6 2 102Rh --86775 5 206.0 d 2.1 ( 1 - , 2 - ) 91 92Ta.A T //+=80 5; /3--=20 5 102Rhm --86634 5 140.75 0.08 3.76 y 0.10 6 (+) 91 92Ta.A T /3+~100; IT=0.23 3

102pd --87926 3 STABLE 0 + 91 IS=l.02 l; 2/3 + ? 102Ag --81970 70 12.9 m 0.3 5 + 91 /3+=100 102Agm --81960 70 9.3 0.4 7.7 m 0.5 2 + 91 /3+=51 5; rr--49 5 102Cd --79380 70 5.5 m 0.5 0 + 91 /3+=100 102In --70130 390 22 s l (6 + ) 91 95Sz01 TDJ /3+=100; /3+p=0.0093 13 102Sn --64750# 400# 4.6 s 1.4 0 + 91 95Fa.A TEl /3+=100; /3+p ?

. lO2y D : / 3 - n : average 96Me09=4.0(1.5)% ENSDF=6.0(I.7)% • 102Rh T : average 92Ta.A=206(3) 61Hi06=206(3)

103Sr --47550# 500# > 150 as 95Cz.A T / 3 - ? 103y --58740# 300# 224 ms 19 5 /2+# 96Me09 TD /3-=100; /3-n=8.3 3 103Zr --68370 110 1.3 s 0.1 ( 5 / 2 - ) 94 91Ho16 J / 3 -=100 103Nb --75320 70 1.5 s 0.2 (5/2 + ) 93 / 3 - =100 103Me --80850 60 67.5 s 1.5 (3/2 + ) 93 / 3 - =1130 103Te --84599 10 54.2 s 0.8 5/2 + 93 /3-=100 l°3Ru --87258.9 2.0 39.26 d 0.02 3/2 + 93 /3 - =100 103Rum --87020.7 2.1 238.2 0.7 1.69 ms 0.07 11/2-- 93 IT=100 103Rh --88022.3 2.8 STABLE 1/2-- 93 IS=100. 103Rh n' --87982.5 2.8 39.756 0.006 56.114 m 0.009 7/2 + 93 IT=100 103pd --87479.2 2.9 16.991 d 0.019 5/2 + 93 e=100 103Ag --84792 17 65.7 m 0.7 7/2 + 94 /3+=100 103 Agm --84658 17 134.44 0.04 5.7 s 0.3 1/2-- 94 l T : 100 103Cd --80650 15 7.3 m 0.1 5/2 + 93 87Bu01 J /3+=100 1031n --74600 25 65 s 7 (9/2) + 93 /3+=100 103Sn --66950# 300# 7 s 3 5 /2+# 93 /3+=100; /3+p=? 103Sh --55780# 500# > 1.5 us 5 /2+# 95Le14 T /3+ ?

. lO3y T : average 96Me09=230(20) 96Lh04=190(50)

104Sr --44400# 700# > 150 as 0 + 95Cz.A T f l - ? 104y --54540# 400# > 150 as 96 / 3 - ? l°4Zr --66340# 400# 1.2 s 0.3 0 + 94 / 3 - =100 l°4Nb --72230 110 * 4.9 s 0.3 (1 + ) 94 96Me09 TD /3-=100; /3--n=0.06 3 104Nbm --72010 100 220 120 BD * 920 ms 40 high 94 96Me09 D /3-=100; /3-n---0.05 3 104Mo --80330 60 60 s 2 0 + 94 /3 -=100 104Tc --82490 50 18.3 m 0.3 (3 + ) 96 /3 -=100 104Ru --88091 4 STABLE 0 + 94 IS=18.7 2; 2fl-- ? 104Rh --86950.0 2.8 42.3 s 0.4 1 + 96 /3-- ~,-':",100; /3+--0.45 10 104Rhm --86821.0 2.8 128.967 0.004 4.34 m 0.03 5 + 96 IT~,~,I00; /3-----0.13 1 104pd --89391 5 STABLE 0 + 96 IS=ll .14 8 104Ag --85112 6 69.2 m 1.0 5 + 96 /3+=100 104Agm --85105 6 6.9 0.4 33.5 m 2.0 2 + 96 /3+~100; 1T<0.07 104Cd --83976 10 57.7 m 1.0 0 + 96 /3+=100 1041n --76070 14(I 1.80 m 0.03 (5 + ) 96 87Eb02 J /3+=100 1041nm --75980 140 93.48 0.10 15.7 s 0.5 (3 + ) 96 rr=80; /5'+=20 l°4Sn - 7 1 5 5 0 150 20.8 s 0.5 0 + 96 /3+=100 104Sb --59350# 360# 470 ms 130 96 95Fa.A TD /3+=?; f l+p<7; p<7; a ?

• 104Nb T : average 96Me09=5.0(0.4) 7 6 A ~ . 8 ( 0 , 4 ) • 104Nb D : /3-n=0,71% of 83En03, at variance, not used • 104Sb T : symmetfized from 440(+150-110)



105Sr > 15(1 ns

105y --51150# 500# > 150 ns 105Zr --62360# 400# 6110 105N6 --70850 1011 2.95 105Mo --77_3411 70 35.6 105To --82290 60 7.6 l°SRu --85930 4 4.44 1°SRh --87847 5 35.36 1°SRh"S --87717 5 129.781 0.0114 45 105pd --88414 5 STABLE 10SAg --87058 11 41.29 105 Ag" --87043 11 25.465 0.012 7.23 105Cd --84330 11 55.5 1051n --79481 17 5.117

105In m --78807 17 674.1 (1.3 48 105Sn --73220 90 34 105 Sb -- 637811 150 1.12

95Cz.A T f l - ? 5 /2+# 94Be24 T /3 ?

ms 100 96Me09 TD /3-=100; /3 n ? s 0.06 15/21- ) 94 96Me09 D f l -=100 ; f l - n = l . 7 9

s 1.6 ( 5 / 2 - ) 93 f l -=10( ) m 0.1 ( 3 / 2 - ) 93 / 3 - =10() h 0.02 3/2 + 93 / 3 - =100 h 0.116 7/2 + 93 f l - =101) s 1 / 2 - 93 IT ?; / 3 - ?

5/2 ~ 93 IS=22.33 8 d 0.07 1 / 2 - 93 /3+=100 m 11.16 7/2 + 93 IT~1011; fl+--0.34 7 m 0.4 5/2 + 93 /3 ~ =100 m 0.07 9/2 ~ 93 87Eb02 J /3 + =1~) s 6 ( 1 / 2 ) - 93 IT=100 s l ( 5 / 2 ~ ) 93 95PfDl T /3+=1011;/3+p=? s 0.16 (5/2 + ) 94Ti03 JD /3+ ?; p ~ l ; /3+p ?

*105Rh m T : no error given; other value is 30s (see ENSDF: remeasurement recommended) *105Sn J : from 85De08 *105Sb T : from 95Fa.A, supersedes 95Sc28=1.30(0.15), preliminary from same group

1('~6 Y --46370# 700# 1G6Zr --597011# 500# 1°6Nb --66890# .300# 106Mo --76257 22 IOSTc --79777 14 106Ru --86324 8 106Rh --86364 8 106Rhm --86228 I1 136 12 BD 106pd --89905 5

l°6Ag --869411 5 106Agm --86850 5 89.66 0.07 106Cd --87134 6 1061n --80610 14 1061nm --80581 14 28.6 0.3 106Sn --77430 50 106Sb --66360# 310# m6Te --580311# 400#

*106Zr T : T>240 ns in post cut-off date 97So07 *106Nb T : average 96Me09=900(20) 83Sh06=1020150) *106Cd T : also 96Da25>0.26 Ey for same channel *106Sb T : from 95Le.B, Fig. 4, preliminary *I06Te T : average 94Pa11=60(+40-20) 81Sc17=601+30-10)

> 150 ns 95Cz.A T fl ? > IS0 ns 0 + 94Be24 T f l - ?

920 ms 40 2+# 94 96Me09 TD f l -=100 ; f l - n= 4 .5 3 8.73 s 0.12 0 + 94 95Jo02 T /3 =100 35.6 s 11.6 ( 1, 2) 94 /3 - =100

373.59 d 0.15 0 + 94 f l - =100 29.80 s 0.08 1 + 94 /3 =100

131 m 2 (6) + 94 /3 -=100 STABLE 0 t 94 IS=27.33 3

23.96 m 11.04 1 + 94 /3+=?; /3-- ~0 .5 8.28 d 0.02 6 + 94 /3+=100; IT<4.2e~6

STABLE >6.6Ey 0 + 94 96Ba46 T 1S=1.25 4; 2/3 + ? 6.2 m 0.1 7 '~ 94 /31-=100 5.2 m 0,1 (3 + ) 94 fl~=10(1 1.92 m 0.08 0 + 94 /3+=100 6@1 ms 200 (4 + ) 94 94Se01 J /3+=100 70 .us 20 0 + 94 94Pal I T a=100

107 y

107Zr --55090# 6011# 107Nb --64920# 400# 107Mo --72940 160 107To --79100 150 107Ru --83920 120 107Rh --86861 12 107pd --88372 6 107 Pdm --88157 6 214.9 0.5 10TAg --88405 6 107 Agm --88312 6 93.125 0.019 1°Tcd --86988 7 IO7 In -- 83562 13 107In m --82884 13 678.5 0.3 l°7Sn --785611 90 107S6 --70650# 30(1# 107Te --60510# 3iX)#

*107Zr T : T>240 ns in post cut-off date 97So07 *107Nb T : average 96Me09=300(30) 91Hi02=3001101 *107Sb T : value is now in post cut-off date 97Sh13

> 150 ns 5 /2+# 95Cz.A T /3 - ? > 150 ns 94Be24 T /3 - ?

.",~) ms 9 5 /2+# 94 96Me09 TD /3-=100; /3-n=6.0 15 3.5 s 0.5 94 /3 -=100

21.2 s 0.2 5 /2+# 96 /3 =100 3.75 m 0.05 (5/2) + 96 /3-=1011 21.7 m 0.4 7/2 ÷ 94 /3 -=100 6.5 My 0.3 5/2 + 96 /3-- =I t~

21.3 s 0.5 I 1/2-- 96 IT=I00 STABLE 1/2-- 96 1S=51.839 7

44.3 s 0.2 7/21 96 1T=I00 6.50 h 0.02 5/2 ~ 96 /3+ =10() 32.4 m 1).3 9/24 94 /3 ~ =100 50.4 s I).6 I/2 94 IT=100 2.90 m 0.05 (5/2 b ) 96 /3~ =100 4.6 s 11.8 (5/2 + ) 96 96Hu.A TD /3+=100 3.1 ms 0.1 5 /2+# 96 or=70 30; fl~=31) 30

G. Audi et a l . /Nuc lear Physics A 624 (1997) 1-124 51


108y

108Zr --51900# 700#

108Nh --60540# 500#

108Mo --71190# 200#

108Tc --75940 130

108Ru --83660 120

t08Rh --85020 l l 0

108 Rhm -- 850711 40 --60 110

108Pd --89522 4

108Ag --87604 6

1°8 Agm --87495 6 109.440 0.007

108Cd --89253 6

1081n --84100 40

108 in m -- 84070 40 29.75 0.05

108Sn --82000 40

108Sb --72510# 210#

108Te --65680 150

108I --52820# 360#

> 150 ns 95Cz, A T , 8 - ?

> 150 ns 0 + 95Cz.A T , 8 - ?

193 ms 17 (2 + ) 96Pe25 TJ ,8 -=100; , 8 - n--6.2 5 *

1.09 s 0.02 0 + 95 , 8 - = 100

5.17 s 0.07 (2 + ) 95 , 8 - =loo

4.55 m 0.05 0 + 94 ' 8 - =IOO

• & 16.8 s 0.5 1 + 94 ,8-=100 BD * & 6.0 m 0.3 (5 + ) 94 ,8-=100

STABLE 0 + 95 IS=26.46 9

2.37 m 0.01 1 e 95 ,8-=97.15 20; ,8+=2.85 20

418 y 21 6 + 95 ,8+=91.3 6; IT=8.7 6 *

STABLE >410Py 0 + 95 95Da.3 T IS=0.89 2; 2,8 + ?

58.0 m 1.2 7 + 94 '8+ =IOO

39.6 m 0.7 2 + 94 ,8+=100

10.30 m 0.08 0 + 95 ,8+=100 7.4 s 0.3 (4 + ) 95 95Ce01 J ,8+=100; ,8+p ?

2.1 s 0.1 0 + 95 85"I102 D ,8+=51 4; oz--49 4; . . .

36 ms 6 1+# 95 94Pa12 D a=?; '8+--9#; p< l

*108Nb T : average 96Me09=190(20) 96Pe25=2f10(30) from same group but obtained with

.108 Nb T : different methods D : ,8--n intensity is from 96Me09

*t08Agm T : discrepant results: 418(71 3101130) 127(21), see ENSDF

*108Sb T : average 96Hu.A=7.6(0.3) 76Ox01=7.0(0.5); 96Hu.A value now in tx~st cut-off date 97Sh13

*108Te D : . . . ; ,8+ p=2.4 10; ,8+a<0.065

.108I D : '8+=9%# estimated by 94Pa12 using theoretical ,8 + half-life ~,4OO ms

*g¢

109 Zr

109Nb --58100# 5(10#

109Mo --67250# 300#

109Tc --74870# 210#

I09Ru --80850 70

109Rh --85012 12

l°gPd --87604 4

109pdm --87415 4 188.990 0.010

t09Ag --88720 3

109 Agm --88632 3 88.0341 0.OOl 1

t09Cd --88505 4

109In --86485 6

1091nm --85835 6 650.1 0.3

109In" --84383 6 2101.8 0.2

109Sn --82636 10

l°9sb - 7 6 2 5 6 19

l°gTe --67570 70

t09I --57570 150

*109Te D : . . . ; ,8+p--9.4 31; ,8+a<0.OO5

.1091 D : from 94Pal l

> 150 ns 95Cz.A T , 8 - ?

190 ms 30 5 /2+# 96 96Me09 TD /3-=100; ,8--n=31 5

530 ms 60 94 ' 8 - =100

870 ms 40 5 /2+# 94 96Me09 D '8 -=100; '8--n---0.08 2

34.5 s 1.0 (5/2 + ) 96

80 s 2 7 /2 + 94

13.7012 h 0.0024 5/2 + 94

4.696 m 0.003 1 1 / 2 - 94

STABLE 1/2-- 94

39.6 s 0.2 7/2 + 94

462.6 d 0.4 5/2 + 96

4.2 h 0.1 9/2 + 96

1.34 m 0.07 1 / 2 - 96

209 ms 6 (19/2 + ) 96

18.0 m 0.2 5/2 (+) 96

17.0 s (1.7 (5/2 + ) 96

O - = 1 0 0

, a - = t 0 0

, 8 - = 100

1T=I0(I

IS-~8.161 7

IT=IOO

e=loo

/3+=100

IT=loo

IT=loo

fl+ = l oo ,8+=IOO

4.6 s 0.3 (5/2 + ) 96 85"1102 D /3+=?; a=3.9 13; . . .

IOO ,us 5 (5/2 + ) 96 87Gi02 J p,~ 100; a<0 .5

J : from 95Pa01


Nuclide Mass excess Excitation Half-life ./or Ens Reference Decay modes and intensities (keV) energy(keV) (%)

II0Zr > 150 ns 0 + 95Cz.A T / 3 - ?

l l°Nb --53390# 600# 170 ms 20 2+# 96Me09 TD ,6-=100; / 3 - n - ~ 0 8

ll0Mo --65460# 400# 300 ms 40 0 + 94Lh02 T /3 =100; / 3 - n ?

IIOTc --71360# 400# 920 ms 30 (2 + ) 93 94Lh02 J /3-=100; /3-n=0.04 2

IIORu --80140 230 14.6 s 1.0 0 + 93 /3 -=100

IIORh --82950 220 * 3.2 s 0.2 I v 93 /3 -=100

tl0Rhm --82950 100 0 200 BD * 28.5 s 1.5 (> 3) 93 /3 -=100

ll0pd --88350 11 STABLE >600Py 0 + 93 52Wi26 T IS=11.72 9; 2 /3- ?

l l0Ag --87458 3 24.6 s 0.2 l + 93 / 3 - ~100; e--0.30 6

II0Agm --87340 3 117.59 0.05 249.76 d 0.20 6 + 93 /3-=98.64 6; r r=l .36 6

I I°cd -90349 .7 3.0 STABLE 0 ~ 93 IS= 12.49 12

ll01n --86472 12 4.9 h 0.1 7 + 93 /3+=100

I101n m --86411) 12 62.08 0.04 69.1 m 0.5 2 + 93 89Kr12 E /3+=I(X)

II0Sn --85835 16 4.11 h 0.10 0 + 93 e=100

l l0sb --77540# 200# 23.11 s 0.4 3 + 93 /3+=100

I10Te --72280 51) 18.6 s 0.8 0 t 93 /3v ~ 100; a~0 .003

ll01 --60350# 310# 650 ms 20 1+# 93 /3+=83 4; at=IT 4; /3+p=ll 3; . . .

I I0xe --51720# 400# 600# ms 0 + 93 /3+ ?; a ?

• l l0Tc D : / 3 - n intensity is from 96Me09

• l l0sb J : arguments for ./Tr_~+ are given in post cut-off date 97La13

• 1101 D : . . . ; /3+ot=l.l 3

IIIN6 > 150 ns 5/2~'# 95Cz.A T f l - ?

l l l M o --61000# 500# > 150 ns 94Be24 T 13-- ?

IIIT¢ --69820# 400# 290 ms 20 5 /2+# 96 96Me09 TD /3-=100; /3--n--0.85 211

IIIRu --76790# 31~# 2.12 s 0.07 (5/2 + ) 96 96Lh.B J /3 -=100

l l lRh --82290# 2111# 11 s 1 (7/2 + ) 96 /3--=1110

I I I P d - - 861130 40 23.4 m 0.2 5/2 + 96 /3-- =100

Illpdm -85860 40 172.18 0.08 5.5 h 0.1 1 1 / 2 - 96 IT=73 3; /3--=27 3

IIIAg --88217 3 7.45 d 0.01 1 / 2 - 96 /3 -=100

IllAgm --88157 3 59.82 0.04 64.8 s 0.8 7/2 + 96 IT=99.3 2; /3--=0.7 2

I l l c d -89254 .2 3.0 STABLE 1/2 + 96 IS=12.80 8

I l lcdm --88858 3 396.2t4 0.021 48.54 m 0.05 11/2-- 96 1T=100

l l l l n --88389 5 2.8047 d 0.0005 9 /2 ; 96 6=100

llllnm --87852 5 536.95 0.06 7.7 m 0.2 1 / 2 - 96 IT=I0(I

l l lSn --85944 7 35.3 m 0.6 7/2 ~ 96 /3+=11111

I r i sh --80840# 200# 75 s 1 (5/2 + ) 96 /3+=100

l l lTe --73480 70 19.3 s 0.4 5 /2+# 96 /3+=1110; /3+p=?

l t l l --64950# 300# 2.5 s 0.2 5 /2+# 96 /3+~100; ot=0.088

l l l X e --54370# 300# 740 ms 200 5 /2+# 96 94Pal l D /3+ ?; a=10 7

I I I Xe" non existent EU 900 ms 200 90Tu.A T

, l i t Mo T : T>240 ns in post cut-off date 97So07

* l l l T c T : supersedes 88Pe13=300(30) from same group

* I I I x e D : symmetrized from a=8(+8-5 )%

* l l l xe m I : from assigning a decay to isomer in older version of ENSDF

* : , g

G. Audi et al. /Nuclear Physics A 624 (1997) 1-124 5 3

Nuclide Mass excess Excitation Half-life J~ Em Reference Decay modes and intensities (keV) eucrgy(keV ) (%)

ll2Nb > 150 ns 2+# 95Cz.A T ,8-- ?

l l2Mo --58830# 600# > 150 es 0 + 94Be24 T /3-- ?

l l2Tc --65910# 500# 230 ms 20 2+# 97 96Me09 "I 'D ,8--=100; ,8--n=2.6 5

112Ru --75870# 540# 1.75 s 0.07 0 + 97 fl--=100

ll2Rh --79540# 500# * 2.1 s 0.3 1 + 97 ,8--=100

ll2Rhm --79340# 520# 200# 150# * 6.8 s 0.2 > 3 97 fl--=100

l t2pd --86337 18 21.03 h 0.05 0 + 97 f l - = 1 0 0

112Ag --86625 17 3.130 h 0.009 2 ( - ) 97 , 8 - = 100

112Cd --90581.0 2.8 STABLE 0 + 97 IS=24.13 14

l121n --87995 5 14.97 m 0.10 1 + 97 /3+=56 3; ,8----44 3

1121nm --87838 5 156.59 0.05 20.56 m 0.06 4 + 97 IT=100

l l2Sn --88659 4 STABLE 0 + 97 IS=0.97 1; 2g~- ?

l l2sb --81604 23 51.4 s 1.0 3 + 97 /3+=100

112Te --77260 170 2.0 m 0.2 0 + 97 ,8+=100

1121 --67100# 210# 3.42 s 0.11 1+# 97 78Ro19 D f l+~100; t*=0.0012; . . .

II2Xc --59930 150 2.7 s 0.8 0 + 97 94Pal l D fl+.~100; o/--0.9 8

II2Cs --46270# 300# 500 p,s 100 1+# 97 p=?; a ?

• 1121 D : . . . ; fl+p--0.88 10; fl+a=O.104 12

• 112I D : ,8+p and fl+o, are derived from f l+p/a=735(80) fl+p/fl+a=8.5(2), in 85Ti02

• l l2Xe D : a intensity is estimated from 94Pa11=0.8(+1.14).5)% and 78Ro19=0.84%

II3N b > 150 m 5 /2+# 95Cz, A T , 8 - ?

l l3Mo --54000# 600# > 150 ns 94Be24 T , 8 - ?

l l3Tc --63970# 600# 130 ms 50 5 /2+# 94 , 8 - = 100

II3Ru --72150# 500# 800 ms 50 94 , 8 - = 100

l l3Rh --78790# 400# 2.80 s 0.12 (7/2 + ) 94 93Pel l TJ , 8 - = 100 *

l l3pd --83690 40 93 s 5 (5/2) + 94 , 8 - = 100

ll3pdn' --83610 40 81.1 0.3 300 ms 100 ( 9 / 2 - ) 94 93Pel l T lT=100

ll3pdn non existent RN > 100 s 94 81Mel7 1 IT ? *

113Ag --87033 17 5.37 h 0.05 1 / 2 - 94 ,8 -=100

ll3Agm --86990 17 43.50 0.10 68.7 s 1.6 7 /2 + 94 IT=64 7; , 8 - = 3 6 7

l l 3 c d --89049.9 2.8 7.7 Py 0.3 1/2 + 94 96Dal l T IS=12.22 8; , 8 - = 100

ll3cdm --88786.3 2.8 263.59 0.12 14.1 y 0.5 1 1 / 2 - 94 f l - ~ 1 0 0 ; IT=0.14

l13In --89366 3 STABLE 9/2 + 94 IS=4.29 2

1131n m --88974 3 391.691 0.008 1.6582 h 0.0006 1 / 2 - 94 IT=I00

l l3Sn --88330 4 115.09 d 0.04 1/2 + 94 ,8+=100

ll3Snm --88253 4 77.389 0.019 21.4 m 0.4 7/2 + 94 IT=91.1 23; fl+=8.9 23

l l3sb --84414 22 6.67 m 0.07 5/2 + 94 ,8+=100

ll3Te --78310# 200# 1.7 m 0.2 (7/2 + ) 94 ,8+=100

113I --71120 50 6.6 s 0.2 5/2 + 94 ,8+=100; a=3.31e-7; f l + a ?

l l3Xe --62050 90 2.74 s 0.08 5 /2+# 94 85'I]02 D ,8+~,100; ot~0.011 5; ,8+p=7 4; . . . *

l l3Cs --51660 150 17 ,us 2 (5/2 + ) 94 94Pa12 T p,~.100; j6'+~0.03 *

• l l3Rh T : supersedes 88Pe13=2.72(0.22) from same group **

• ll3pd" 1 : existence is not possible since discovery of 113pdra by 93Pel l **

• l l3Xe D : . . . ; ,8+ ot~,.~0.007 4 **

• l l3Xe D : ot--0.0024-0.0204% from estimated limit for the reduced width, see 85"1102 **

• l l3Xe D : f l+p and ~ff~-a derived from ,8+p/a=605(35) and fl+p/fl+ct=500-1500 in 85Ti02 **

• l l3Cs J : fi'om 87Gi02 **

54 G, Audi et al./Nuclear Physics A 624 (1997) 1-124


114Me > 150 ns 0 ÷ 95Cz.A T , 8 - ?

II4Tc --59730# 600# > 150 as 2~# 94Be24 T , 8 - ?

I14Ru --70790# 360# 530 ms 60 0 + 95 ,8 -=100; , 8 - n ?

ll4Rh --75590# 300# * 1.85 s 0.05 1 + 95 ,8 -=100; , 8 - n ?

ll4Rhm --75390# 340# 200# 150# * 1.85 s 0.05 ( > 3) 95 , 8 - = 100

ll4pd --83494 25 2.42 m 0.06 0 + 95 , 8 - =100

ll4Ag --84945 26 4.6 s 0.1 1 + 95 , 8 - =100

114Agm --84746 26 198.9 0.5 1.50 ms 0.05 ( < 7 ~) 95 IT=I00

114Cd --90021.3 2.8 STABLE >92Py 0 + 95 95Da.3 T IS=28.73 28; 2 ,8- ?

1141n --88569 3 71.9 s 0.1 1 + 95 ,8---99.50 15; ,8+=0.50 15

ll4lnm --88379 3 190.29 0.03 49.51 d 0.01 5 + 95 IT=96.75 24; ,8+=3.25 24

1141n# --88067 3 501.93 0.03 43.1 ms 0.6 8-- 95 1T=I00

l l4sn --90558 3 STABLE 0 + 95 IS=0.65 l

114Sb --84680 200 3.49 m 0.03 3 + 95 ,8+=100

ll4Te --81920# 200# 15.2 m 0.7 0 + 96 ,8+=1011

1141 --72800# 300# 2.1 s 0.2 1 + 96 fl+=100; ,8+p ?

1141m --72530# 300# 265.9 0.5 6.2 s (7) 96 ,8+=9l 2; IT=9 2

114Xc --66930# 210# 10.0 s 0.4 0 + 95 ,8+=100

114Cs --54570# 310# 570 ms 20 (1 + ) 95 96He25 D ,8+~100; a--0.018 6; . . .

114Ba --45701)# 450# 500 ms 230 01 95 95Ja.A TD ,8+=?; a<0.37; ,8+p=?; . . .

• l l4Tc T : T>2ddl ns in post cut-off date 97So07

• l l 4cd T : > 7 Ey, given in ENSDF, is for 0p-2,8-- decay alone

• 1141m D : ENSDF'95 ",8+<100; IT<10ft ' m-evaluated for NUBASE by J. Blachot, based on

• l141m D : 1141 IT decay, see ENSDF

• II4Cs D : . . . ; ,8~ p=8.7 13; ,8+o,--0.19 3

• II4Cs D : ,8+p intensity is from 96He25; ,8+a derived from ,8+p/fl+a-~5.5(12) in 85Ti02

• l l4Ba D : . . . ; 12C<0.038 D : a and 12C intensities are from 95Gu10

• l l4Ba T : symmetrized from 440(+250-150)

g~,9

l15Mo > 150 ns 95Cz.A T f l - ?

115Tc --57490# 71)0# > 150 ns 5 /2+# 94Be24 T fl ?

l l5Ru --66780# 600# 740 ms 80 94 92Ay02 T f l - = 100 ; , 0 - n ?

llSRh --74400 500 991/ ms 50 (7/2 + ) 94 ,B-=100

l l5pd --80400 6(1 25 s 2 (5/2 + ) 94 ,8-- =100

115pdm --811310 60 89.3 0.2 50 s 3 111 /2 - ) 94 , 8 -=92 .0 20; IT=8.0 20

llSAg --84990 30 20.0 m 0.5 1/2-- 92 , 8 - =100

115Agm --84950 30 41.10 I).20 18.0 s 0.7 7/2 + 92 ,8--=79.0 3; IT=21.0 3

115Cd --880911.9 2.8 53.46 h 0.10 1/2 + 96 ,8 =100

115Cd m --87909.9 2.8 181.0 0.5 44.6 d 0.3 1 1 / 2 - 96 , 8 - = 100

115In --89537 4 44l Ty 25 9/2 + 94 IS--95.71 2; , 8 - = 100

1151nm --89201 4 336.24 0.03 4.486 h 0.004 1 / 2 - 94 IT=95.0 7; , 8 - = 5 .0 7

115Sn --901132.6 3.0 STABLE 1/2 + 96 IS--0.34 1

llSsb --87003 20 32.1 m 0.3 5/2 + 96 ,81=101/

115Te --82360 110 * 5.8 m 0.2 7/2 + 96 ,8+=100

ll5Te m --823511 110 10 7 * 6.7 m 0.4 11/21 + 96 ABBW E ,8+~,~100; IT ?

1151 --76460# 470# 1.3 m 0.2 (5/2 ~ ) 96 ,8~=1011

115Xe --684311# 240# 18 s 4 (5/2 + ) 94 ,8+=100; ,8+p--0.34 6; ,8+a=0.0003 1

115Cs --59670# 430# 1.4 s :0.8 9 / 2 + # 94 ,sv=100; ,8~p~0.07

l lSBa --48710# 600# 400 ms 200 5 /2+# 95Gu01 TD ,8~=100; ,8+p=?

• ll5Tem E : less than 20 keV, from ENSDF


Nuclide Mass excess Excitation Half-life f r Ens Reference Decay modes and intensities (keV) energy(keV ) ( % )

II6Tc > 150 ns 95Cz.A T / 3 - ?

lt6Ru --65060# 700# > 150 ns 0 + 94Be24 T / 3 - ?

l l6Rh --71060# 500# * 680 ms 60 11- 95 fl-=lO0; fl-n ? l l6Rh m --70860# 520# 200# 150# * 900 ms 400 ( 5 , 6 , 7 ) 95 , 8 - = 100

l l6pd --79960 60 11.8 s 0.4 0 ÷ 96 /3 -=100

116Ag --82570 50 2.68 m 0.10 ( 2 ) - 95 /3 -=100

ll6Agm --82490 50 81.90 0.20 8.6 s 0.3 (5 + ) 95 /3--=94.0 15; IT=6.0 15

l l 6 c d - 8 8 7 2 0 3 34 Ey 3 0 + 95 94Ku25 T IS=7.49 12; 2 /3 -=100

1161a --88250 4 t4.10 s 0.03 1 + 95 / 3 - ~ 1 0 0 ; ~<0.06#

ll61nm --88123 4 127.267 0.006 54.29 m 0.17 5 + 95 /3 -=100

116In n --87960 4 289.660 0.006 2.18 s 0.04 8 - 95 IT=I00

116Srl --91524.7 3.0 STABLE 0 + 95 IS= 14.54 11

l l6sb --86818 6 15.8 m 0.8 3 + 95 /3+=100

ll6sbm --86430 40 380 40 BD 60.3 m 0.6 8 - 95 /3+=100 ll6Te --85310 90 2.49 h 0.04 0 + 96 /3+=100

116I --77560 140 2.91 s 0.15 1 + 96 /3+=100

l l6xe --72900# 250# 59 s 2 0 + 95 /3+=1(10

l l6Cs --62490 350 * 700 ms 40 (1 + ) 95 B+=I00; /3+p=0.28 7; /3+ot--0.049 25

ll6Csm --62390# 360# 100# 60# * 3.85 s 0.13 > 4 + 95 /3+=100; /~+p---0.51 15; /3+ot--0.008 2

l l6Ba --54330# 500# 1.35 s 0.15 0 + 95Ja.A TD /3+=100; /3+p=?

• l l6Ru T : T>240 ns in post cut-off date 97So07

• l l 6 c d T : average 94Ku25=26(+9-5) 95Da09=27(+5-4; + 9 ~ ) 96Ar.1=37.5(3.5 statistics + 2.0 systematics)

• t i6Ba T : supersedes 95Gu01=300(200) ms from same group

117Tc > 150 es 5 /2+#

l l7Ru --60740# 800# > 150 ns 96

llTRh --69540# 600# 440 ms 40 (7/2 + ) 96

l l7pd --76530# 300# 4.3 s 0.3 (5/2 + ) 96

llTpdm --76330# 300# 203.2 0.3 19.1 ms 0.7 ( 1 1 / 2 - ) 96

11TAg --82270 50 73.6 s 1.4 ( 1 / 2 - ) 96

117Agm--82240 50 28.60 0,20 5.34 s 0.05 (7/2 + ) 96

117Cd --86426 3 2.49 h 0.04 1/2 + 96

117Cd m --8621Y0 3 136.4 1).2 3.36 h 0.05 ( 1 1 / 2 ) - 96

117In --88943 6 43.2 m 0.3 9/2 + 96

1171n m --88628 6 315.302 0.012 116.2 m 0.3 1 j 2 - 96

llTSn --90398.0 2.9 STABLE 1/2 + 96

llTSnm --90083.4 2.9 314.58 0.04 13.60 d 0.04 1 1 / 2 - 96

l lTsb --88641 9 2.80 h 0.01 5/2 + 96

UTTe --85107 19 62 m 2 1/2 + 96

117Tern --84791 22 316 12 103 ms 3 1 1 / 2 - 96

1171 --80441) 70 2.22 m 0.04 (5/2) + 96

ll7Xe --73990 180 61 s 2 5/2 f+} 96

117 Cs -- 66470 50 * 8.4 s 0.6 9/2 + # 96

llTCs m --66320# 110# 150# 100# * 6.5 s 0.4 3 /2+# 96

l l7Ba --56950# 650# 1.75 s 0.07 (3/2) (+#) 96

l l7La --46570# 890# 500# ms 1 1 / 2 - #

.117Ru T : T>240 ns in post cut-off date 97So07

• l l7Ag T : symmetrized from 72.8(+2.04).7)

• ll7Te m E : probably decays by unobserved low-energy M2 to 296.0 level, from ENSDF;

• ll7T•m E : half-life suggests an energy below 40 keV, thus 296.0 + 20(12)

• l lTBa D : and /3+p///+ a=350-1200

95Cz.A T 13-?

3-? 3-=I00

3-=100

IT=f00

3- =I00

~---94.0 15; 1T=6.0 t5

~3- =100

~3- =100

8 - =100

8----52.9 15; IT-----~7.1 15

IS=7.68 7

IT=100

B + =100

,8+=100

1T=I00

/3+=100

3+=100; /3+p=0.0029 6

3+=100

,8+=100

/3 + = 100; B + p=?; B + or=7

B ~ ? ; p ?

56 G. Audi et at/Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay moaes and intensities (keV) energy(keV ) (%)

H8Tc

II8Ru --58660# 900#

ll8Rh --65740# 700#

llSpd --75470 210

llSAg --79570 60

118Agm --79440 60 127.49 0.05

HScd --86709 21)

llSln --87230 8

llSIn m --87130# 50# 100# 50#

llSlnn --86990# 50# 241)# 50#

t18Sn --91653.1 2.9

118Sb --87996 4

118Sb m --87746 6 250 6 BD

llSTe --87723 16

1181 --80690 80

l181m --8050(/ 80 190,1 1.0

118Xe --77710 1000

118Cs --68414 13 *

118Csm --68310# 60# 100# 60# *

l l8Ba --62000# 500#

118La --49770# 800#

• 118Rh T : T>240 us in post cut-off date 97So07

• 1181u" E : i38.2(0.5) keV above lt81n m, from ENSDF

• IISCs D : . . . ; ,8+tr<0.0024 4

• l lSfsm D : . . . ; ,8+a<0.0024 4

> 150 ns 95Cz.A T

> 150 ns 0 + 94Be24 T

> 150 ns 94Be24 T

1.9 s 0.1 0 ÷ 95

3.76 s 0.15 1-- 95 93Ja03 J

2.0 s 0.2 4 I+) 95 95Ap.A E

50.3 m 0.2 0 + 95

5.0 s 0.5 1 + 95

4,364 m 0.007 5 + 95 94It.A T

8.5 s 0,3 8 - 95

STABLE 0 + 95

3.6 m 0.1 1 + 95

5.00 h 0.02 8 - 95

6.00 d 0.02 0 + 95

13.7 m 0.5 2 - 95

8.5 m 0.5 ( 7 - ) 95 94Ka39 E

3.8 m 0.9 0 + 95

14 s 2 2 95

17 s 3 ( 7 - ) 95 93Be46 J

5.2 s 0.2 0 +

l# s

/ 3 - ?

B - 7 / t - ? •

B - =100

`8 -=100

/ 3 - =59; IT=41

, 8 - =100

/ 3 - =100

`8-=100

IT=98.6 3; `8- =1.4 3 *

IS=24.22 11

`8+=100

,8+=100

~=100

,8~ =100

,8+ ~ 100; IT ?

,8+ =10o

,8+=100; `8+p<0.042 6; ... *

`8+=100; `8+p<0.042 6; ... *

95Ja.A TD /3+=100; ,8+p ?

119Ru

llgRh --63940# 800#

l lgpd --72020# 300#

l l9Ag --78560 90

ll9Agm --78540# 90# 20# 20#

l l9cd --83910 80

119Cdm --83760 80 146.54 0.11

l19In --87704 8

llglnm --87393 8 311.37 0.03

ll9Sn --90067.2 2.8

l l9sn m --89977.7 2.8 89.531 0.013

l lgsb --89473 8

119Sb m --86632 8 2841.1 0.6

H9Te --87180 8

119Tenl --86919 8 260.96 0.05

1191 - 83670 60

l lgxe - 7 8 6 6 0 120

119Cs --72311 14

119Csm --72260# 30# 50# 30#

l l9Ba --64220 1020

ll9La --54970# 700#

ll9Ce --440(}0# 900#

> 150 ns

> 150 ns 7 /2+#

920 ms 130 93

* & 6.0 s 0.5 ( 1 / 2 - ) 94

* & 2.1 s 0.1 (7 /2 + ) 94

2.69 m 0.02 3/2 + 93

2.20 m 0.02 ( 1 l / 2 - ) 93

2.4 m 0.1 9/2 + 93

18.0 m 0.3 1 / 2 - 93

STABLE 1/2 + 93

293.1 d 0.7 11/2 - 93

38.19 h 0.22 5/2 + 93

850 ms 90 (25/2 + ) 93

16.03 h 0.05 1/2 + 93

4.70 d 0.04 11/2 - 93

19.1 m 0.4 5/2 + 93

95Cz.A T

94Be24 T

5.8 m 0.3 5/2 t+l 93 90Ne.A J

43.0 s 0.2 9/2 + 93 75Ho09 D

30.4 s 0.1 3/2 (+1 93

5.4 s 0.3 (5/2 + ) 93

2# s 11/2--#

200# ms 5/2 + #

* l lgAg" E : estimated from 7/2 + level in isotopes 113Ag=43(0) 115Ag--41(0) l t7Ag=28(0)

`8-? p-?

/3-=100

fl-=100

,8-=100

,8- =I00

,8- =I00

,8- =I00

,8-=94.4 15; IT=5.6 15

IS=8.58 4

IT=I00

e=100

IT=I00

fl+ =100

,8~ ~ 1~0; IT<0.008

/~+=100

/3+=100

/3+ =100; ,8+ ot<2e-6

B+=I00

,8 + =100; ,8 + p=? /3 ~ ?

,8+ ?



120Ru

120Rh --59820# 800#

12°pd --70770# 400#

12°Ag --75650 70

t20Agm --75450 70 203 1

120Cd --83973 19

120In --85730 40

120 Inn' --85670 70 70 60

120In" --85430# 200# 300# 200#

120Sn --91103.3 2.5

120Sb --88423 8

120Sb m --88420# 100# 0# 100#

120Te --89405 10

12°1 --83790 18

t20lm --8,M-70 150 320 150 BD * 53 m 4 ( 7 - ) 88 95Ka17 J

12°Xe --81830 40 40 m 1 0 + 88

120Cs --73888 10 * 61.2 s 1.8 2 ( - # ) 94 93A103 T

120Csm --73790# 60# 100# 60# * 57 s 6 7 - # 94 75Ho09 D ,8+=100; ,8+ct<2.0e-5 4; ,8+p<7e41 3

120Ba --68890 ~ 24 s 2 0 + 88 92Xu04 T ,8+=100

120La --57690# 600# 2.8 s 0.2 88 ,8+=100; ,8+p=?

120Ce --49710# 800# 250# ms 0 + ,8+ ?

• 120Cs T : average 93A103=60(21 77Ge03=64(3)

• 120Cs D : isomers not distinguished by 75Ho09 in ,8+or and ,8+p. Values replaced

• 120Cs D : by upper limits for both (cf. ENSDF evaluation of I Igcs)

> 150 ns 0 + 95Cz.A T f l - ?

> 150 ns 94Be24 T / 3 - ?

500 ms 100 0 + 93Ja03 T , 8 - = 100

1.23 s 0.03 3 + 88 93Ru01 D ,8-=100; ,8 -n<0 .003

320 ms 40 6 - 88 ,8-- ~63; IT-~,~37

50.80 s 0.21 0 + 88 ,8 -=100

* 3.08 s 0.08 1 + 88 , 8 - = 100

* 46.2 s 0.8 5 + 88 87Eb02 J , 8 - = 100

* 47.3 s 0.5 8 ( - ) 88 79Fo10 J , 8 - = 100

STABLE 0 + 88 IS=32.59 10

* 15.89 m 0.04 1 + 88 ,8+=100

* 5.76 d 0.02 8 - 88 ,8+=100

STABLE 0 + 88 IS=0.096 2; 2,8 + ?

* 81.0 m 0.6 2 - 88 /3+=100

/3 + =100

3+ =100

,8+=100; ,8+a<2.0e-5 4; ,8+p<7e~6 3 *

121Rh --57680# 900#

121pd --66900# 500#

121Ag --74660 150

121Cd --81(160 80

121Cdm --80850 80 214.89 0.10

121 In -- 85838 27

1211n m --85524 27 313.69 0.10

12tSn --89202.8 2.5

121Sn m --89196.5 2.5 6.3(I 0.08

121Sb --89592.9 2.3

121Te --88557 25

121Te m --88263 25 293.98 0.03

1211 --86288 11

121Xc -- 82543 24

121Cs --77143 14

121Csm --77075 14 68.5 0.3

121Ba --70340 300

12lLa --62400# 500#

12ICe --52470# 700#

121pr --41580# 800#

*121pd T : T>240 ns in pest cut-off date eJ'/So07

> 150 ns 7 /2+# 94Be24 T , 8 - ?

> 150 ns 94Be24 T 3 - ?

780 ms I0 (7/2 + ) 91 93Ru01 D 3 - = 1 0 0 ; fl--n--0.076 5

13.5 s 0.3 (3/2 + ) 91 /3 -=100

8.3 s 0.8 ( 1 1 / 2 - ) 91 , 8 - = 100

23.1 s 0.6 9 /2 + 91 f l - =100

3.88 m 0.10 1 / 2 - 91 f l -=98 .8 2; IT=l.2 2

27.06 h 0.04 3/2 + 91 f l - =100

55 y 5 l l / 2 - 91 IT=77.6 20; f l - = 2 2 . 4 20

STABLE 5/2 + 91 IS=57.21 5

19.40 d 0.10 1/2 + 96 94Si.A T fl+=100

154 d 7 1 1 / 2 - 96

2.12 h 0.01 5/2 + 91

40.1 m 2.0 5/2 (+) 91

155 s 4 3/2 (+) 91

122 s 3 9/2 (+1 91

29.7 s 1.5 5/2 (+1 96

5.3 s 0.2 11 /2- -# 92

1# s 5 /2+#

IT=88.6 11; /3+=11.4 11

,8+=100

fl+=100

3+=100

//+=83; 1T=I7

3+=1oo; 3+r~-o.o2 1

,8+=100; fl+p ?

,8+ ? 600 ms 300 ( 3 / 2 - ) 91 90Bo39 TJD p=?; ,8+ ?; ,8+p ?

*121Te T : difference with 73Ka45=16.78(0.35) is remarkable

*t21Ce D : ,8+p~,-~1% and T=I.I(0.1) s in post cut-off date 97Li19

*121pr T : T=1.4(0.8) s in ENSDF: not trusted to belong to this nuclide

5 8 G. Audi et al, /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life J'~ Ens Reference Decay modes and intensities (keV) energy(keV) (%)

122Rh

122pd --65390# 500#

122Ag --71430# 210#

122Agm --71350# 220# 80# 50#

122Cd --811570# 210#

t221n --83580 50

1221nm --83540# 80# 40# 60#

1221n" --83290 130 290 140 BD

I22Sn --89944.9 2.7

122Sb -88328 .5 2.2

122Sb'n --88164.9 2.2 163.5591 0.0017

122Te --90311.1 1.9

1221 --86077 5

122Xe --85190 90

122Cs --78132 16

122Csm --780.)9 10 123 19 MD

122Csn --78005 16 127.0 0.5

122Ba --74280# 300#

122La --64540# 500#

122Cc --57740# 600#

122pr --45040# 800#

*122pd T : T>240 ns in post cut-off date 97So07

*122Ag D : /3-- n intensity is from 93Ru01

*122Cs T : average 93A103=21.210.2) 69Chl8=21.010.71

*122Cs D : /3+or intensity upper limit is from 75Ho09

50# ms

> 150 ns (1;- 94Be24 T

* 520 ms 14 (3 + ) 94 95Fe12 T

* 1.5 s 0 .5 8 # 94

5.24 s 0.03 0 i 94

* 1.5 s 0.3 1 t 94

* 10.3 s 0.6 5;- 94

10.8 s 11.4 8 94

STABLE 0 q 94

2.7238 d 0.0002 2 - 94

4.191 m 0.003 ( 8 ) - 94

STABLE 0 h 94

3.63 m 0.06 I + 94

2(I. 1 h 0. I 0 + 94

21.18 s 0.19 1 + 96 93A103 T

3.70 m 0.11 8 - 96

360 ms 20 (5) - 96

1.95 m 0.15 0 ~ 94

8.7 s 0.7 94

2# s 04 94

500# ms

*122Ce I : T=8.7(0.7) s in NDS 71 (1994) was misprint for 122La. Corrected in ENSDF

/ 3 - '?

/ 3 - 7 *

/ 3 - =100; /3-n--0.186 10 *

/3-=100; / 3 - n ?

/3 =1013

/ 3 - = 100

/ 3 - = 103

/ 3 - =l(xl

IS=4.63 3; 2 /3- ?

/3----97.59 12; ,8+=2.41 12

IT : I00

1S=2.603 4

/3t =100

6=100

/3+ = 100; /3+ cr<2e-7 *

/3+=100

IT=I00

/3+=100

/3+ = 100; 13 ; p=?

/3+ ?; ,8+p ? *

/3+ ?

t23pd --61240# 600#

t23Ag --69960# 300#

123Cd --773111 41)

123Cd m --769911 40 316.52 0.23

123In --83426 24

123In m --83099 24 327.21 0.04

123Sn --87819.5 2.7

123Snm --87794.9 2.7 24.6 0.4

J23Sb --89222.5 2.0

123Tc --89169.2 1.8

123Te m --88921.6 1.8 247.55 0.04

1231 - - 87935 4

123 X e - - 85259 15

123Cs --81049 12

123Csm --80892 12 156.74 0.21

t23Ba --75590# 300#

123La --68710# 40(0

123Ce --60070# 500#

123pr --503411# 700#

,~123Ag T : average 95Fe12=293(7) 86Ma42=300(20) 83Re05=300(10)

*123Te T : and 24(9) Ey for e(K) , same authors

* 123Te 1 : This nuclide is not considered 'stable' since K • has been obsecved

*123Cs T : average 93AI03=5.87(0.05) 68Ch18=5.87(0.05)

> 150 ns 94Be24 T / 3 - ?

296 ms 6 (7/2 + ) 94 95Fe12 T /3-=100; f l -n=0 .55 5

2.10 s 0.02 (3/2) + 94 / 3 - =100

1.82 s 0.03 ( 1 1 / 2 - ) 94 , 8 - =?; IT=?

5.98 s 0.06 9/2 + 94 / 3 - =100

47.8 s 0.5 1 / 2 - 94 /3 - =100

129.2 d 0.4 1 1 / 2 - 94 , 8 - = 100

40.06 m 0.01 3/24 94 , 8 - =100

STABLE 7/2 + 94 1S--~2.79 5

> 600 Ty 1/2 + 94 96A130 T IS=0.908 2; e=100

119.7 d 0.1 1 1 / 2 - 94 IT=I00

13.27 h 0.08 5/2 + 94 /3+=100

2.118 h 0.02 1/2 + 94 90Ne.A J ,8+=100

5.87 m 0.04 1/2 + 94 93A103 T / l+=lif0

1.64 s 0.12 111 /21- 94 1T= 100

2.7 m 0.4 5/2 ;- 94 /3 + = 100

17 s 3 1 1 / 2 - # 94 /31 =100

3.8 s 0.2 (5/2) (+#1 94 /3+=100; /3t p=?

800# ms 3 /2+# /3+ ?

D : fi'om 93Ru01


Nuclide Mass excess Excitation Half-life ,W Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

124pd 200# ms 0 + / 8 - ?

124Ag --66570# 400# 172 ms 5 3+# 95Fe12 T .8--=100; /8 -n>0 .1

12~Agm --66570# 410# 0# 100# 8- -# 95Kr.A I /8-- ?; IT ?

124Cd --76710 60 900 ms 200 0 + 85 /8 -=100

124In --80880 50 * 3.17 s 0.05 3 + 85 /8--=100

12A'Inm --80900 50 --20 70 BD * 2.4 s 0.4 8 ( - # ) 85 79FOI0 J / 8 - ~ 1 0 0 ; 1T ?

124Sn --88236.1 1.4 STABLE >100Py 0 + 85 52Ka41 T IS=5.79 5; 2 /8- ?

124Sb --87618.6 2.0 60.20 d 0.03 3 - 85 /8 - =100

124Sbm --87607.7 2.0 10.8633 0.0011 93 s 5 5 + 85 IT=75 5 ; / 8 - = 2 5 5

124Sb" -87581 .8 2.0 36.8456 0.0015 20.2 m 0,2 8 - 85 IT=f00

124Te --90523.1 1.5 STABLE 0 + 85 IS--4.816 6

124I --87363.5 2.4 4.1760 d 0.0003 2 - 85 92Wo03 T /8+=100

124Xe --87657.5 2.0 STABLE >48Py 0 + 96 89Ba22 T IS=0.10 1; 2/8 + ?

124Cs -81743 12 30.9 s 0.4 1 + 85 93A103 T /8+=100

124Csn~ --81280 12 462.6 0.5 6.3 s 0.2 (7) + 85 IT=100

I24Ba --79095 14 11.9 m 1.0 0 + 85 /8+=100

124La --70300# 300# * 29 s l ( 7 - , 8 - ) 85 92Id01 JT /8+=100

124Lain --70200# 320# 100# 100# * 2# s low 92Id01 J IT ?

124Ce --64720# 500# 6 s 2 0 + 85 /8+=100

12Apr --53130# 600# 1.2 s 0.2 86Wi15 TD /8+=100; /8+p=?

• 124Ag D : /8--n intensity limit is from 93Ru01

*124Agm I : '"l~aere is some evidence for a low-spin and a high-spin isomer in 124Ag"

* 124Cd T : 1.25(0.02) s in post cut-off date ENSDF'97

-1241n T : 3.11(0.10) s in post cut-off date ENSDF'97

*t241nn' T : 3.7(0.2) s in post cut-off date ENSDF'97

*l~Sbm E : 10.8630(0.0011) in post cut-off date ENSDF'97

*124Sb" E : 36.8440(0.0014) and J ~ = ( 8 ) - in post cut-off date ENSDF'97

*124Cs T : average 93A103=30.9(0.5) 78Ek05=30.8(0.5)

*124Csm E : 462.55(0.17) in posi cut-off date ENSDF'97

*124Ba T : 11.0(0.5) s in post cut-off date ENSDF'97

J g *

Walt

12SAg --64700# 400# 166 ms 7

125Cd --73360 70 * 650 ms 20

125Cdm --73310 50 50 70 BD * 570 ms 90

1251n --80480 30 2.36 s 0.04

125 Inn' --80120 30 360.12 0.09 12.2 s 0.2

125Sn --85897.8 1.5 9.64 d 0.03

125Sn m --85870.3 1.5 27.50 0.14 9.52 m 0.05

125Sb --88261.1 2.8 2.7582 y 0.0011

IL~Te --89027.8 1.9 STABLE

125Te m --88883.0 1.9 144.795 0.010 57.40 d 0.15

1251 --88842.0 1.9 59.408 d 0.008

125Xe --87189.5 2.0 16.9 h 0.2

125Xe m --86936.7 2.0 252.8 0.3 57 s 1

1ZSCs --84091 8 45 m 1

125Ba --79530 250 3.5 m 0.4

12SEa --73900# 300# 76 s 6

125Ce --66570# 400# 9.0 s 0.6

125pr --57910# 500# 3.3 s 0.7

7/2+# 95Fe12 "I'D /8-=100; /8-n=? (3/2) + 94 /8--=100

(11/2-) 94 8-=100

9/2 ¢+~ 94 fl-=100

I/2 (-) 94 /8- =I00

11/2- 94 /8--=I00

3/2 + 94 fl-- =lO0

7/2 + 94 / 8 - =100

1/2 + 94 1S=7.139 6

1 1 / 2 - 94 1T=100

5/2 + 94 e=100

I/2 + 94 90Ne.A J /8+=100 9 / 2 - 94 90Ne.A J IT=I00

I /2 (+) 94 81Th06 J /8+=100

1/2 (+) 94 /8+=100

( 1 1 / 2 - - ) 94 /8+=100

(5/2 + ) 94 83Ni05 D /8+=100; /~-p=?

3/2+# 95Os03 TD /8+=100; ~+p ?


Nuclide Mass excess Excitation Half-life frr Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

126Ag --61010# 400# 107 ms 12 3+# 95Fe12 TD /3-=100; / 3 -n=?

126Cd - 7 2 3 3 0 50 506 ms 15 0 + 93 /3 - =100

1261n --77810 40 * 1.60 s 0.10 3 (+) 93 /3-- =100

1261nm --77710 50 l(g) 60 BD * 1.64 s 0.05 8 ( - # ) 93 79Fo10 J / 3 - =100

I~Sn --86020 11 207 ky 2l 0 + 93 96Ha45 T / 3 - = 100

126Sb --86400 30 12.46 d 0.03 ( 8 ) - 93 / 3 - =100

126Sb" --86380 30 17.7 0.3 19.15 m 0.08 (5) + 93 / 3 - = 8 6 4; IT=I4 4

126Sb n --86360 30 40.4 0.3 11 s ( 3 ) - 93 11"--100

126Te --90070.3 1.9 STABLE 0 + 93 IS=18.952 11

1261 --87915 4 13.11 d 0.05 2 - 93 /3+=56.3 20; /3---43.7 20

126Xe --89173 6 STABLE 0 + 93 IS=0.09 1; 2/3 + ?

126Cs --84M9 12 1.64 m 0.02 1 ~ 93 /3+=100

126Ba --82676 14 100 m 2 0 + 93 3+=100

126La --75110# 300# 54 s 2 94 /3+=100

126Ce --707110# 400# 50 s 3 0 + 93 /3 ~ =100

126pr --6026(1# 500# 3.12 s 0.18 (> 5) 93 88Ba42 TJ /3"+=100;/3:p=?

t26Nd --53030# 700# 1# s 0 + /3+ ?

* 126Sn T : half-life has been determined from isotopic abundance 0.000923(87)%

*126pr T : average 95Os03=3.14(0.22) 88Ba42=3.0(0.4) and 83Ni05=3.2(0.6)

127Ag --58800# 500#

127Cd --68530 70

127In --76990 40

127In m - 7 6 5 3 0 70 460 70 BD

127Sn -83508 25

127 Snm -83503 25 4.7 0.3

127Sb -86709 6

127Te --88290 3

127 Tem --88202 3 88.26 0.118

127I --88987 4

127Xe --88325 4

127xem --88028 4 297.10 0.08

127Cs --86240 9

127Ba --82790 100

127 Barn --82710 100 80.33 0.12

127La --78100# 220#

127La m --78090# 220# 14.8 1.2

127Ce --71960# 300# *

127Cem --71960# 320# 0# 100# *

127pr --64430# 400#

127 N d - - 55420# 600#

• 127Ag T : supel~edes 95Fe12=109(251 from same group

79 ms 3 7/2 + #

370 ms 70 (3/2 + ) 96

1.09 s 0.01 9 /2 (+) 96 87Eb02 J

3.67 s 0.04 ( 1 / 2 - ) 96

2.10 h 0.04 (11 / 2 - - ) 96

4.13 m 0.03 (3/2 + ) 96

3.85 d 0.05 7/2 + 96

9.35 h 0.07 3/2 + 96

109 d 2 11/2 - 96

STABLE 5/2 + 96

36.4 d 0.1 1/2 + 96

69.2 s 0.9 9 / 2 - 96

6.25 h 0.10 1/2 + 96

12.7 m 0.4 1/2 + 96

1.9 s 0.2 7/2 - 96

5.1 m 0.1 ( 1 1 / 2 - ) 96

3.7 m 0.4 (3/2 + ) 96

29 s 2 (5/2 + ) 96 96Ge07 T

M s 2 (1/2 + )

4.9 s 0.3 3/2 + # 96

1.8 s 0 . 4 5 / 2 + # 96

96Wo.A TD f l - = 100 ; f l - n = ?

/ 3 - = 100

/ 3 - =100; / 3 - n~0.03

/3-=100; / 3 - n---0.69 4

/ 3 - =lOO

/ 3 - =IOO

/3--=100

/3--=100

IT=97.6 2; /3-- =2.4 2

IS=100.

e=100

IT=I00

/3+=100

/3+=100

IT=I00

/3+=100

/3+ ~ 100; f f ?

/3+ =100

96Ge07 TID /3+ =100

/3+=100

//+=100; /3+ p=?


Nuclide Mass excess Excitation Half-life J~ Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

128Ag

128Cd --67290 290 128In --74360 50 128In m --74040 50 320 60 BD 128Sn --83336 27 ,:. 128 Snm --81245 27 2091.48 0.12 / 128Sb --84610 25 * 128Sbm --84600 24 10 7 *

128Te --88993.6 1.8 t281 --87742 4

128Xe --89860.8 1.4 128Cs --85932 6 128Ba --85410 11 128La --78760 400 * 128Lam --78660# 410# 100# 100# * 128Ce --75570# 300# 128pr --66320# 400# 128Nd --60180# 600# 128pm --48200# 900# 800# ms

• 128Te T : see also 92Be3~)=7.7(0.4) not used for consistency with I30Te (set? below) • 128Te D : from 92Be30 • 128Cs T : average 93AI03=3.66(0.02) 76He04=3.62(0.02) • 128La T : and 5.4(0.2) m in post cut-off date 97Ha30 • 128Lam T : half-life shorter than 2 m, , f f = ( l + , 2 + ) in post cut-off date 97Ha30 • 128Ce T : to be replaced by post cut-off date 97Ha30--4.1(0.3) m, from same authors • 128pr T : average 88Ba42=3.1(0.3) 85Wi07=3.2(+0.54).4) D : from 85Wi07 • 128Nd T : 83Ni05 gave 4(2) s. Proved, by 85Wi07, to be due to t28pr, not to 128Nd

58 ms 5 96Wo.A TD /3-=100; / 3 -n=? ms 30 0 + 84 86(3ol0 T 13-=100

776 ms 24 (2, 3) + 84 93Ru01 TD 13-=100; 13-n=0.038 3 776 ms 24 (7, 8 ) - 84 93Ru01 T /3 -=100 59.1 m 0.5 0 + 84 13- =100 6.5 s 0.5 ( 7 - ) 84 IT= 100

9.01 h 0.03 8 - 84 13-=100 10.4 m 0.2 5 + 84 95Au04 E 13- --96.4; IT=3.6 2.2 Yy 0.3 0 + 84 96Ta04 T IS=31.687 l l ; 213-=100

24.99 m 0.02 l + 84 13-=93.1 8; 13+=6.9 8 STABLE 0 + 84 1S=I.91 3

3.640 m 0,014 1 + 84 93A103 T 13+=100 2.43 d 0.05 0 + 84 e=100 5.0 ra 0.3 (5 + ) 84 95Ha16 J fl+=100 1# m low 95Ha16 J IT ?

4.07 m 0.12 0 + 84 92Ha.C T /5"+=100 3.15 s 0.25 (4 ,5) 88Ba42 TJ /3+=100; fl+p=? 5# s 0 + 84 83Ni05 T fl+ ?; 13+p ?

93Li40 D fl+ ?; p=:0

129Ag

129Cd --63100# 400# 1291n --72980 130 1291nm --72600 140 380 70 BD 129Sn --80630 120 129 Snnt --80590 120 35.2 0.3 129Sb --84626 21 129 Sbm --82775 21 1851.05 0.10 129Te --87006 3 129Tem --86901 3 t05.50 0.05 1291 --88504 3 129Xe --88697.4 0.8 129Xe m --88461.3 0.8 236.14 0.05 129Cs --87501 5 129Ba --85070 11 129Barn --85062 11 8.42 0.06 129La --81350 50 129La m --81180 50 172.1 0.4 129Ce --76300# 210# 129 Pr --69990# 300# 129prm --69910# 310# 80# 80# t29Nd --62170# 360# t29pm --52950# 800#

50# ms 7 /2+# 95Fe12 ID 13-=100; 13-n=? 270 ms 40 3 /2+# 96 86(3o10 D 13-=100; 13--n ? 611 ms 4 9 /2+# 96 93Ru01 T 1.23 s 0.03 1 / 2 - # 96 2.23 m 0.04 3 /2+# 96 6.9 m 0.1 1 1 / 2 - # 96

4.40 h 0.01 7/2 + 96 17.7 m 0.1 ( 1 9 / 2 - ) 96 69.6 m 0.3 3/2 + 96 33.6 d 0.1 1 1 / 2 - 96 15.7 My 0.4 7/2 + 96

STABLE 1/2 + 96 8.88 d 0.02 1 1 / 2 - 96

32.06 h 0.06 1/2 + 96 2.23 h 0.11 1/2 + 96 2.16 h 0.02 7 /2+# 96 11.6 m 0.2 3/2 + 96 560 ms 50 11/2 -- 96

13-=100; fl--n---0.25 5 13- ~,d00; IT<0.3; 13- n=2.5 5 13-=100 B - ~100; ITs0 .002 O - M 0 0 ,8 -=85; IT=I5 /3 - =1130

IT--63 17; 13-=37 17 13-- =100 1S=26.4 6 IT=100 13 4. =100 13+=100 13+ ~ 100; IT=? 13+=100 IT=I00

3.5 m 0.3 (5/2 + ) 96 93A103 T /3+=100 * & 30 s 4 (3/2 + ) 96 96Gi08 J /3+=100 * & 11/2- -# ffl- ?

4.9 s 0.2 5 /2+# 96 /3'+=100; 13+p=? 1# s 5 /2+# B + ?

*129Ag I : observed, by 95Fe12, with low statistics in f l - n decay *1291a T : average 93Ru01=611(5) 86Wa17=610(10) *129Ce J : from 96Gi08 (5/2 + in ENSDF was from theory) *129prm E : estimated from 1 1 / 2 - level in isotolaes 131pr=152(0) 133pr=167(0) 135pr=358(0) *129prm E : 382,7 j~ r= (11 /2 - ) in post cut-off date 97Gi.2

* : I t

31t~

3 k *


Nuclide Mass excess Excitation Half-life j~r Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

130Cd - 6 1 5 0 0 # 400# 200 ms 4(I 0 + 90

130In --70000 50 * 278 ms 3 1 - 90 85Re.A T 1301nm --69950 50 50 50 BD * 538 ms 5 ( 1 0 - ) 90 93Ru01 TD 130Inn --69600 60 400 60 BD 550 ms 10 (5 -~ ) 90 93Ru01 D 13°Sn -80246 29 3.72 m 0.04 0 + 90 130Sn" --78299 29 1946.88 0.10 1.7 m 0A ( 7 - ) 90 130Sb --82394 25 39.5 m 0.8 ( 8 - ) 90 130Sbm --82389 25 5.10 0.20 6.3 m 0.2 (5) + 90 94Wa.A E

130Te --87352.9 1.9 790 Zy 100 0 + 90 96Ta04 TD 1301 --86933 3 12.36 h 0.03 5 + 90 1301m --86893 3 39.9525 0.01.113 9.0 m 0.1 2 + 90 130Xe --89881.8 0.9 STABLE 0 + 94 130Cs --86903 8 29.21 m 0.04 1 + 90 130Cs m --8674(1 8 163.25 0.11 3.46 m 0.06 5 - 90 130Ba --87271 7 STABLE 0 + 94

130Ba'n --84796 7 2475.12 0.18 8.8 ms 0.2 8 - 94 94Br15 T 130La --81670# 210# 8.7 m 0.1 3 I+) 96 130Ce --79460# 610# 22.9 m 0.5 0 ~ 94 96Xu04 T 130pr --71370# ~ 40.0 s 0.4 (6 ,7 ) 94 88Ba42 J 130pr'n --71370# 300# 2+# 88Ba42 J 130Nd --66340# 500# 28 s 3 0 + 90 130pm --55470# 700# 2.3 s 0.5 90 85Wi07 T 130Sm --47850# 900# 5000 ms 0 ¢

• I301n D : / 3 - n intensity is from 93Ru01 • 130lnn' T : average 93Ru01=542(9) 85Re.A=532(6) and 86Wa17=550(10) • 1301nm T : 76Lu02=580(10) at variance, not used • 130Te T : see also numerous (not used) results in 95Tr07 • 130prm J : there is also a low-spin component in 130pr activity • 130pm T : symmetrized from 2.2(+0.641.41

/3--=100; ,8-- n ~ 4 /3--=1(10; '8--n=l.Ol 22 '8--=100; '8--n=1.65 18 '8--=100; '8--n=1.65 18 ' 8 - =1oo /3-=1oo , 8 - = 100 , 8 - = 100 1S=33.799 10; 2 /3 -=100 , 8 - = 100 1"1"--84 2; , 8 - = 1 6 2 1S=4.1 1

,8 ~ =98.4; ,8--=1.6 1T~-~,I00; ,8+--0.16 2 IS=0.106 2; 2/3 + ? IT=I00

,8+ =100 ,8+=100 ,8+ =100

,8+ =100 ,8+=100; ,8+ p=?

,8+ ?

J31Cd 180# ms 7 / 2 - # 1311n --68220 80 280 ms 30 (9/2 + ) 94 93RuOl D 131Inn' --67860 80 350 40 BD 350 ms 50 ( 1 / 2 - - ) 94

131in,, --64120 100 4100 80 BD 320 ms 60 (19/2 +_23/2 + ) 94 131Sn --77390 70 56.0 s 0.5 (3/2 + ) 94 131Snm --77150 70 241.8 0.8 58.4 s 0.5 ( 1 1 / 2 - ) 94 131Sb --82020 70 23.03 m 0.04 (7/2 + ) 94 13tTe --85211.3 2.0 25.0 m 0.1 3/2 + 94 131Tern --85029.1 2.0 182.250 0.020 ~ h 2 1 1 / 2 - 94 t31I --87444.8 1.1 8.02(170 d 0.00011 7/2 + 94 131Xe --88415.6 1.0 STABLE 3/2 + 94 131Xem --88251.7 1.0 t63.930 0.008 11.84 d 0.07 11/2-- 94 131Cs -88063 5 9.689 d 0.016 5/2 + 94 131Ba --86693 7 11.50 d 0.06 1/2 + 94 131Ba'n --86506 7 187.14 0.12 14.6 m 0.2 9 / 2 - 94 131La --83730 100 59 m 2 3/2 + 94 13ICe --79710 410 i0.2 m 0.3 (7/2 + ) 96 131Cem--79650 410 6t.8 0.1 5.0 m 1.0 (1/2 + ) 96 96Gi08 E 131pr --74460 440 1.50 m 0.03 (3/2 + ) 94 96Gi08 T 131pfm --74310 44(I 152.4 0.2 5.7 s 0.2 ( 1 1 / 2 - ) 94 96Ge12 ED 131Nd --67900 460 33 s 3 (5/2) (+#) 94 96Ge12 T 131pm --59800# 600# 4# s 5 /2+# 94 131Sm --50400# 900# 1.2 s 0.2 5 /2+# 94

*131Inm D : . . . ; 1T<0.018

*131pr T : average 96Gi08=1.57(0.07) 93A103=1.48(0.02) and 83Ga.A=l.58(0.05)

' 8 - ? /3-=100; ' 8 -n=2 .2 3 ' 8 - ~100; ' 8 - n < 2 . 0 4; . . . * / 3 - > 9 9 ; f l - n=0.028 5; IT<I .8--=100 fl--=100; IT<0.000401 13 /3 -=100 ' 8 - = 1 0 0 /3---77.8 16; 1T=22.2 16 ' 8 - =I00 IS=21.2 4 IT=I00 e=100 /3+=100 IT=100 ,8+=100 '8+=100 '8+=100 ,8 + =100 . IT---96.4 12; ,8+=3.6 12 '8+=100; '8+ p=?

'8+ ?; '8+p ? ,8+=100; ,8+ p=?


Nuclide Mass excess Excitation Half-life fir Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

132In --62490 70 206 ms 4 ( 7 - ) 92 93Ru01 TD ,8-=100; ,8-n=5.2 12 *

t32Sn --76621 26 39.7 s 0.5 0 + 92 ,8-=100

132Sb --79724 23 2.79 m 0.05 (4 +) 92 ,8-=100

132Sbm --79520 40 200 30 4.15 m 0.05 ( 8 - ) 92 89St06 E ,8-=100

132Te --85210 11 3.204 d 0.013 0 ÷ 92 ,8-=100

1321 --85703 11 2.295 h 0.013 4 + 92 ,8-=100

132Im --85595 10 108 15 BD 1.387 h 0.015 ( 8 - ) 92 IT-~6 2; ,8-=14 2

132Xe --89279.5 1.1 STABLE 0 + 92 IS=26.9 5

132Xe m --86527.2 1.1 2752.27 0.17 8.39 ms 0.11 (10 +) 92 IT=I00 132Cs --87160 3 6.479 d 0.007 2 + 92 ,8+---98.13 9; 8--=1.87 9

132Ba --88440 3 STABLE 0 + 94 IS=0.101 3; 2/T F ?

132La --83730 40 4.8 h 0.2 2 - 94 /T~ =100

132Lain --83540 40 188.18 0.11 24.3 m 0.5 6 - 94 IT=76; /5+=24

132Ce --82450# 200# 3.51 h 0.11 0 + 96 fl~ =100

132Cem --80110# 200# 2340.8 0.5 13 ms 1 ( 8 - , 9 - ) 96 IT=I00 132pr --75340# 200# * 1.49 m 0.11 (2 +) 94 94Bu18 JT ,8+=100 *

132p1~' --75340# 220# 0# 100# * (5 + ) 90Ko25 J ,8+ ?

t32Nd --71610# 300# 1.56 m 0.10 0 + 94 95Bull T ,8+=100 *

132pm --61710# 500# 6.3 s 0.7 (3 +) 92 ,8+=100; ,8+p~Se-5

132Sm --55130# 700# 4.0 s 0.3 0 + 92 /3+=100; ,8+p ? 132Eu --42700# 900# 400# ms 93Li40 D ,8+ ?; p=0

*132In T : average 93Ru01=221(11) 85Re.A=204(6) and 86Wa17=204(6)

*1321h" T : average 94Bu18=1.47(0.12) 74Ar27=1.6(0.3)

*132Nd T : average 95Bu11=1.47(0.12) 77Bo02=1.75(0.17)

1331n --57440# 400#

133In m --57110# 400# 330# 40#

133Sn --70970 80

133Sb --78960 80

133Te --82960 80 133Te nl --82630 80 334.26 0.04

1331 --85878 26

1331nf --84244 26 1634.174 0.017

133Xe --87648 4

133Xe m --87415 4 233.221 0.018

133Cs --88075.7 3.0

133Ba --87558 3

133Ba m --87270 3 288.247 0.009

133La --85330 200

133Ce --82390# 200#

133CenJ --82350# 200# 37.1 0.8

133pr . --78060# 200#

133Nd --72460# 300#

133Nd" --72330# ~ 127.97 0.11

133pm --65470# 500# &

133pmm --65.M0# 500# 130.4 1.0 &

133Sm --57070# 600#

133Eu --47600# 900#

*1331n D : ,8-n intensity is from 93Ru01

2.19 d 0.01

STABLE

10.51 y 0.05

38.9 h 0.1

3.912 h 0.008

97 m 4

4.9 h 0.4

6.5

70 7O

15

180 ms 15 (9/2 +) 95 96Ho16 JT ,8-=100; ,8-n=85 10

180# ms ( 1 / 2 - ) 96Ho16 J IT ?

1.45 s 0 .03 ( 7 / 2 - ) 95 93Ru01 D ,8-=100; ,8--n=0.0294 24

2.5 m 0.1 (7/2 + ) 95 ,8- =100 12.5 m 0.3 (3/2 + ) 95 ,8-- =100 55.4 m 0.4 (11 /2- ) 95 ,8-=82.5 30; IT=17.5 30

20.8 h 0.1 7/2 + 95 ,8- =100 9 s 2 (19 /2- ) 95 IT=100

5.243 d 0.001 3/2 + 95 ,8-- =100

11/2- 95 IT=100

7/2 + 95 IS=I00.

1/2 + 95 t=100

11/2- 95 IT~,-~I00; ~=0.0096 11

5/2 + 95 ,8+=100

1/2 + 95 ,8+=100

9 /2 - 95 ,8+=100 m 0.3 (3/2 + ) 95 ,8+=100

s 10 (7/2 + ) 95 ,8+=100

s (1/2) + 95 95Br24 D ,8+=100 s 3 (3/2 +) 95 96Ga17 J ,8+=100

(11/2- ) 96Ga17 EJ ,8+ ?; IT ?

3.7 s 0.7 5/2+# 95 /3+=100; ,8+0=?

1# s 11/2-# ~+ ?



1341n --51550# 500# 138 ms 8 high 96Ho16 TJ /3-=100; / 3 -n>17 ; , 8 - 2 n < 4

134Sn --66640 l i d 1.12 s 0.08 0 + 94 /3-=100; /3-n=17 13

134Sb --740111 5(1 * 780 ms 60 ( 0 - ) 95 , 8 - = l i d

IMsbm --73930 110 80 110 BD * 10.22 s 0.09 ( 7 - ) 95 ,8-=100; /3-n=0.091 8

134Tc --824011 30 41.8 m 0.8 0 + 95 /3 -=100

1341 --83949 t5 52.5 m 0.2 (4) + 94 / 3 - = l i d

L'~'I'~ --83633 15 316.49 0.22 3.60 m 0.10 (8)-- 94 IT=97.7 10; ,8 -=2 .3 10

134Xc --88124.4 0.8 STABLE > l l P y 0 + 94 89Ba22 T IS=10.4 2; 2 /3- ?

134Xen' --86158.9 0.9 1965.5 0.5 290 ms 17 7 - 94 IT= l id

J~Cs --86895.9 3.0 2.0648 y 0.0010 44 94 ,8-=100; e---0.0iD3 1

134Cs"~ --86757 3 138.7441 0.0026 2.903 h 0.008 8 - 94 IT=liD

134Ba --88954.5 3.0 STABLE 0 + 95 IS=2.417 27

134La --85241 26 6.45 m 0.16 1 ~ 94 /3+=100

134Ce --84740 200 3.16 d 0.04 0 + 94 ~=100

134pr - 7 8 5 5 0 # 300# * 17 m 2 2 - 94 ,8+=100

IMprm --78550 220 0# 200# * 11 m ( 5 - ) 94 ,8+=100

134Nd --75780# 330# 8.5 m 1.5 0 + 96 /34 = l i d

134pm --66610# 390# * 22 s 1 (5 + ) 94 /3+=100

IMpmm --66610# 400# 0# 100# * 5 s (2 ÷ ) 94 /3~ = l i d

134Sm --61460# 500# 10 s 1 0 + 94 /3~ =100

IMEu --500(]00 700# 500 ms 200 94 /34=100; /3+p=?

• 1341n D : /3--n and / 3 - 2 n intensity limits are from 95Jo.A

1351n liD# ms 9 /2+# f l - ?; /3+n ?

135Sn --60800# 400# > 150 ns 7 / 2 - # 94Be24 T f l - ?; / 3 - n ?

135Sb --69710 110 1.680 s 0.015 7 /2+# 88 93Ru01 TD ,8-=100; ,8-n=17.6 22

135Te --77830 90 19.0 s 0.2 ( 7 / 2 - ) 88 / 3 - = l i D

135I --83788 23 6.57 h 0.02 7/2 + 88 /3 -=100

135Xe --86436 10 9.14 h 0.02 3/2 + 88 , 8 - = 100

135Xe'+ --859139 10 526.551 0.013 15.29 m 0.05 11/2-- 88 IT,~IID; /3---0.004

135Cs --87587 3 2.3 My 0.3 7/2 ~ 88 8 - = 1 0 0

135Cs m --85954 3 1632.9 1.5 53 m 2 1 9 / 2 - 88 IT=liD

135Ba --87855.9 3.0 STABLE 3/2 + 88 IS--6.592 18

135Ba m --87588 3 268.219 0.020 28.7 h 0.2 1 1 / 2 - 88 IT=liD

135La --86656 10 19.5 h 0.2 5/2 + 88 ,8"=100

135Ce --84630 11 17.7 h 0.2 1/2 (+1 96 /3+=100

135 Cem - 8 4 1 8 4 11 445.8 0.2 20 s 1 11/2 I - ) 96 IT=liD

135pr --81010 150 24 m 2 3/2 I+) 96 /3~=1/}0

135Nd --76160# 210# 12.4 m 0.6 9/2-- 96 /3+=100

135Ndm --76100# 210# 65.1 0.5 5.5 m 0.5 (1/2 + ) 96 89Ko07 E /34 = l i d

135pro --70220# 320# * 49 s 3 (5/2 + ) 96 89Ko07 TJ /3+=1110

135pro" --70120# 250# liD# 200# * 40 s 3 ( 1 1 / 2 - ) 96 89Ko07 TJ ,81~=100

135Sm --631120# 5(}0# * 111.3 s 0.5 (7/2 + ) 96 ,8+=100; /3~ p=0.02 1

135Sm m --63020# 580# 0# 30(0 * 2.4 s 0.9 ( 3 / 2 + , 5 / 2 + ) 88 89Vi04 TJD /3+=100

135Eu --542911# 6{X)# 1.5 s 0.2 11/2--# 96 /3+=1110; /3+p ?

135Gd 1.1 s 0.2 5 /2+# 96Xu07 TD /3+=100; /3+p~2

• 1351n 1 : T=195(3) ms in 93Kr05 is a misprint for 133In

• 135Sb T : average 93Ru01=1.662(0.010) 77Ru04=1.706(0.014) and 68To19=1.700(0.020)

• 135Smm 1 : existence of 135Smm is discussed in ENSDF

* : g

g t ~


Nuclide Mass excess Excitation Half-life f i r Eas Reference Decay modes and intensifies (keV) energy(keV) (%)

136Sn --56500# 500# > 150 ns 0 + 94Be24 T / 3 - ? ; / 3 - n ? 136Sb --64590# 300# 923 ms 14 1 - # 94 93Ru01 TD /3-=100; /3 -n=17 3 * 136Te --74420 50 17.63 s 0.08 0 + 94 93Ru01 TD /3-=100; /3--n=1.30 6 *

1361 --79500 50 83.4 s 1.0 ( 1 - ) 94 / 3 - =100 t361m --78850 110 650 120 BD 46.9 s 1.0 ( 6 - ) 94 / 3 - =100 136Xe --86424 7 STABLE >210Ey 0 + 94 93Vu02 T IS=8,9 1; 2/3-- ? 136Cs --86344 4 * 13.16 d 0.03 5 + 94 /3 -=100 136Csm --86140# 140# 200# 140# * 19 s 2 8 - 94 IT=?; /3-- ? 136Ba --88892.4 3.0 STABLE 0 + 94 IS=7.854 36 136Barn --86862 3 2030.52 0.02 308.4 ms 1.9 7 - 94 IT=I00 l ~ L a --86020 70 9.87 m 0.03 1 + 94 /3+=100 136Lain --85780 70 241 7 114 ms 3 (7 ,8 ) (-#~ 94 ABBW E IT=I00 *

I ~ C e --86500 50 STABLE 0 + 94 1S--0,19 1; 2/3 + ? l ~ p r --81370 50 13.1 m 0.1 2 + 94 /3+=100 136Nd --79160 60 50.7 m 0.3 0 + 96 /3+=100 136pm --71310 210 * 107 s 6 5 (+) , 6-- 94 /3+=100 136pmm --71070# 320# 240# 240# * 47 s 2 (2 + ) 94 /3+=1011 136Sm --66790# 400# 47 s 2 0 + 94 /3+=100 136Eu --56360# 500# * 3.3 s 0.3 (7 + ) 94 89Vi04 D /3+=100; /3+p=0.09 3 136Eu" --56360# 710# 0# 500# * 3.7 s 0.3 (3 + ) 94 89Vi04 D /3+=100; fl+p--0.09 3

136Gd --49300# 700# 1# s 0 + /3+ ? • 136Sb T : supersedes 76Lu02=820(20) from same group ** • 136Te T : average 93Ru01=17.66(0.09) 78Ct03=17.5(0.2) ** ,136 Lam E : less than 22 keV above 230.1 level, from ENSDF, thus 230.1 + 1 1 (7) **

137Sn --50500# 600# > 150 ns 5 / 2 - # 94Be24 T / 3 - ? 137Sb --60260# 400# > 150 ns 7 / 2 + # 94Be24 T / 3 - ? ; / 3 - n ? 137Te --69560 120 2.49 s 0.05 ( 7 / 2 - - ) 94 93Ru01 D /3-=100; /3-n=2.99 16 1371 --76501 28 24.13 s 0.12 (7/2 + ) 94 93RB01 TD /3--=100; /3--n=7.14 23 * 137Xe --82379 7 3.818 m 0.013 7 / 2 - 94 f l - =100 137Cs --86551.1 3.0 30.07 y 0.03 7/2 + 96 /3--=100 137Ba --87726.8 3.0 STABLE 3/2 + 94 IS=I 1.23 4 137Ba m --87065 3 661.660 0.003 2.552 m 0.001 11/2-- 94 IT=I00 I37La --87130 50 60 ky 20 7/2 + 94 e=100 137Ce --85900 50 9.0 h 0.3 3/2 + 94 /3+=100 137Cem --85650 5(1 254.29 0.05 34+4 h 0.3 11/2-- 94 IT=99.22 3; /3+--0.78 3 137pr --83200 5(1 1.28 h 0.03 5/2 + 94 fl+=100 137Nd --79510 70 38.5 m 1.5 1/2 + 96 /3+=100 137Nd m --78990 70 519.6 0.5 1.60 s 0.15 1 1 / 2 - 96 IT= 100 137pm --73860# 140# * & 2# m 5 /2+# /3+ ? 137pm'+ --73860 90 0# 100# * & 2,4 m 0.1 1 1 / 2 - 94 /3+=100 137Sm --67960 110 45 s 1 ( 9 / 2 - ) 94 /3+=100

137Smm --67780# 120# 180# 50# 20# s 1/2+# /3+ ? 137Eu --60350# 500# 8+4 s 0.5 ( 1 1 / 2 - ) 94 88Be+A T /5+=100 137Gd --51560# 600# 7 s 3 7 / 2 + # 94 /3+=100; /3+p=? 137Tb 150# ms 1 1 / 2 - # p ?; fl+ ?

• 1371 T : supersedes 74Ru08=24.5(0.2) from same group **

138Sb --55000# 500# > 150 ns 2 - # 94Be24 T fl-- ?; /3--n ? t38Tc --65930# 210# 1.4 s 0.4 0 + 95 /3-=100; fl--n=6.3 21 1381 --72300 80 6.49 s 0.07 ( 2 - ) 95 93Ru01 D / 3 - =100; / 3 - n=5.46 18 * t38Xe --80120 40 14.08 m 0+08 0 + 95 /3-- =100 t38Cs --82893 10 33.41 m 0.18 3 - 95 /3 -=100 t38csm --82813 10 79.9 0.3 2.91 m 0.08 6 - 95 IT=81 2; / 3 - = 1 9 2 138Ba --88267.2 3.0 STABLE 0 + 95 1S=71.70 7 t38La --86529 4 t05 Gy 2 5 + 95 1S=0.0902 2; ff----66.4 5; . . . * 138Ce --87574 11 STABLE 0 + 95 IS=0.25 1; 213 + ? 138Cem -85445 11 2129.17 0.12 8.65 ms 0.20 7 - 95 IT=100




. . . A-group continued . . . 138 Pl' --83137 15 1.45 m 0.05 1 + 95 3+=100 138 Pt'~ --82773 23 364 22 BD 2.12 h 0.04 7-- 95 /3+=100 138Nd --82040# 200# 5.04 h 0.09 0 + 95 /3+=100 138pro --75040# 320# * & 3.24 m 0.05 ( 5 - , 4 + ) 95 fl+=100 138pmm --74950# 210# 80 260 BD * & 10 s 2 1 + 95 /3+=100 I38pmn non existent EU 3.24 m 0.05 (3 + ) 95 81De38 I /3+=100 138Sm --71220# 300# 3.l m 0.2 0 + 95 3+=100 138Eu --61990# 400# 12.1 s 0.6 ( 6 - ) 95 /3+=100 138Gd --55920# 500# 5# s 0 ÷ 95 /3+ ? 138Tb --43900# 800# 400# ms 93Li40 D /3+ ?;p=O

• 1381 T : ENSDF averages 6 values. Also 93Ru01=6.23(0.03) • 138La D : . . . ; / 3 - = 3 3 . 6 5

• I38pm" D : Arguments for a second isomer, with intermediate spin, is not convincing

139Sb --50570# 600# > 150 ns 7 /2+# 94Be24 T 139Te --60800# 400# > 150 ns 5 / 2 - # 94Be24 T 1391 --68840 30 2.282 s 0.010 (7/2 + ) 89 93RuOl TD 139Xe --75650 21 39.68 s 0.14 3/2-- 89 139Cs --80707 4 9.27 m 0.05 7/2 + 89 139Ba --84919.3 3.0 83.06 m 0.28 7 / 2 - 89 139La --87236 3 STABLE 7/2 + 89 139Ce --86958 8 137.640 d 0.023 3/2 + 89 139Cem --86204 8 754.24 0.08 56.54 s 0.13 1 1 / 2 - 89 94It.A T 139pr --84829 8 4.41 h 0.04 5/2 + 89 139Nd --82040 50 29.7 m 0.5 3/2 + 89 139Ndm --81810 50 231.15 0.05 5.50 h 0.20 1 l / 2 - 89 139pm --77540 60 4.15 m 0.05 (5/2) + 89 139pmm --77350 60 188.7 0.3 180 ms 20 ( 1 1 / 2 ) - 89 139Sm --72375 15 2.57 m 0.10 1/2 (+) 89 87AI.A J 139Sm" --71917 15 457.8 0.4 10.7 s 0.6 ( 1 1 / 2 ) - 89 139Eu --65360# 150# 17.9 s 0.6 ( 1 1 / 2 ) - 89 139Gd --57680# 500# 5.7 s 0.4 9 / 2 - # 89 88Be.A T 139Tb --48410# 700# 700# ms 11/2- -# 139Dy 200# ms 7 /2+#

• 1391 T : average 93Ru01=2.280(0.011) 80A115=2.29(0.02) • 139Gd T : average 88Be.A=5.8(0.4) 83Ni05--4.9(1.0)

O - ? / 3 - ? ; / 3 - n ? /3-=100; / 3 - n=10.0 3 / 3 - =11]0 / 3 - =100 / 3 - =100 IS--99.9098 2 e=100 IT=I00 /3+ =100 /3+=100 /3+=88.2 4; IT=l l .8 4 /3+=1o0 I T ~ 100; /3+----0.16#

/3+=100 IT=93.7 5; fl+=6.3 5 /3+=100 3+ ~,."~ 10(1; /3+ p=?

/3+ ? B + ?

140Te --57100# 500# > 150 ns 0 t 94Be24 T 1401 - 6 4 0 8 0 # 210# 860 ms 40 (3) ( - # ) 95 140Xe --73000 60 13.60 s 0.10 0 + 95 140Cs --77056 9 63.7 s 0.3 1 - 95 140Ba --83276 8 12.752 d 0.003 0 + 95 140La - 8 4 3 2 6 3 1.6781 d 0.0003 3 - 95 140Ce --88088 3 STABLE 0 ÷ 95 140pr --84700 7 3.39 m 0.01 1 + 95 140Nd --84477 19 3.37 d 0.02 0 + 95 140pm --78430 30 9.2 s 0.2 1 + 95 140pmm --77990 70 440 70 BD 5.95 m 0.05 8 - 95 140Sm --75459 15 14.82 m 0.12 0 + 95 140Eu --66990 50 1.51 s 0.02 14 95 140Eu)n --66780 50 210 15 125 ms 2 5 - # 95 ABBW E 140Gd --61530# 400# 15.8 s 0.4 0 + 95 91Fi03 T 140Tb --50730# 900# 2.4 s 0.2 5 95 91Fi03 D 140Dy --43040# 900# 700# ms 0 +

*140Eum E : less than 50 keV above 185.3 level, from ENSDF, thus 185.3 + 25(15) *140Tb D : 0.26(13)% is for f l+p decay (not p, as given by ENSDF)

/ 3 - ? ; / 3 - n ? , 8 - = 1 0 0 ; / 3 - n--9.3 10 3 - =100 /3 -=100 /3 -=100 /3 -=100 IS=88.48 10 /3+ =100 e=100 #+ =100 /3+=100 ~+=100 /3+=100 IT~,-.~, 100; 13 + < 1 3 + =100 /3+=100; /3+p=0.26 13

/3+ ?


Nuclide Mass excess Excitation Half-life j~r Eas Reference Decay modes and intensities (keV) energy(keV) (%)

141Ze --51800# 500# > 150 ns 5 / 2 - # 94Be24 T /3- ?; /3--n 7

1411 --60710# 300# 430 ms 20 7/2+# 91 93Ru01 D /3-=100; /3-n=22 3

141Xe --68330 90 1.73 s 0.01 5/2 ( -#) 91 93Ru01 D /3-=100; /3--n=0.043 3 141Cs --74479 l0 24.94. s 0.06 7/2 + 91 93Ru01 D /3-=100; /3--n=0.035 3

141Ba --79730 8 18.27 m 0.07 3 / 2 - 91 /3-=100 14lEa --82943 5 3.92 h 0.03 (7/2 +) 91 /3-=100

14ICe --85445 3 32.501 d 0.005 7 / 2 - 91 /3-=100

141pr --86026 3 STABLE 5/2 + 91 IS=100.

141Nd -- 84203 4 2.49 h 0.03 3/2 + 91 15 + =100

14lNdm --83446 4 756.7 0.1 62.0 s 0.8 11/2-- 91 IT~,I00; /3+<0.05

t41pm --80475 27 20.90 m 0.05 5/2 + 91 /3+=100

141Sm --75946 12 10.2 m 0.2 1/2 + 91 /3+=100

14lSmm --75770 12 175.8 0.3 22.6 m 0.2 11/2- 91 /3+,,"~100; IT=0.31 3

141Eu --69968 28 40.7 s 0.5 5/2 + 91 93A103 T /3+=100

141Eu m --69872 28 96.4 0.1 2.7 s 0.3 11/2- 91 IT=86 3; /3+=14 3 141Gd --63150# 300# 14 s 4 (1/2 +) 91 ~'+=100; fl+p--0.03 1

141Gd m --62770# 300# 377.8 0.2 24.5 s 0,5 ( 1 1 / 2 - ) 91 fl+=89 2; IT=II 2 14lTb --54810# 600# * 3.5 s 0,2 (5/2--) 91 /3+=100

14tTb" --54810# 630# O# 200# EU * 7.9 s 0,6 1 1 / 2 - # 91 88Be.A I fl+=100

t41Dy --45470# 700# 900 ms 200 ( 9 / 2 - ) 91 /3+=100; /3+p=? 14trio 100# ms 11/2--# p ?; /3+ ?

.141Xe J : positive parity, adopted by ENSDF, is the only case for even-Z/odd-N *14lXe J : nuclides in this region. Needs to be confirmed. .141 Ell T : average 93A103=41.4(0.7) 77De25=40.0(0.7)

.t41Eu m D : symmetrized from IT=87(+2-4)% and fl+=13(+4-2)%

*141Tbm 1 : existence discussed in 88Be.A. Provisionally accepted

.141Ho I) : proton emitter, in post cut-off date 97Da.A

142Te --47970# 600# > 150 os

1421 --55720# 400# 200 ms

142Xe --65480 100 1.22 s 0.02

142Cs --70521 l l 1.689 s 0.011

142Ba --77828 6 10.6 m 0,2

142La --80039 6 91.1 m 0,5

142Ce --84543 3 STABLE >50Py

142pr --83797 3 19.12 h 0.04

142 Prn' --83793 3 3.6815 0.0011 14.6 m 0,5

142Nd --85959.5 2.8 STABLE 142pm --81090 40 40.5 s 0,5

142pm"f --80210 40 883.17 0.16 2.0 ms 0~2

t42 Sm -- 78997 11 72.49 m 0.05 142Eu --71350 30 2.36 s 0.10

142Eum --70830 40 520 50 BD 1.223 m 0.00~ 142Gd --66850# 300# 70.2 s 0.6

142Tb --56950# 760# 597 ms 17

142Tbm --56670# 760# 280.1 1.0 303 ms 7 142Dy --50050# 790# 2.3 s 0.3

142Ho --37390# 1000# 300# ms

• 142Cs T :average 93Ru01=1.684(0.014) 77Re05=1.70(0.02)

• 142Ce T : lower limit is for a decay (not double/3- decay, as given by ENSDF)

• 142Eu T : average 91Fi03=2.34(0.12) 75Ke08=2.4(0.2)

0 + 94Be24 T /3-- ?

2 - # 75Kr17 T /3--=100; /3-n=25#

0 + 9 1 93Ru01 D /3--=100; /3-n=0.41 3

0 - 91 93Ru01 TD /3--=100; /3-n--0.091 4

0 + 91 /3-- =100

2 - 91 /3--=100 0 + 91 61Ma05 T IS=11.08 10; 2/3- ?; ot ? 2 - 91 /3--~100; e--0.0164 8

5 - 91 IT=I00 0 + 91 IS=27.13 12

1 + 91 fl+=100 ( 8 ) - - 91 1T=I00

0 + 96 /3 + = 100

1 + 96 91Fi03 T /3+=100

8-- 96 93A103 T /3+ =100

0 + 91 /3+=100 1 + 91 91Fi03 D fl+=100; fl+p---0.0022 11

( 5 - ) 91 91Fi03 D IT~I00; fl+<0.5 0 + 91 91Fi03 D /3+=100; /3+p=0.06 3

93Li40 D /3+ ?; p=0

:,i¢ a.lt


Nuclide Mass excess Excitation Half-life fir Ens Reference Decay modes and intensities ( keV ) energy ( keV ) ( % )

1431 --52100# 400# > 150 ns 7 /2+# 94Be24 T /3 - ? •

143Xe --60650# 220# 300 ms 3~ 5 / 2 - 91 /3 - =100

143Cs --67691 22 1.791 s 0.008 3/2 + 91 93Ru01 TD , 8 - = 1 0 0 ; / 3 - n=1.62 6 *

143Ba -73945 13 14.33 s 0.08 5 / 2 - 91 / 3 - =100

143La --78191 15 14.2 m 0.1 (7/2) + 91 /3-=100 143Ce --81616 3 33.039 h 0.006 3 / 2 - 91 /3 -=100

143pr --83078 3 13.57 d 0.02 7/24 91 /3 -=100

143Nd --84011.8 2.8 STABLE 7/2-- 96 1S=12.18 6

143pm --82970 4 265 d 7 5/2 + 91 /3+=100

143Sm --79528 4 8.83 m 0.01 3/2 + 91 /3+=100 143smn' --78774 4 754.0 0.2 66 s 2 1 1 / 2 - 91 IT~I00; /3+=0.24 6

143Smn --76734 4 2794.7 0.5 30 ms 3 23/2 ( - ) 91 IT=100

143Eu --74253 13 2.586 m 0.026 5/2 + 96 93AI03 T /3+=100 *

143Gd --68240 200 39 s 2 (1/21 + 91 78Fi02 D /3+=100; /3+p=?; /3+a=? *

143Gd" --68090 200 152.6 0,5 112 s 2 1 1 / 2 - 9l 78Fi02 D /3~-=100; /3+p=?; /3+or=?

143Tb --60780# 4~)# * 12 s 1 (11 /2 - - ) 94 /3+=100

143Tb n' --60780# 450# 0# 200# * < 21 s 5 /2+# 94 /3+ ?

143Dy --52320# 500# 3.9 s 0.4 1/2+# 83Ni05 TD /3+=100; /3+p=? *

143Ho --42210# 700# 300# ms 1 1 / 2 - # /3+ ?

* 1431 D : from systematics,/3-- n can be est imated/3- n=40%#

*143Cs T : average 93Ra01=1.809(9) 79En02=1.78( 11 77Re05=1.79(2) 76Lu02=1.78( 11

*143Eu T : average 93A103=2.57(0.031 74Ke07=2.63(0.05)

*143Gd D : 78Fi02: /3+p and/or /3+a for 143Gd+143Gdm=0.001%+ 39 particles detected

*143Dy T : average 84Ni03=3.2(0.6) 83Ni05=4.1(0.31

1441 --46940# 500#

144Xe --57540# 320#

144Cs --63316 28

144Csm --63020# 200# 300# 200#

144Ba --71780 14

144La --74900 6(}

144Ce --80441 4

144pr --80760 4

144 Plall --80701 4 59.03 0,03

144Nd --83757.5 2.8

144pm --81426 4

144Sm --81976 3

144Eu --75661 18

144Gd --71920# 200#

]44Tb --62850# 300#

144 Tbm - 62450# 300# 396.9 0.5

144Dy --56760# 400#

144Ho -- 450Y0# 6(k3#

144Er --36710# 800#

* 1441 D : from systematics,/3-- n can be est imated/3- n=40%#

*144Cs T : average 93Ru01=982(5) 79Ri09=1000(10) and 79En02=1030(10)

> 150 as

1.15 s 0.20

* 993 ms 13

* < 1 s

11.5 s 0.2

40.8 s 0.4

284.893 d 0.008

17.28 m 0.05

7.2 m 0.3

2.29 Py 0.16

363 d 14

STABLE

10.2 s 0.1

4.5 m 0.l

I s

4.25 s 0.15

9.1 s 0.4

700 ms 100

400# ms

1 - # 94Be24 T f l - ?

0 + 89 /3-=100; / 3 - n ?

l f - # ) 89 93Ru01 TD /3-=100; /3-n=3.20 21

( > 3) 89 /3 -=? ; IT ?

0 + 89 /3-=100; /3 -n=3.6 7

( 3 - ) 89 /3 =100

0 + 89 /3-- =100

0 - 89 / 3 - =100

3 - 89 I T ~ 100; /3-=0.07

0 + 96 1S=23.80 12; ot=100

5 - 89 /3+ =100

0 + 89 IS=3.l 1; 2/3 + ?; ot ?

1 + 96 /3+=151

0 + 96 /3+=100

(1 + ) 89 /3+=100; /3+p ?

( 6 - ) 89 IT=66; 13 ÷ =34; /3+p ?

0 + 89 /3+=100; /3+ p=?

89 /3+=100; /3+ p=?

0 + /3+ ?


Nuclide Mass excess Excitation Half-life j , r Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

145Xe --52470# 400#

145Cs --60190 50

145Ba --68070 60

145La --72990 70

145Ce --77100 40

145pr --79636 8

145Nd --81441.6 2.8

145pm --81279 4

145 Sm -- 80662 3

145Eu --7800"2 4

145Gd --72950 40

145Gdm --72200 40 748.7 0.1

145Tb --66250# 230# *

145Tb m --66250 200 0# 100# *

145Dy --58730# 300#

145Dym --58610# 300# 118.2 0.2

145 Ho --49480# 600#

t45 Er --39630# 700#

• 145Cs T : average 93Ru01=579(6) 82Ra13=594(13)

900 ms 300 3 / 2 - # 7 lWo02 TD f l - = 1 0 0

582 ms 6 3/2 + 93 93Ru01 TD f l -=100 ; /3-n=14.3 8

4.31 s 0.16 5 / 2 - 93 /3 -=100

24.8 s 2.0 (5/2 + ) 93 96Llt02 J f l - =100

3.01 m 0.06 (3/2) - 93 f l - =100

5.984 h 0.010 7/2 + 93 f l -=lO0

STABLE 7/2-- 93 IS=8.30 6

17.7 y 0.4 5/2 + 93 e=100; a=2.8e-7

340 d 3 7/2-- 93 e=100

5.93 d 0.04 5/2 + 93 fl+=100

23.0 m 0.4 1/2 + 96 fl+=100

85 s 3 11/2-- 96 IT--94.3 5; fl+=5.7 5

20# m (3/2 + ) 96 93To04 J 13 + ?

30.9 s 0.7 ( 1 1 / 2 - ) 96 93AI03 T ,8+=100

9.5 s 1.0 (1/2 + ) 93 93A103 T /3+=100; fl+p=?

14.1 s 0.7 ( 1 1 / 2 - ) 93 93To04 T fl+=100

2.4 s 0.1 ( 1 1 / 2 - ) 93 fl+=100

900 ms 300 1/2+# 93 fl+ =100; fl+p=?

*145Tbm T : average 93A103=31.6(0.6) 82No08=29.5(1.0) and 82Alff'/=29.5(1.5)

,145Dy T : average 93A103=10.5(1.5) 93To04--6(2) and 84Sc.C=10(1)

*145Dym T : average 93To04=14.5(1.0) 82No08=13.6(1.0) JIc*

146Xe --49090# 400#

146Cs --55740 80

146Ba --65110 80

146La --69210 70 *

146Lain --69080 150 130 130 *

146Ce --7~740 70

146pr --76770 60

146Nd --80935.5 2.8

146pm --79464 5

146Sm --81006 4

146Eu --77128 7

146Gd --76098 5

146Tb --67830 50 *

146Tbm --67680# 110# 150# 100# *

146Tb" --66900# 110# 930# 100#

146Dy --62670 110

146 Dym --59730 110 2935.6 0.7

146Ho --52070# 500#

146Er --44600# 600#

146Tin --31210# 700#

146Tmm --31140# 700# 71 7 p

• 146Cs T : average 93Ru01=321(2) 76Lu02=343(7)

• 146Lain E : derived from Q(146Lam)=6660(120) in 79Ke02

• l'16Tb" E : 779.6 keV above 146Tbm. 0"ore ENSDF

> 150 ns 0 + 90 94Be24 T /~- ?

323 ms 6 1 - 90 93Ru01 TD ,8-=100; f l -n=14 .2 5

2.22 s 0.07 0 + 90 93Ru01 D f l - = 100 ; / 8 -n<0 .02

6.27 s 0.10 2 - 90 93Ru01 D fl--=100; f l - -n<0 .007

10.0 s 0.1 ( 6 - ) 90 79Keff2 E ~ - =100

13.52 m 0.13 0 + 90 f l - = 1 0 0

24.15 m 0.18 ( 2 ) - 90 f l - = 1 0 0

STABLE 0 + 90 IS=17.19 9; 2 ,8 - 7; a~ ?

5.53 y 0.05 3-- 90 ~=66.0 13; 1~--=34.0 13

103 My 5 0 + 90 ot=100

4.59 d 0.03 4-- 90 ~fl-=100

48.27 d 0.10 0 + 96 ~=100

8 s 4 1 + 90 fl+=100

24.1 s 0.5 5 - 90 93A103 T ,8+=100

1.18 ms 0.02 (10 + ) 90 IT=I00

33.2 s 0.7 0 + 90 93A103 T ,8+=100

150 ms 20 ( 10 + ) 90 IT=100

3.6 s 0.3 ( 10 + ) 90 g+ =100; fl+p=?

1.7 s 0.6 0 + 93To05 TD fl+=100; fl+p=?

235 ms ( 6 - ) 93Li18 TD p ~ 100; fl+ ?

72 ms (10 + ) 93Li18 TD p~100; .fl"- ?



147Xe --43770# 500# > 150 ns 3 / 2 - # 94Be24 T / 3 - ?; / 3 - n ?

147Cs --522911 150 225 ms 5 (3/2 + ) 92 93Ru01 D /3-=100; / 3 - n=28.5 17

147Ba --61490 90 893 ms 1 ( 3 / 2 - ) 92 93Ru01 D /3-=100; /3-n=0.06 3

147La --67240 80 4.015 s 0.008 (5/2 + ) 92 93Ru01 D /3-=100; /3-n=0.040 3

147Ce --72180 50 56.4 s 1.0 ( 5 / 2 - ) 92 /3 - =100

147pr - 7 5 4 7 0 40 13.4 m 0.4 (3/2 + ) 92 /3 -=100

147Nd --78156.3 2,8 10.98 d 0.01 5 / 2 - 92 /3 -=100

147pm --79052.3 2.9 2.6234 y 0.0002 7/2 + 96 / 3 - =100

147Sm --79276.4 2.9 1116 Gy 2 7/2 92 IS=15.0 2; ct=100

147Eu --77555 4 24.1 d 0.6 5/2 + 92 /3+,'~100; o,--0.0022 6

147Gd --75368 4 38.116 h 0.12 7 / 2 - 96 /3+ =100

147Tb --70759 12 1.7 h 0.1 (1/2 + ) 96 /3+=100

147Tbm --70708 12 50.6 0.9 1.87 m 0.05 ( 1 1 / 2 ) - 96 93A103 T /3+=100

147Dy --64390 50 40 s 10 1/2 + 92 84'I"o07 D /3~=100; /3+p~0.05

147Dym --63640 50 750.5 0.4 55 s 1 1 1 / 2 - 92 /3+=65 4; 1T=35 4

147Ho --56040# 400# 5.8 s 0.4 1 1 1 / 2 - ) 92 /3+=100; /3+p ?

147Er --47220# 500# & 2.5 s 11/2 + ) 92 /3+=100; /3+p=?

14TErm --47120# 500# 100# 50# & 2.5 s 0.2 ( 11 / 2 - - ) 92 /3+=100

147Tin --362511# 600# 580 ms 40 111/2-- ) 92 93To02 TD /3+=85 5; p=15 5

*147La J : from 96Ur02

* 147T'o T : 1.6410.03) h in post cut-off date 97Wa04

*147Tb m T : average 93AI03=1.92(0.07) 73Bo13=1.83(0.06) E : from 87Li09

*I47E]J" E : estimated from 1 1 / 2 - level in isotones 141Sm=175101 143Gd=152(01 145Dy=118(0)

*147Tm T : average 93To02=640160) 83La27=560140)

148Cs - 4 7 6 0 0 590 158 ms 7 911 93Ru01 D /3-=100; /3-n=25.1 25

148Ba --58115() 1411 607 ms 25 0 + 90 93Ru01 D /3-=100; /3-n---0.4 3

148La --63160 IX) 1.05 s 0.01 ( 2 - ) 90 93Ru01 D /3-=100; /3-n--0.15 3

148Ce --70430 121.) 56 s 1 0 + 90 / 3 - =100

148pr --72490 90 * 2.27 m 0.04 1 - 90 /3 -=100

148 Prm --72440# 90# 51)# 30# * 2.0 m 0.1 (4) 90 ABBW E /3--=100

148Nd --77418 3 STABLE >3.0Ey 0 + 90 82Be20 T IS=5.76 3; 2/3-- ?; a ?

148pro --76878 7 5.370 d 0.009 1 - 90 / 3 - =100

148pmm --76741 7 137.00 0.10 41.29 d 0.11 6 - 90 /3 -=95 .0 4; IT=5.0 4

148Sm --79346.6 2.9 7 Py 3 0 + 90 IS=11.3 1; o,=1130

148Eu --76239 18 54.5 d 0.5 5 - 911 /3+=100; a--9.4e-7 28

148Gd --76280 3 74.6 y 3.0 0 + 96 o'=100; 2/3 + ?

148Tb --70520 30 611 m I 2 - 911 /3 + =100

148 Tb"~ --711430 311 90.1 0.3 2.20 m 0.05 9 + 90 /3+=100

148Dy --67830 30 3.1 m 0.1 0 + 9(1 /3+=100

148Ho --58430# 270# * 2.2 s 1.1 1 + 90 /3+=100

148Horn --58430 250 11# 100# * 9.49 s 0.12 6-- 90 93A103 T /3+=100; /3+p=0.08 1

148Hon --57740# 290# 690# 100# 2.35 ms 0.04 ( 10 + ) 90 IT=I00

148Er --51750# 400# 4.6 s 0.2 0 + 90 /3+=100; /3+p~0.15

148Tm --39540# 700# 700 ms 200 (10 + ) 90 /3+=11]0

148yb --30960# 800# 250# ms 0 + /3+ ?

• 148pl'm E : derived from ENSDF estimate E<90 keV

*148Hom T : average 93A103=9.30(0.20) 89Ta11=9.59(0.151

* 148Hon E : 694.4 keV above 148 Ho m, from ENSDF


Nuclide Mass excess Excitation Half-life ./,n. Ens Reference Decay modes and intensities ( key ) energy( keY ) ( % )

149Cs --44040# 300# > 50 ms 3 /2+# 95 87Ral2 T / 3 - ?; / 3 - n ?

149Ba --53600# 400# 344 ms 7 3 /2 - -# 95 /3-=100; /3-n---0,43 12

149La --61130# 300# 1,05 s 0.03 5 /2+# 95 93Ru01 D f l - = 1 0 0 ; / 3 - n = 1 . 4 3

149Ce --668130 80 5.3 s 0.2 3 / 2 - # 95 / 3 - = 100

149pr --70988 11 2.26 m 0.07 (5/2 + ) 95 / 3 - =100

149Nd --74385 3 1.728 h 0.001 5 / 2 - 95 / 3 - =100

149pm --76076 4 53,08 h 0.05 7/2 + 95 / 3 - = 100

149Sm --77146,8 2.9 STABLE >2Py 7 / 2 - 95 IS=13.8 1

149Eu --76451 5 93.1 d 0.4 5/2 + 95 ~=100

149Gd --75138 4 9.28 d 0,10 7 / 2 - 96 /3+=100; a=4,3e-4 10

149Tb --71500 5 4.118 h 0.025 1/2 + 95 /3+=83.3 17; ot=16.7 17

149Tbm --71464 5 35.78 0.13 4.16 m 0.04 1 1 / 2 - 95 /3+~100; a--0.022 3

149Dy --67688 11 4.20 m 0,t4 7/2 t - ) 95 88Ah02 J /3+=100

149Dy" --65027 11 2661.1 0.4 490 ms 15 ( 2 7 / 2 - ) 95 IT=99.3 3; /3+--0.7 3

149H0 --61674 22 21.1 s 0.2 ( 1 1 / 2 - ) 95 /3+=100

149Ho m --61625 22 48.80 0.20 56 s 3 (1/2 + ) 95 /3+=100

149Er --53860# 470# 4 s 2 (1/2 + ) 95 /3+=100; /3+p=7 2

149Erm --53120# 470# 741.8 0.2 8.9 s 0,2 ( 11 /2 - - ) 95 /3+--96.5 7; 1T=3.5 7; /3+p--0.18 7

149Tm --44110# 600# 900 ms 200 ( 1 1 / 2 - ) 95 /3+=100; /3+p=0.26 15

149yb --34020# 700# 600# ms ( 1 / 2 + , 3 / 2 + ) 95 13 + ?

*149Tm D : symmetrized from /3+p=0.2(+0.2-0.1)%

150Cs - 3 9 1 5 0 # 500# > 511 ms 87Ra12 T / 3 - ? ; / 3 - n ?

I ~ B a --50660# 500# ~ ms 0 + 95 /3--=100; /3--n ?

150La --57220# 400# 510 ms 30 (3 + ) 97 95Ok02 TJ /3-=100; /3-n=2.7 3

150Ce --64990 12(1 4.0 s 0.6 0 + 95 /3-- =100

150pr --68000 80 6.19 s 0.16 ( 1 ) - 96 /3 -=100

150Nd --73694 4 21 Ey 5 0 + 96 95Ar08 TD IS=5.64 3; 2/3--=100 *

150pm --73607 20 2.68 h 0.02 ( 1 - ) 95 8 - =100

150Sm --77061.1 2.9 STABLE 0 + 96 IS=7.4 1

150Eu --74801 7 36.9 y 0.9 5 ( - ) 95 /3+=100

150Eum --74759 7 42.1 0.5 12.8 h 0.1 0 - 95 / 3 - =89 2; ,8+=11 2; IT_Se-8

150Gd --75772 7 1.79 My 0.08 0 + 96 a=lO0; 2/3 + ?

150Tb --71116 8 3.48 h 0.16 ( 2 - ) 96 /3+~100; a<0.05

I~Tbm --70640 50 470 50 BD 5.8 m 0.2 9 + 96 /3+~100; IT ?

150Dy --69322 5 7.17 m 0.05 0 + 96 /3+=64 5; a=36 5

150Ho --62080# 100# * 76.8 s 1.8 2 - 95 93A103 T ,8+=100 *

150Horn --61960 50 120# 110# * 23.3 s 0.3 (9) + 95 /3+=100

150Er --57970# 100# 18.5 s 0.7 0 + 95 /3+=100

150Tm --46880# 500# * & 3# s ( l 4 ) 88Ni02 J /3+=100

150Tm m --46740# 520# 140# 140# * & 2.20 s 0.06 ( 6 - - ) 95 9(K3a24 T /3+=100; /3+p=1.2 3 *

150Tmn --46070# 520# 810# 140# 5.2 ms 0,3 ( 10 + ) 95 IT=I00 *

150yb --39130# 600# 700# ms 0 + /3+ ?

150Lu --25460# 700# 35 ms 10 (5 - - , 6-- ) 95 93Se04 J p=?; /3+=20#

• 150Nd T : symmetrized from 18.8(+6.6-3.9 statistics + 1.9 systematics) **

• 150Ho T : average 93A103=78(2) 82No08=72(4) **

• lSOTmn~ T : average 96Ga24=2.22(0.07) 88Ni02=2.15(0.10) and 87To05=2.2(0.2) **

• lSOTmm T : 82No08=3.5(0.6) at variance, not used D : from 88Ni02 **

• 150Tm n E : 671.6 keV above 150Tram, from ENSDF **


Nuclide Mass excess Excitation Half-life fir Eas Reference Decay modes and intensities (keV) energy(keV) (%)

151Cs - 3 5 4 0 0 # 700# > 50 lSIBa --45920# 600# > 150 151La --54440# 500# > 150 15ICe - 6 1 4 4 0 # 3,00# 1.02 151Pr --66860 40 18.90 151Nd --70957 4 12.44 lSlpm --73399 6 28.40 15lSm --74586.2 2.9 90 tS1Eu --74662.9 2.9 STABLE lSlGd --74199 4 124 151Tb --71634 5 17.609 151Tbm --71534 5 99.54 0.06 25 151Dy --68763 4 17.9 151Ho --63639 12 35.2 151Ho m --63598 12 41.10 0.20 47.2 151Er --58260# 300# 23.5 151El a~t --55680# 300# 2585.5 0.6 580 151Tm --50830# 140# & 4.13 151Tmm --50780# 130# 45# 15# & 5.2 151yb --41690# 320# * 1.6 151ybm --41690# 590# 0# 500# * 1.6 151Lu --30600# 600# * & 15ILu m --30600# 600# 0# |00# * & 85

.151pr J : ( 3 / 2 - ) in post cut-off date ENSDE'97 • 15lNd J : 3 / 2 - in post cut-off date ENSDF'97 .15lGd .151Ho m

.151Tin

.151Tm m • 151Tm m

.151Tmm

.151yb

.151 yb m

.151Lu

.151 Lu m

ms 3/2+# 89 87Ra12 T , 8 - ?; ,0--n ? ns 3 / 2 - # 94Be24 T , 0 - ? ns 5 /2+# 94Be24 T , 0 - ?

s 0.06 3 / 2 - # 89 , 8 - = 100 s 0.07 ( 1 / 2 , 3 / 2 , 5 / 2 ) - 89 , 0 - = 100 m 0.07 (3/2) + 89 , 8 - =100 h 0.04 5/2 + 89 , 0 - =100 y 8 5 / 2 - 89 fl-- =IG0

5/2 + 89 IS=47.8 15 d 1 7 / 2 - 89 e=100; a=l .0e-6 6 h 0.001 1/2 (+) 96 '8+,~-,100; a=0.0095 15 s 3 ( 1 1 / 2 - - ) 96 IT--93.8 4; /3+=6.2 4 m 0.3 7/2 ( - ) 96 /~=94 .4 4; a=5,6 4 s 0.1 11/2 ( - ) 89 87Ne.A J / ~ = ? ; 0"=22 3 s 1.0 1/2 (+) 89 91To08 ED ot=77 18; ,0~ ? s 1.3 ( 7 / 2 - ) 89 ,0+=100

ms 20 ( 2 7 / 2 - ) 89 IT=95.3 3; ,8+--4.7 3 s 0.11 ( 1 1 / 2 - ) 89 ,0+=100

s 2.0 ( 1/2 + ) 89 ,0+=100 s 0.5 (1/2 + ) 89 86To12 T ,0+=100; ,0+p=? s 0.5 ( 1 1 / 2 - ) 89 86To12 TD ,0+=100;,8~-p=?

1/2+# ,0+ ? ms 10 ( 1 1 / 2 - ) 89 93Se04 D p=?; ,0+=30#

D : a=0 .8 (+0 .8q) .4 )e~% in post cut-off date ENSDF'97 D : symmetrized from a=80(+15-20)% J : from 87Ne.A T : 4.17(0.10) s in post cut-off date ENSDF'97 T : 6.6(1.4) s in post cut-off date ENSDF'97 E : 97Da07=96.4(7.0) keV should replace the estimated AME'95=45# in next AME E : AME'95=45# estimated from 1 1 / 2 - level in isotopes 153Tm: 43(0) 155Tm: 41(6) T : derived from 1.6(0.1). for mixture of ground-state and isomer with almost same half-life

D : IT=0.4%# in post cut-off date ENSDF'97 I : Low spin ground-state not believed to exist. Kept for consistency with AME'95. T : 88(10) ms in post cut-off date ENSDF'97

152Ba --42700# 700# 100# ms 0 -~ 152La --50200# 600# > 150 ns 96 152Ce --59260# 400# 1.1 s 0.3 0 + 96 90Ta07 T 152pr --63710# 300# 3.63 s 0.12 ( 4 - ) 97 152Nd --70160 30 11.4 m 0.2 0 + 97 152pm --71270 70 * 4.12 m 0.08 1 + 97 152pmm --71120 80 140 110 BD * 7.52 m 0.08 4 - 97 152pmn --71020# 170# 250# 150# * 13.8 m 0.2 (8) 97 152Sm --74772.6 2.9 STABLE 0 + 97 152Eu --72898.3 2.9 13.537 y 0.006 3-- 97 152Eum --72852.7 2.9 45.5998 0.0004 9.3116 h 0.0013 0 - 97 t52Eu" --72750.5 2.9 147.86 0.10 96 m 1 8 - 97 152Gd --74717.1 3.0 108 Ty 8 0 + 97 152Tb --70730 40 17.5 h 0.1 2 - 97 152Tbm --70230 40 501.74 0.19 4.2 m 0.1 8 + 97 152Dy --70129 5 2.38 h 0.02 0 + 97 152Ho --63580 30 161.8 s 0.3 2 - 97 152 Hom -- 63420 30 160 1 50.0 s 0.4 9 .9 97 I52Er --60470 30 10.3 s 0.l 0 + 97 152Tm --51880# 300# * 8.0 s 1.0 (2#)-- 97 152Tm m --51680# 330# 200# 150# * 5.2 s 0.6 (9) + 97 152yb --46420# 360# 3.04 s 0.06 0 + 97 152Lu --33900# 700# 650 ms 70 ( 5 - - , 6 - - ) 97 88Ni02 T

• 152Ce T : average 90Ta07=1.4(0.2) 9lAy.A=0.8(0.3) • 152pmn E : ENSDF: "Probably feeds 7.52 m level" at 140 keV • 152Lu T : average 88Ni02=600(100) 87To02=700(100)

~ - ?

/ 3 - ?

f l - = l O 0 f l - = l O 0 f l - = l O 0 , 0 - =I00 f l - =I00 f l - ~ I00; IT=? IS=26.7 2 /3+--72.1 3; ,8 -=27 .9 3 , 8 - =72 4; ,8+ =28 4 IT=I00 IS--0.20 1; a=100; 20 + ? ,0+=100; a< 7e - 7 IT=78.8 8; /#-=21.2 8 e~,-~lO0; a=O.lO0 7 fl+=88 3; o,=12 3 ,0+=89.2 17; a=lO.8 17 0,=90 4; ,0+=10 4 ,0+=100 ,0+ =100 ,89=100; ,0+p ? ,8+=100; ,0+p=15 7


Nuclide Mass excess Excitation Half-life j.n. Ens Reference Decay modes and intensities (keV) energy(keV ) ( % )

I53Ba --37620# 900# 80# ms 5 / 2 - # . 8 - ?

153La --47090# 700# > 150 ns 5 /2+# 94Be24 T / 3 - ?

153Ce --55350# 500# > 150 ns 3 / 2 - # 94Be24 T . 8 - ?

153pr --61810# 301)# 4.3 s 0.2 5 / 2 - # 90 / 3 - = 100

153Nd --67352 27 28.9 s 0.4 3 /2 - -# 90 /3--=100

153pm --70688 11 5.250 m 0.017 5 / 2 - 90 87Gr.A T . 8 - = 1 0 0

153Sm --72569.0 2.9 46.27 h 0.01 3/2 + 90 . 8 - =100

153Smm --72470.6 2.9 98.4 0.2 10.6 ms 0.3 1 1 / 2 - 90 IT=100

153Eu --73377.3 2.9 STABLE 5/2 + 90 IS=52.2 15

153Gd --72892.9 3.0 241.6 d 0.2 3 / 2 - 90 e=100

153Tb --71324 5 2.34 d 0.01 5/2 + 90 ,8+=100

153Dy --69153 5 6.4 h 0.1 7 /2 ( - ) 96 f l+~100 ; a=:0.0094 14

153Ho --65023 6 2.02 m 0.03 l l / 2 ( - ) 90 93A103 T .8+~100; a=0.051 25

153Ho m --64954 6 68.7 0.4 9.3 ra 0.5 1/2 + 90 94Xu09 E .8+~100; a=0.18 8

153Er --60460 11 37.1 s 0.2 7/2 ( - ) 94 85Ah.1 J a=53 3; fl+=47 3

153Tin --54001 22 1.48 s 0.01 ( 1 1 / 2 - ) 90 a=91 3; fl+--9 3

153Tm m --53958 22 43.20 0.20 2.5 s 0.2 (1/2 + ) 90 89Ko02 ED a=92 3; .8+=?

153yb --47310# 300# 4.2 s 0.1 ( 7 / 2 - ) 95 88Wi05 D /3+=?; a~=50#; .8+p=0.008 2

153Lu --38480# 600# * 900 ms 200 ( 1 1 / 2 - ) 95 89Ni04 TD /9+=?; a ?

153Lu m --38450# 620# 50# 150# * l / 2 + # fl+ ?

• 153Nd J : (1/2, 3/2, 5/2) in ENSDF suggested by apparent feeding of 3/2 + 450keV level

• 153Ho J : fi'om 87Ne.A

• 153Lu D : p=0% in post cut-off date 97It01

• 153Lun' E : 80(5) keV and p=0% in post cut-off date 97It01

154La --42480# 800# 100# ms . 8 - ?

154Ce --52800# 600# > 150 ns 0 + 94Be24 T . 8 - ?

154pr --58320# 40(0 2.3 s 0.1 (3 + ) 93 96To05 J . 8 - = 1 0 0

INNd --65690 110 25.9 s 0.2 0 + 97 . 8 - =100

154pm --68420 70 * 1.73 m 0.10 (0, 1) 93 . 8 - =100

l~pmm --68370 110 50 130 BD * 2.68 m 0.07 (3 ,4 ) 93 .8--=100

l ~ S m --72465.3 3.0 STABLE 0 + 93 IS=22.7 2; 2 .8- ?

154Eu --71748.0 2.9 8.593 y 0.004 3 - 93 . 8 - ~100; e=0.02 1

154Eu'~ --71602.7 2.9 145.3 0.3 46.3 m 0.4 ( 8 - ) 93 IT=I00

INGd --73716.3 2.9 STABLE 0 + 93 IS=2.18 3

l ~ T b --70150 50 * 21.5 h 0.4 0 93 .8+ ~ 100; . 8 - < 0 . 1

154Tbm --70140 50 12 7 * 9.4 h 0.4 3 - 93 ABBW E /~+=78.2 7; IT=21.8 7; . 8 - < 0 . 1

IMTb" --69950# 160# 200# 150# * 22.7 h 0.5 7 - 93 .8+--98.2 6; IT=I.8 6

154Dy --70400 9 3.0 My 1.5 0 + 96 ot=100; 213 + ?

154Ho --64649 9 11.76 ra 0.19 2 - 93 87Ne.A J .8+~.~I00; or--0.019 5

154Horn --64390 50 260 50 AD 3.10 In 0.14 8 + 93 /3+=100; a<0.001; 1T~,0

154Er --62618 6 3.73 m 0.09 0 + 97 .8+~100; a--0.47 13

154Tin --54560# 110# * 8.1 s 0.3 ( 2 - ) 94 .8+=56 15; o~=44 15

154Tmm --54370 50 200# 120# * 3.30 S 0.07 (9 + ) 94 a=?; .8+=10#

154yb --50080# 100# 409 ms 2 0 + 94 96Pa01 T ~=92.8 20; fl+=7.2 20

154Lu --39960# 500# * & 2# s ( 2 - - ) 97Da07 J .8+ ?

154Lum --39900# 500# 59 9 * & 1.12 s 0.08 (9 + ) 94 97Da07 JE .8+~100; .8+p=?; .8+ol=?; at=0.002#

154Hf --33300# 700# 2 s 1 0 + 94 ff~- ,100; a~,~0

• 154Tbm E : less than 25 keV, from ENSDF

• 154Tmm D : f l + ~ 1 0 % using calculated t~ half-life 30 s, from ENSDF

• l~Tmm D : IT decay has not been observed. Assumed by ENSDF to be negligible

• 154Lu" D : .8+p and .8+ct modes observed by 88Vi02; /3+p confirmed by 90Sh.A


Nuclide Mass excess Excitation Half-life jcr Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

155La --39000# 900# 60# ms 5 /2+# f l - ? 155Ce --48400# 700# > 150 ns 5 / 2 - # 94Be24 T /3 - ? t55pr --55900# 500# 1# s 5 / 2 - # / 3 - ?

155Nd --62760 150 8.9 s 0.2 3 / 2 - # 94 /3 -=100 155pm --66980 30 41.5 s 0.2 ( 5 / 2 - ) 94 /3 -=100 155Sm --70201.2 3.0 22.3 m 0.2 3 / 2 - 94 / 3 - = 100 155Eu --71828.0 2.9 4.7611 y 0.0013 5/2 + 94 /3--=100 155Gd --72080.1 2.9 STABLE 3/2-- 94 IS=14.80 5 155Gdm --71959.1 2.9 121.05 0.19 31.97 ms 0.27 1 1 / 2 - 94 1T=I00 155Tb --71259 12 5.32 d 0.06 3/2 + 94 e=100 155Dy --69164 12 9.9 h 0.2 3 / 2 - 96 /3+ =100 155Ho --66062 23 48 m 1 5/2 + 94 /3+=100 155Er --62220 50 5.3 m 0.3 7 / 2 - 94 /3+ ~100; o~--0.022 7 155Tm --56643 13 21.6 s 0.2 ( 11 / 2 - - ) 95 /3+=98.1 3; tx=l.9 3 155Tm" --56602 14 41 6 45 s 3 (1/2 + ) 95 /3+>92; tr<8 155yb --50490# 300# 1.793 s 0.019 ( 7 / 2 - ) 94 96Pa01 T a=89 4; /3+=11 4 155Lu --42630# 130# * 138 ms 8 (1/2 + ) 94 97Da07 TJD a=76 16;/34 ? 155Lure --42610# 140# 26# 16# * 68.6 ms 1.6 ( 1 1 / 2 - ) 94 T/Daft'/ TD a=88 4;/3+ ?

155Lu" --40830# 140# 1800# 50# 2.696 ms 0.028 ( 2 5 / 2 - ) 94 96Pa01 T tr,-~100; IT ? 155Hf --34690# 600# 890 ms 120 7 / 2 - # 94 /3+=100; a ?

• 155yb T : average 96Pa01=1.80(0.02) 91To08=1.75(0.05) • 155Lu T : average 97Da07=150(24) 96Pa01=136(9) 91To09=140(20) • 155Lum T : average 96Pa01=70(1) 97Da07=63(2) 91To09=-66(7) 79Ho10=70(6) • 155Lu m E : T/Da07=-I9.9(6.2) keV should replace the estimated AME'95=26# in next AME • 155Lu m E : the negative sign means inversion of the (1/2 + ) and the ( 1 1 / 2 - ) levels • 155Lu m D : a : average 97Da07=90(2)% 79Ho10=79(4)% with Birge ratio B=4.4 • 155Lu n T : average 96Pa01=2.71(0.03) 81Ho.A=2.62(0.07) • 155Lu~l E : 96Pa01=1781(2) keV above the ( 1 1 / 2 - ) isomer will become the exact • t55Lu" E : excitation energy after inversion of the (1/2 + ) and the ( 1 1 / 2 - ) levels

156Ce - 4 5 4 0 0 # 800# 150# ms 0 t 156pr - 5 2 0 5 0 # 600# 500# ms 156Nd - 6(B60# 400# 5.47 s 0.11 0 + 92 156pm --64220 40 26.7 s 0.1 4 ( -~ 92 I~Sm --69372 10 9.4 h 0.2 0 + 92 L¢~5 Eu --70094 6 15.19 d 0.08 0 + 92 I~Gd --72545.2 2.9 STABLE 0 + 92 156Tb --70101 5 5.35 d 0.10 3 - 92 156Tb" --70047 6 54 3 24.4 h 1.0 ( 7 - ) 92 156Tb" --70013 5 88.4 0.2 5.3 h 0.2 (0 + ) 92 156Dy --70534 7 STABLE >lEy 0 + 92 156Ho --65470# 200# 56 m 1 4 (+) 92 156Horn --65420# 200# 52.2 0.1 9.5 s 1.5 1 + 92

l ~ E r --64260 70 19.5 m 1.0 0 + 92 t56Tm --56810 60 83.8 s 1.8 2 - 92 156Tm m non existent RN 19 s 3 9 + 156 Yh -- 53240 30 26.1 s 0.7 0 + 92 156Lu --43870# 300# * 494 ms 12 (2#) - 92 156Lure --43550# 340# 320# 170# * 198 ms 2 (9) 4 92 156Hf --37960# 360# 23 ms 1 0 ~ 92 156Ta --26370# 600# 144 ms 24 ( 2 - - ) 156Tam --26290# 600# 82 18 p 360 ms 40 (9 + ) 92

• l ~ T b " E : derived from E3 24h to 4 + 49.630 level and E ( IT )< B(L)=9 keV *156Dy T : lower limit is for a decay *156Hom J : from 87Ne.A, but .1=5 is also possible, see ENSDF *156Hom l : 3 isomers reported in Karlsmhe char~ 1981 and 1995. *156Lum D : derived from original a--98(9)% *156Hf D : derived from original ot=100(6)% * l ~ T a T : supersedes 92Pa05=165(+165-55) from same group *156Ta"~ T : average 96Pa01=375(54) 93Li34=320(80) .156Tam

Not traceable

J : from 93Li34

E : 96Pa01=102(7) keV should replace the preliminary AME'95=82(18) in next AME

58Ri23 T 87Ne.A J 95Ka.A T

9 ITo08 I

96Pa01 TJ 96Pa01 TJD 96Pa01 TD 96Pa01 TJD 96Pa01 TJ

/ 3 - ? / 3 - ? , 8 -=100

/3 -=100 /3-=100 /3-=100 IS=20.47 4 /~=100; /3-- ? IT=IO0

IT=?;/3+=? 1S=0.G6 1; a ?; 2/3 + ? /3+=100 IT=?; /3+ ? /3+=t00 /3+,.~~100; tr---0.064 t0

/3+=90 2; a=10 2 a=?; /3+=5# a=94 6; .B + ?

a=97 3;/3+ ? /3+--95.8 9; p--4.2 9 p~,~,100; /3+ ?


Nuclide Mass excess Excitation Half-life f,r Em Reference Decay modes and intensifies (keV) eeergy(keV ) (%)

157Ce --40670# 900# 50#

157 l:h" --49210# 700# 300#

157Nd --56570# 500# 2#

157pro --62220# 300# 10.56 157Sm --66740 50 8.03

157Eu --69471 6 15.18

157Gd --70833.9 3.0 STABLE

157Tb --70773.8 3.0 71

157Dy --69432 7 8.14

157 Dy" --69233 7 199.38 0.07 21.6

157Ho --66890 50 12.6 m

157Er --63390 80 18.65 m

157Erm --63230 80 155.4 0.3 76 ms

157Tm --58910 110 3.63 m 157yb --53410 50 38,6 s

157Lu --46480 22 6.8 s

157Lu m --46448 22 32.0 2.0 AD 4.79 s

157Hf --39000# 300# 115 ms

157Ta --29670# 600# * 4.3 ms

157Tam --29570# 610# 100# 100# * 1.7 ms .157Nd .157Dym

.157Lu

.157Ta

.157Ta

.157Ta m

ms 7 /2+# ' 8 - .9 ms 5 / 2 - # ' 8 - ?

s 5 / 2 - # 96 ' 8 - .9 s 0.10 ( 5 / 2 - ) 96 '8-=100

m 0.07 (3/2--) 96 ' 8 - =100

h 0.03 5/2 + 96 '8-- =100

3 / 2 - 96 IS=15.65 3

y 7 3/2 + 96 e=100

h 0.1)4 3 / 2 - 96 fl+ =100

ms 1.6 11/2-- 96 IT=100

0.2 7/2-- 96 fl+=100

0.10 3/2-- 96 '8+=100 6 (9/2 + ) 96 IT=100

0.09 1/2 + 96 '8+=100

1.0 7/2 - 96 '8+--99.5; a=0.5

1.8 (1 /2+ ,3 /2 +) 96 fl+ ?; a=? 0.12 ( 1 1 / 2 - ) 96 '8+=?; a---6 2

l 7 / 2 - 96 96Pa01 T a=869 ; ' 8+=149

0.1 1/2+# 96 96Pa01 'I'D a=91 9; ~ ?

0.1 high 96 96Pa01 J a=?; fl+ ? T : a half-life of several seconds has been repotted. See ENSDF

T : as adopted by ENSDF evaluator from 3 inconsistent results

T : ENSDF'96 average of very discrepant 91To09=5.7(0.5) 91Lel5, 92Po14--9.6(8)

D : p=3.4(1.2)% and f i r=l /2+ in post cut-off date 97Ir01 D : derived from original a--95(12)%

E : 22(5) keV, f l r= l l / 2 - - and p=0% in post cut-off date 97Ir01

158pr --44920# 800# 200# ms

158Nd --54150# 600# 700# ms 0 +

158pm --58970# 400# 4.8 s 0.5

158Sm --65220 80 5.30 m 0.03 0 +

158Eu --67210 80 45.9 m 0.2 ( 1 - )

158Gd --70699.9 3.0 STABLE 0 +

158Tb --69479.9 3.0 180 y 11 3 -

158Tbm --69370 3 110.3 1.2 10.70 s 0.17 0 -

158Dy --70417 4 STABLE 0 + 158Ho --66190 30 11.3 m 0.4 5 +

158Ho"~ --66120 30 67.200 0.010 28 m 2 2 -

158Ho" ~66010# 80# 180# 70# 21.3 m 2.3 (9 +)

158Er --65290# 100# 2.29 h 0.06 0 +

158Tm --58690# 120# 3.98 m 0.06 2-- 158Tm m non existent RN 20 s (5 + )

t58yb --56022 10 1.49 m 0.13 0 +

158Lu --47350# 120# 10.6 s 0.3 2--

t58Hf --42250# 100# 2.84 s 0.07 0 +

t58Ta --31330# 510# & 49 ms 8 (2--)

158Ta m --31190# 510# 141 9 & 36.0 ms 0.8 (9 +)

158W --24280# 700# 1.0 ms 0.4 0 +

*158Tm m I : T~20 s in 81Dr07 was a typo. Value in Fig. 2 was conect. See 96Dr.A

*158Hf T : average 96Pa01=2.85(0.07) 73To02=2.8(0.2)

*158Ta T : average 97Da07=72(12) 96Pa01--46(4) with Birge ratio B=2 *158Ta D : derived from original a~100(8)%

*158Tam T : average 97Da07=37.7(1.5) 96Pa01=35(1) 79Ho10=36.8(1.6) .158W T : symmetrized from 0.9(+0.44).3)

'8-- 9

' 8 - ? 96 /3- =100

96 f l - =100

96 ' 8 - =100 96 IS=24.84 12

96 ff~=83.4 7; '8-=16.6 7

96 IT~100; f l - <0.6; '8+ <0.0| 96 IS=0.10 1; a ?; 2'8 + ?

96 '8+ -->93; a ?

96 IT>81; '8+<19

96 '8+ ->93; IT_<7 96 ~=100

96 '8+=100 96Dr.A I

96 '8+~,100; a~,~,0.(1021 12

96 95Ga.A J '8+--99.09 20; a::=0.91 20

96 96Pa01 TD '8+=55 3; a=45 3

96 97Daft'/ TJD a=96 4; ,8 + ?

96 97Daft7 TJE a---93 6; '8+ ?; IT ?

96 96Pa01 T a=100


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

159pr --41700# 90(1# 100# ms 5 / 2 - - # ,8-- ?

159Nd --49940# 7(10# 500# ms 7 /2+# ,8-- ?

159pm --56700# 500# 3# s 5 /2 - -# ,8-- ?

1598m --62220# ~ 11.37 s 0.15 1 5 / 2 - ) 94 /3 - =100

159Eu --66057 8 18.1 m 0.1 5/2 + 94 , 8 - = 1 0 0

159Gd --68571.9 3.0 18.479 h 0.004 3 / 2 - 94 , 8 - = 1 0 0

159Tb --69542.4 3.0 STABLE 3/2 + 94 IS=100.

159Dy --69177 3 144.4 d 0.2 3 / 2 - 94 e=100

159Ho --67339 4 33.05 m 0.11 7/2-- 94 ,8~=100

159Ho m --67133 4 205.91 0.05 8.30 s 0.08 1/2 + 94 rr=lOO

159Er --64570 5 36 m 1 3 / 2 - 94 ,8+=100

159Tin --60730 70 9.13 m 0.16 5/2 + 94 ,8+=100

159yb --55750 90 1.72 m 0.10 5 /21-~ 94 93A103 T ]3+=100

159Lu --49730 50 12,1 s 1.0 1/2~# 94 '8+ ~ 100; a--0.04#

159Hf --42850# 300# 5.20 s 0.10 7 / 2 - # 94 96Pa01 T ,8+=59 5; a=41 5

159"Fa --34550# 120# & 1.04 s 0.09 (1/2 + ) 97Da07 TJD 0"=34 5; ,8+ ?

159Tam --34440# 140# 110# 50# & 514 ms 20 ( 1 1 / 2 - - ) 94 96Pa01 TJ 0"=56 5; ,8+ ?

159W --25820# 600# 8.2 ms 0.7 7 / 2 - # 94 96Pa01 TD 0"=82 16; ,8+ ?

*I59yh T : supet'sodes 80A114=1.40(0.20) from same group

*159Ta T : average 97Da07=0.83(0.18) 96Pa01=l.1010.10)

*159Tam T : average 97Da07=500(111 96Pa01=544(16)

*159Ta m D : average 97Da07=55(1)% 79Ho10=80151%

*159Ta m E : 97Da07=63.7(5.2) keV should replace the estimated AME'95=II0# in next AME

*159W D : derived from original 0:=92(23)%

¢~ag

a g ~

16°Nd --47140# 800#

160pm --53100# 600#

I60Sm --60420# 400#

160Eu --63370# 200#

160Gd --67951.9 3.0

16°Tb --67846.3 3.0

16°Dy --69682 3

160Ho --66392 15

160 Horn --66332 15 59.98 0.03

160Hon --66195 22 197 16

160Er --660611 511

t60Tm --604611 300

160 Tin" --60390 300 711 20

160yb --58160# 211}#

160Lu --50280# 230#

160Lure --50280# 250# 0# 100#

160Hf --45910 30

160Ta --36(100# 310#

160Ta'n --35580# 340# 420# 180#

J60W --29460# 360#

Ir0Rc -- 17250# 61111#

300# ms 0 +

2# s

9.6 s 0.3 0 + 97

38 s 4 I t - ) 97

STABLE > 130Py 0 + 97 95Bu18 T

72.3 d 0.2 3 - 97

STABLE 0 + 97

25.6 m 0.3 5 + 97

5.02 h 0.05 2 - 97

3 s (91 ) 97 ABBW E

28.58 h 0.{';9 0 '~ 97

9.4 m 0.3 1 - 97

74.5 s 1.5 5 I+#) 97

4.8 m 0.2 0 ~ 97

36.1 s 0.3 2 - # 97

40 s 1 97

13.6 s 0.2 0 + 97

1.70 s 0.20 ( 2 # ) -

' 8 - ?

' 8 - ? 3 - =100

3 - =100

IS=21.86 4; 2 /3- ?

3 - = 1 0 0

IS=2.?,4 5

B + =100

IT=65 3; fl+=35 3

1T=llgl

e=100

'8+ =100

IT=85 5; 3+=15 5

3+=100

,8 + = 100; 0" < l.e~[

'8+~,~100; 0" ?

,8+ =99.3 2; o,---41.7 2

96Pa01 TJD ,8+ ?; 0"=?

1.55 s 11.04 (9) 4 97 96Pa01 TJ fl+=66#; a=?

90 ms 5 0 r 97 96Pa01 TD a=87 8; fl+ ?

790 ,u,s 160 ( 2 - - ) 97 92Pa05 J p=91 10; a=9 5

*I60Ho" E : less than 55 keV above 169.55 level, from ENSDF

*160"Fa J : from 0" conelation with 156Lu line

*lr0Tam J : fi'om 0" correlation with 156Lure line

*160W T : avecage 96Pa01=91(5) 81Ho10=81(15)

*160Re J : plx~tons from d3/2 orbital

~t



161Nd --42540# 9(10#

161pm --50430# 700#

161Sm --56980# 500#

161Eu --61780# 300#

161Gd --65516 3

161Tb --67472 3

161Dy --68065 3

161Ho --67206 4

16tHorn --66995 4 211.14 0.03

16t Er --65203 10

16lTm --62041) 90

161yh --57890# 220#

161Lu --52590# 240#

161Lure --52420# 240# 166 18

161Hf --46270 70

161 -lZa -- 38780 50

161W --30660# 310#

161Re --20810# 600#

161 Rein --20810# 630# 0# 200#

200# ms 1 / 2 - # / 3 - ?

700# ms 5 / 2 - # /3-- ?

3# s 7 /2+# / 3 - ?

26 s 3 5/2 +# 90 /3--=100

3.646 m 0.003 5/2 - 90 941LA T /~ - =100

6.88 d 0.03 3/2 + 90 /3 -=100

STABLE 5/2 + 90 1S=18.9 1

2.48 h 0.05 7 / 2 - 90 e=i00

6.76 s 0.07 1/2 + 90 rr=lOO

3.21 h 0.03 3 / 2 - 90 /3+=100

30.2 m 0.8 7/2 + 90 93A103 T /3+=100

4.2 m 0.2 3/2-- 90 /3+=100

77 s 2 1/2 (+) 90 92Bo.A J fl+=100

7.3 ms 0.4 ( 9 / 2 - - ) 90 ABBW E IT=I00

* &

* & 14 ms 2 11/2--# 90 96Pa01 T

18.7 s 0.1 3 / 2 - # 90 95Hi12 TD fl+~,100; a=0.30 5

2.89 s 0.14 1 /2+# 90 92Hal0 T fl+=95#; a=?

409 ms 16 7 / 2 - - # 90 96Pa01 TD a=73 3;/3+=27 3

1 /2+# p ?

a=100

*161Lu m E : less than K binding energy (61 keV) above 135.8 level, from ENSDF

*161Ta T : average 92Ha10=3.00(0.15) 86Ru05=2.7(0.2)

*I61W T : average 96Pa01=409(18) 79H010=410(40)

*161Re T : 370(40) ,us, f ' r = l / 2 + and p=100(7)% in post cut-off date 971v01

*161Rem E : 123.8(1.3) keV. T=16(1) ms, J~r= l l /2 - - and p-~,.8(6)% in post cut-off date 971r01

162pm --46310# 800#

162Sm --54750# 600#

162Eu --58650# 400#

162Gd --64291 5

162Tb --65680 40

162Dy --68190 3

162H0 --66050 4

162Ho m --65944 8 106 7

162Er -- 66~'~,6 4

162Tm --61510 30

162Tm m --61410 30 96 17

162yb --59850# 210#

162Lu --52890# 220#

162Lum --52770# 300# 120# 200#

162Lu" --52590# 300# ?d)0# 200#

162Hf --49180 II

162Ta --39920# 130#

162W --34150# 100#

162Re --22630# 510#

162Rein --22460# 510# 172 8

162Os --15070# 700#

*162Er T : lower limit is for a decay

500# ms

2# s

10.6 s 1.0

8.4 m 0.2

7.60 m 0.15

STABLE

15.0 m 1.0

67.0 m 0.7

/ 3 - ?

o + / 3 - ? 91 f l - =100

0 + 91 / 3 - =100

1 - 91 f l--=100

0 + 91 IS=25.5 2

1 + 91 fl+=lO0 6-- 91 IT=62; /3+=38

IS=0.14 1; ot ?; 216 + ?

fl+=100

1T=82 4; ,/3+=18 4

/3+=100

/3 + =100

/3+~100; IT ?

/ /+~100; IT ?

0 + 94 95Hi12 TD f f ~ 1 0 0 ; or=0,008 1

3~-# 91 f l+~100; a---0.073 14

0 + 91 fl+ ?; ct=47 3

( 2 - ) 97Da07 TJD a - - ~ 6; /3+ ?

(9 + ) 91 97Da07 ETJ a=91 5; /3+ ?

0 + 91 96Bi07 T tr=100

STABLE > 140Ty 0 + 91 56P016 T

21.70 m 0.19 1 - 91

24.3 s 1.7 5 + 91 ABBW E

18.87 m 0.19 0 + 91

1.37 m 0.02 1 ( - ) 91 92Bo.A J

1.5 m 4 - # 91

1.9 m 91

39.4 s 0.9

3.52 s 0.12

1.39 s 0.04

& 107 ms 13

& 76 ms 9

1.7 ms 0.5

* 162Tmm E : above 66.90 level and less than 125 keV, from ENSDF

*162Hf T : average 95Hi12=39.8(0.4) 82S¢15=37.6(0.8)

,162Re" T : average 96Pa01=66(7) 97Da07=84.6(6.2)

*162Ren' D : average 96Pa01=85(9)% 97Da07=94(6)%

*162Os T : average 96Bi07=1.5(+0.7-0.5) 89Ho12=1.9(0.7)


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

163pm --43300# 900# 200# ms 5 / 2 - # / 3 - ?

163Sm --50900# 700# 1# s 1 / 2 - # / 3 - ?

163Eu --566.'30# 500# 6# s 5 /2+# / 3 - ?

163Gd --61490# 300# 68 s 3 7 /2+# 97 f l - =100

163Tb --64605 5 19.5 m 0.3 3/2 + 97 fl-- =100

163Dy --66390 3 STABLE 5/2-- 97 IS=24.9 2

163Ho --66387 3 4.570 ky 0.025 7 / 2 - 97 e=100

163Ho m --66089 3 297.88 0.07 1.09 s 0.03 1/2 + 97 88Ka20 T IT= 100

163Er --65177 5 75.0 m 0.4 5 / 2 - 97 ,8+=100

163Tin --62738 6 1.810 h 0.005 1/2 + 97 /3+=100

163yb --59370 100 11.05 m 0.25 3 / 2 - 97 /3+=100

163Lu --54770 220 238 s 8 1/2 C+) 97 92Bo.A J /3+=100

163Hf --49320# 320# 40 s 6 3 / 2 - # 97 95Hi12 D /3+=100; a<0.0001

163Ta --42550 70 l l . 0 s 0.8 5 /2 - - # 97 /3+ ~ 100; ot ~0 .2

163W --34900# 310# 2.75 s 0.25 3 /2 - -# 97 /3+=59 5; t~=41 5

163Re --26111}# 110# 390 ms 70 (1/2 + ) 97Da07 TJD 0t=32 3;/3 + ?

163Re m --25940# 140# 170# 70# 214 ms 5 ( 1 1 / 2 - - ) 97 97Da07 TD a--66 4; /3+ ?

163Os --16720# 600# 5.5 ms 0.6 7 /2 - - # 97 96Bi07 TD a~.~100; /3+ ?; f l+p ?

*163Lu J : positive parity from 92Sc03

*163Rem E : 97Da07=115.1(4.0) keV should replace the estimated AME'95=I70# in next AME

*163Re m T : also 96Pa01=219(23) J : from 96Pa01

m *

m *

I64Sm - 4 8 1 8 0 # 800#

164Eu --53100# 600#

164Gd --59750# 400#

164Tb --62090 100

164Dy --65977 3

164Ho --64990 3

164Horn --64850 3 140.0 0.1

164Er --65953 3

164Tm --61990 19

164Tmm --61980 20 10 6

t64yb - 6 0 9 9 0 # 100#

164Lu --54760# 130#

t64Hf --51770# 200#

164Ta --43250# 400#

164W --38210 HI

164Re --27650# 310#

164Os --20560# 360# 1641r

*164Hom T : symmetrized from 37.5(+1.5-0.5)

* 164Tram E : less than 20 keV, from ENSDF

500# ms 0 +

2# s

45 s 3 0 + 92

3.0 m 0.1 (5 + ) 92

STABLE 0 + 92

29 m 1 1 + 92

38.0 m 1.0 6 -- 92

STABLE 0 + 92

2.0 m 0.1 1 + 92

5.1 m 0.1 6-- 92 ABBW E

75.8 m 1.7 0 + 92

3.14 m 0.03 1 ( - ) 94 92Bo.A J

111 s 8 0 + 92

14.2 s 0.3 (3 + ) 96

6.4 s 0.8 0 + 92

530 ms 230 (2#) - 92 96Pa01 TJ

21 ms 1 0 +" 92 96Pa01 T

1# ms

*164Re T : average 96Pa01=380(160) 81Ho10=880(240)

.164Rc J : from a correlation with 160Ta line

/ 3 - ?

/ 3 - ? / 3 - =100

/ 3 - =100

IS=28.2 2

e=60 5 ; / 3 - = 4 0 5

IT=100

IS=I.61 2; a ?; 2/3 + ?

/3+=100

ITs80 ; /3+ ~ 2 0

E=I00

fl+=100

/3+=100

/3+=100

/3+=97.4 17; o,=2.6 17

o'~,-~58; /3+ ,-~.42

a=?;/3+ =2#

p ?; ct ?

G. Audi etal./Nuclear Physics A 624 (1997) 1-124 7 9

Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

165Sm --43800# 900# 165Eu --50560# 700# 165Gd --56470# 500# 165Tb --60660# 200#

165Dy --63621 3 165 Dy'n --63513 3 108.160 0.003 165Ho --64907.3 3.0 165Er --64531 3 165Tm --62939 4 165yb --60177 20 165Lu --56260 80 165Lu m --56260# 130# 0# 100# 165Hf --51660# 370# 165Ta --45810# 220# 165W --38810 90 165Re --30790# 120# 165 Rem --30690 70 100# 100# 165Os --21910# 310# 165Ir -- 11570# 40O# l~6Irn~ --11570# 410# 230# 110#

EU *

200# ms 5 / 2 - # , 8 - ? 1# s 5 /2+# , 8 - ?

10# s 1 / 2 - # , 8 - ? 2.11 m 0.10 (3/2 + ) 92 /9 -=100

2.334 h 0.001 7/2 + 92 ' 8 - = 1 0 0 1.257 m 0.006 1 / 2 - 92 IT--97.76 11; ' 8 -=2 .24 11

STABLE 7/2-- 92 IS=100. 10.36 h 0.04 5 / 2 - 92 e=100 30.06 h 0.03 1/2 + 92 '8+=100

9.9 m 0.3 5 / 2 - 92 '8+=100 10.74 m 0.10 (7/2 + ) 92 ,8+=100

12 m 1/2 + 92 ,8+ ? 76 s 4 ( 5 / 2 - - ) 92 ,8+=100

31.0 s 1.5 5 / 2 - # 92 ,8+=100 5.1 s 0.5 3 / 2 - # 92 ,8+~100; or<0.2

* & 1# s low# ~ ?; ot ? * & 2.00 s 0.27 11/2- -# 92 96Pa01 T ,8+=87 3; ot=13 3

71.2 ms 2.8 ( 7 / 2 - - ) 92 97Da07 J a>60; '8+ <40 < 1# #s 1 /2+# 97Da07 T p ?; o~ ? 300 .us 60 ( 1 1 / 2 - - ) 97Da07 TJD p=87 4; a=13 4

*I65Lu"~ 1 : existence is discussed in ENSDF. Provisionally accepted *165Re E : the mass in AME'95 was -30690(70) keV, see remark for the isomer. *165Re D : one a decay event has been observed in post cut-off date 97Po.B

*165Rem T : average 96Pa01=1.9(0.3) 81Ho10=2.4(0.6) *165Rem I : this state is the one which was assumed to be the ground-state in AME'95 *165Rem E : 78(57) keV in post cut-off date 97Po.B *16SOs T : average 96Pa01=71(3) 91Se01=73(8)

166Eu --46600# 800# 166Gd --54400# 600# 166Tb --57710# 300# 166Dy --62593 3 166Ho --63079.6 3.0 166Horn --63074 3 5.985 0.018 166Er --64934.5 2.9 166Tm --61895 11 166Tm"~ --61773 14 122 8 t66yb --61591 8 166Lu --56110 160 166Lum --56080 160 34.37 0.05 166Lun --56070 160 42.9 0.5 166Hf --53790# 300# 166Ta --46140# 300# 166W --41899 12 166Re --31860# 140# 166Rem --31860# 240# 0# 200# 166Os --25590# 100# 1661r -- 13500# 510# 1661rm --13330# 510# 172 6 166pt

* &

* & 2 . 5 s 0.2 216 ms 9 10.5 ms 2.2 15.1 ms 0.9 300 las 100

400# ms ' 8 - ? 7# s 0 + B - ? 21 s 6 94Ts.A TD ,8 - = 100

81,6 h 0.1 0 + 92 , 8 - = 100 26.83 h 0.02 0 - 92 , 8 - MOO 1.20 ky 0.18 ( 7 ) - 92 , 8 - = 100

STABLE 0 + 92 1S=33.6 2 7.70 h 0.03 2 + 92 ,8+=100 340 ms 25 6-- 96DtO'/ TJE IT=I00 56.7 h 0.1 0 + 92 e=100 2.65 m 0.10 6 ( - ) 92 92Bo.A J ,8+=100 1.41 m 0.10 3 ( - ) 92 92Bo.A J e=58 5; IT=42 5 2.12 m 0.10 ( 0 - ) 92 ,8+>80; IT<20 6.77 m 0.30 0 + 92 ,8+=100 34.4 s 0.5 (2) + 92 /3+=100 18.8 s 0.4 0 + 92 '8+~,.~100; 0,---0.035 12 2# s low# fl+ ?; ot ?

6+# 92 92Mo10 T fl+ ?; a=5 2 0 + 92 96Pa01 T a=72 13; '8+=28 13

( 2 - ) 92 97Da07 TJD 0,--93 3; p=7 3 (9 + ) 97Da07 TJD a=98.2 6; p=l.8 6 0 + 96Bi07 "I'D a=100

*166Tmm E : less than 25 keV above 109.34 level *166Rein T : average 92Me10=2.3(0.2) 84Sc06=2.8(0.3) *166Rem D : ot intensity is derived from 2% < ot < 8% as discussed in ENSDF -166Os T : average 96Pa01=220(7) 91Se01=194(17) .1661r T : 96Pa01=12(1) ms is probably a mixture of both isomers, not used .166Irm E : fi'ora 97Da07=171.5(6.1) keV

g t *

,,i¢ ,,It



167Eu --43730# 900# 200# ms 5 /2+# , 8 - ?

167Gd --50700# 600# 3# s 5 / 2 - # ' 8 - ?

167Tb - 5 5 8 4 0 # 400# 15# s 3 /2+# ' 8 - ?

167Dy - 5 9 9 4 0 60 6.20 m 0.08 ( 1 / 2 - ) 90 ' 8 - = 1 0 0

167He -62293 6 3.1 h 0.1 7 / 2 - 90 ' 8 - =100

167Er --63299.2 2.9 STABLE 7/2 + 90 IS=22.95 15

167Erm --63091.4 2.9 207.802 0.005 2.269 s 0.006 1 / 2 - 90 IT=I00

167Tin --62551 3 9.25 d 0.02 1/2 ~- 90 e=100

167yh --60597 5 17.5 m 0.2 5 / 2 - 90 '8+=100

167Lu --57470 100 51.5 m 1.0 7/2 + 90 '8+=100

167Hf --53470# 210# 2.05 m 0.05 ( 5 / 2 - ) 90 '8+=100

167Ta --48460# 430# 1.4 m 0.3 5 / 2 - # 90 '8+=100

167W --42220# 310# 19.9 s 0.5 3 / 2 - # 90 '8+ ?; ct=?

167Re --34870# 130# * & 3.4 s 0.4 9 / 2 - # 92Me10 TD a~,~100; 8 + ?

167Rein --34720 90 150# 100# * & 6.1 s 0.2 1/2+# 90 '8+,~,99.3; a-~,0.7

!67Os --26500# 310# 810 ms 60 3 / 2 - # 90 96Pa01 T a=67 9; '8+=33 9

I67Ir --17190# 100# 35.2 ms 2.0 11/2 + ) 90 97Da07 TJD t~=486 ;p=324 ; ' 8~ -?

167Ir" --16970# 140# 220# 90# 30.0 ms 0.6 ( 1 1 / 2 - ) 97Da07 TJD or=80 10; '8+ ?; p--0.4 1

167pt 700 bts 200 7 / 2 - # 96Bi07 T ct=100

• 167Ta J : lowest observed state by 92Th02 is 3/2 +

• 167W J : lowest observed state by 92Th06 is 13/2 +

• 167Os T : avmage 96Pa01=840170) 82En03=800(200) and 77Ca23=650(150)

• 167hm~ E : 97Da07=175.3(2.2) keV should replace the estimated AME'95=220# in next AME : , l t~

168Gd --48100# 700# ~ ms 0 ~ 8 - ?

168Tb --52500# 500# 6# s /3-- ?

168Dy --58470# 300# 8.7 m 0.3 0 + 94 ' 8 - = 1 0 0

168H0 --60085 29 2.99 m 0.07 3 + 94 ' 8 - = 1 0 0

168Hem --60026 29 59 1 132 s 4 (6 ~) 94 90Ch37 E IT~I00; ' 8 - <0.5

168Er - 6 2 9 9 9 . 0 2.9 STABLE 0 + 94 IS=26.8 2

168Tm --61320 3 93.1 d 0.2 3 t 94 ' 8 ~ 1 0 0 ; /3---0.010 7

168yb --61577 4 STABLE >130Ty 0 + 94 56P016 T IS=0.13 1; o~ ?; 2fl + ?

168Lu --57100 80 * 5.5 m 0.1 6 ( - ) 94 92Bo.A J '8+=100

168Lure --56880 t00 220 130 BD * 6.7 m 0.4 3 ~ 94 /3+>95; IT<5

168Hf --55300# 100# 25.95 m 0.20 0 + 94 fl+ =100

168Ta --48640# 370# 2.0 m 0.1 1 2 - , 3 + ) 94 /5'+=100

168W --44840# 200# 51 s 2 0 ~ 94 8+~,~100; ct=0.0032 10

168Re --35760# 400# 4.4 s 13.1 1 5 + , 6 + , 7 + ) 94 '8+~100; a~0 .005

168Rem non existent RN 6.6 s 1.5 92Me10 I

168Os --29960 30 2.06 s 0.06 0 + 94 96Pa01 T '8~-=51 3; a=49 3

168Ir --18660# 330# 125 ms 40 low 94 96Pa01 TJ a=?; '8+ ?

168Irn' -- 18600# 350# 60# 120# 161 ms 2l high 94 96Pa01 TJD ct=82 14

168pt --11150# 360# 2.0 ms 0.4 0 ~- 94 96Bi07 T a=?; '8+ ?

• 168yb T : lower limit is for a decay

• 168Os T : average 96Pa01=2.1(0.1) 84Sc06=2.0(0.2) 82En03=2.2(0.1) 78Ca11=1.9(0.1)

• 168Os T : 84Sc06 supersedes 78Sc26=2.410.2) from same group



169Gd --43900# 800# 169Tb --50100# 600# 169Dy --55610

|69Ho --58807 20 169Er --60930.8 2.9 169Tm --61281.9 2.9 169yb --60373 4 169 ybm --60349 4 24.199 0.003 t69Lu --58080 5 169 Lure --58051 5 29.0 0.5 169Hf --54810 80 169Ta --50380# 210# 169W --44940# 320# 169Re --38350# 210# 169Rem --38200# 220# 150# 70# t690s --30670 90 169Ir --22090# 130# 169Irm --21990 90 100# 100# t69pt -- 12650# 310#

1# s 7 / 2 - # 2# s 3 /2+# 39 s 8 ( 5 / 2 - ) 91 4.7 m 0.1 7 / 2 - 91

9.40 d 0.02 1 / 2 - 91 STABLE 1/2 + 91 32.026 d 0.005 7 /2 + 91

46 s 2 1/2-- 91 34.06 h 0.05 7/2 + 91

160 s 10 1/2-- 91 3.24 m 0.04 ( 5 / 2 ) - 91 4.9 m 0.4 ( 5 / 2 - - ) 91 76 s 6 ( 5 / 2 - - ) 91

, 8 - ? , 8 - ? ,8--=100 3 - -=100 /3-- =100 IS=IO0. ~=100 IT=IO0

,8+=100 IT=100

,8+=100 ,8+=100 ,8+=100

8.1 s 0.5 9 / 2 - # 91 92Me10 TD ,8+=?; a=0.005 3 15.1 s 1.6 1/2+# 91 92Me10 TD ,8+ ?; a te0.2 3.46 s 0.11 3 / 2 - # 91 96Pa01 T fl+=89 1; o,=11 t

* & 200# ms low# a ?; 15 '+ ? * & 308 ms 22 1 1 / 2 - # 91 96Pa01 TD ct=72 13; fl+=28 13

3.7 ms 1.5 3 / 2 - # 91 %Pa01 T a=?; fl+ ? *169Re D : a----'0.005(3)% dadved from original a--0.001% - 0.01% *169Rem T : average 92Me10=16.3(0.8) 84Sc06=12.9(1.1) ,169Os T : average 96Pa01=3.6(0.2) 95Hi02=3.2(0.3) 84Sc06=3.5(0.2) 82En03=3.4(0.2) *1691r E : the mass in AME'95 was -21990(90) keV. see remark for the isomer. *169Ir I : a=50(+40-24)% T=0.64(+0.46-0.24) s in post cut-off date 97Po.B *169Irm I : this state is the one which was assumed to be the ground-state in AME'95 *t69hm I : E=182(56) keV, ot=84(+16-21)% / '--323(+90-66) ms in post cut-off date 97Po.B *169pt T : average 96Pa01=5(3) 81Ho10=2.5(+2.5-1.0)

tT°Tb --46340# 700# 17°Dy --53400# 400# 170Ho --56250 50 * 170Ho nj --56150 60 I00 80 BD * 170Er --60118 3

170Tm --59803.9 2.9 170yb --60771.9 2.9 ITOLu --57313 19 170Lu m --57220 19 92.89 0.09 170Hf --56220# 200# 170"lh --50220# 200# 170W --47240# 470# 170Re --38970# 400# 170Os --33935 13 t70lr --23260# 180# 170lrm --23260# 210# 0# 100# 170pt -- 16460# 100#

• lTOIrm J : fi'om a correlation with 166Re* line • 17°pt D : ,8+ intensity is estimated by 96Ak.A

3# s , 8 - ? 30# s 0 + , 8 - ?

2.76 m 0.05 (6 + ) 96 , 8 - = 100 43 s 2 ( 1 + ) 96 , 8 - =100

STABLE 0 + 96 IS=14.9 2; 2 ,8 - ?; a ?

128.6 d 0.3 1 - 96 f l - ,~,100; e=0.131 10 STABLE 0 + 96 IS=3.05 6

2.012 d 0.020 0 + 96 fl+ =100 670 ms 100 ( 4 ) - 96 IT=I00

16.01 h 0.13 0 + 96 e=lO0 6.76 m 0.06 (3 + ) 96 ,8+=100 2.42 m 0.04 0 + 96 ,8+ ~,~-, 100; a < l # 9.2 s 0.2 (5 + ) 96 fl+ ~ 100; a<0.01# 7.3 s 0.2 0 + 96 96Pa01 D /3+=?; a=8.6 6

* & 830 ms 300 low 96 96Pa01 TJD fl+ ?; ot=36 10 * & 1.05 s 0.15 high 96Pa01 JD ~=?; ,8+ ?

14.7 ms 0.5 0 + 96 96Bi07 T or=?;/3+=2#

17tTb --43500# 800# 171Dy --49850# 500# lTIHo --54530 600 171Er --57729 3 171Tm --59219.0 2.9 17lyb --59315.4 2.8

171Ybm --59220.1 2.8 95.272 0.005 . . . A-group is continued on next p a g e . . .

500# ms 3 /2+# fl-- ? 6# s 7 / 2 - - # ,8-- ? 53 s 2 ( 7 / 2 - - ) 92 ,8--=100

7.516 h 0.002 5/2-- 92 fl-- =100 1.92 y 0.01 1/2 + 92 /3--=100

STABLE 1/2-- 92 IS= 14.3 2 5.25 ms 0.24 7/2 + 92 IT=I00


Nuclide Mass excess Excitation Half-life j~r Ens Reference Decay modes and intensities (keV) energy(keV) ( % )

. . . A-group continued . . . 171Lu --57837 3 8.24 d 0.03 7/2 + 92 /3~ =100 171 Lure --57766 3 71.2 0.2 79 s 2 1 / 2 - 92 IT=I00

I71Hf --55430# 200# * 12.1 h 0.4 (7/2 + ) 92 /3+=100 171Hl~r --55380# 210# 50# 50# * 29.5 s 0.9 1 / 2 - # 95Ca.A TD IT=I00 171"pa --51740# 210# 23.3 m 0,3 ( 5 / 2 - ) 92 /3+=100 171W --471180# 280# 2.38 m 0.04 ( 5 / 2 - ) 92 /3+=100 171Re --41410# 340# 15.2 s 0.4 ( 9 / 2 - ) 92 /3+=100

17108 --34430# 310# 8.3 s 0.2 ( 5 / 2 - ) 92 95Hi02 TD /3+---98.3 3; ct=l.8 2 1711r --26290# 130# 1.52 s 0.08 ( 1 1 / 2 - ) 92 96Pa01 TD ot=58 11; /3+-~12 11 171pt -- 17470# 310# 38 ms 5 3 / 2 - # 92 %Pa01 T 0t~99; /3+ ~ 1 171Au --7660# 250# 10 /zs 1/2+# 97Da07 T p=?; o~ ? 171Aura --7360# 140# 300# 200# 1.02 ms 0.10 ( 1 1 / 2 - ) 97Da07 TJD a=54 4; p=46 4

• 171Os D : average 95Hi02=1.9(0.3)% 79Ha10=1.7(0.3)% ,171ir T : average 96Pa01=1.3(0.2) 78Sc26=1.610.1) 78Ca11=1.4(0.2) J : from 92Sc16 • 171pt T : average 96Pa01=4313) 96Uu. l=25(+ l lqS) 82En03=20(6) and 81De22-~10(10) • 171Aum E : 97Da07 derives/5"--100-260 keV fi'om experiment. Thus, E=180(50) keV should ,171Au m E : replace the estimated AME'95=300# in Next AME

t72Dy --47400# 600# -~ s 0 + / 3 - ? 172Ho --51400# 400# 25 s 3 95 /3 -=100 172Er --56493 5 49.3 h 0.3 0 + 95 /3 -=100 172Tin --57384 6 63.6 h 0.2 2 - 95 /3 -=100 172yb --59263.8 2.8 STABLE 0 + 95 IS=21.9 3 172Lu --56745 3 6.70 d 0.03 4 - 95 /~+ =100 172Lure --56703 3 41.86 0.04 3.7 m 0.5 1 - 95 IT=I00 172Hf --56390 50 1.87 y 0.03 0 ~ 95 e=100 172Ta --51470 190 36.8 m 0.3 (3 + ) 95 /3+=100 172W --48980# 270# 6.6 m 0.9 0 + 95 /3+=100

172Re --41650# 310# * 15 s 3 (5) 95 /3+=100 172Rein --41650# 370# 0# 200# * 55 s 5 (2) 95 /3~=t110 172Os --37190# 200# 19.2 s 0.9 0 ~ 95 95Hi02 D /3+=?;ot=l.l 2 1721r --27350# 400# 4.4 s 0.3 (3 + ) 95 /3+---98; a=2 1721r'n --27210# 400# 139 10 AD 2.0 s 0.1 (7 + ) 95 /3+=77 3; a=23 3 172pt --21070 30 98 ms 4 0 + 95 96Pa01 T a=77 21; /3+ ? 172Au --9210# 330# 4.7 ms 1.1 high 95 96Pa01 TJ a=?; p<2

• t72pt T : average 96Pa01=96(3) 82En03=90(10) 81De22=120(10) 75Ga25=100110) • 172pt D : derived from original a=94132)% • 172Au T : average 96Pa01=6.3(1.5) 93Se09--4(1) • 172Au J : from a correlation with 1681tin line

173Dy --43370# 700# 2# s 9 /2+# /3 - ? 173Ho --49100# 400# 10# s 7 / 2 - # / 3 - ? 173Er --53650# 200# 1.434 m 0.017 ( 7 / 2 - - ) 95 94It.A T /3 -=100 173Tin --56262 5 8.24 h 0.08 (1/2 + ) 95 /3 -=100 173yb --57560.0 2.8 STABLE 5/2-- 95 IS=16.12 21 173Lu --56889.2 2.8 1.37 y 0.01 7/2 + 95 e=100 173Hf --55280# 100# 23.6 h 0.1 1 / 2 - 95 /3+=100 173Ta --52590# 230# 3.14 h 0.13 5 / 2 - 95 /3+=100 173W --48590# 380# 7.6 m 0.2 5 / 2 - 95 134 =100 173Re --43720# 450# 1.98 m 0.26 ( 5 / 2 - ) 95 /3+=100 173Os --37450# 310# 22.4 s 0.9 ( 5 / 2 - ) 95 95Hi02 TD /3+~100; or=0.4 2 1731r --30080# 230# * 9.0 s 0.8 ( 3 / 2 + , 5 / 2 + ) 95 /3+>93; ct<7 1731rm --29980# 210# 100# 100# * 2.20 s 0.05 1 1 1 / 2 - ) 95 /3+=88 1; a=12 1 173pt --21890 100 363 ms 14 5 / 2 - # 95 96Pa01 T 0t=84 6; /3+=16 6 173Au -- 12870# 140# * & 10# ms low# a ?; /3+ ? I73Aum -- 12670 100 200# 100# * & 15 ms 2 l l / 2 # 95 96Pa01 T or=?;/3+=4#

• 173pt T : average 96Pa01=376(11) 82En03=360(20) and 81De22=325(20) • 173Au E : the mass in AME'95 was -12670(100) keV, see remark for the isomer. • I73Au I : ct---94(+6~2)% T=19.5(+9.0--6.0) ms in post cut-off date 97Po.B ,173 Aum I : this state is the one which was assumed to be the ground-state in AME'95 • 173Aum I : E=243(55) keV, ot--92(+8-27)% 7"--121+3-2) ms in post cut-off date 97Po.B

, , g *



174Ho - 4 5 5 0 0 # 500# t74Er --51850# 300# 174Tm --53870 40 174yb --56953.3 2.8 174Lu --55579.0 2.8 174Lure --55408.2 2.8 170.83 0.05 174Hf --55852 3 174Ta --52010 80 174W --50150# 300# 174Re --43680# 410# 174Os --39940# 470# 174Ir --30920# 400# 174Irm --30730# 400# 193 11 AD 174pt --25326 13 174Au -- 14050# 150# 174Hg 2.7 ms 1.3 0 +

*174W T : is ENSDF'S average of 4 results; see also 90Me12=35.3(0.5) *174Os D : symmetfized from a- -0 .020(+10~)%

*174pt T : average 96Pa01=890(20) 82En03--900(10) *174Au T : average 96Pa01=171(29) 83Sc24=120(20) *174Hg T : symmetrized from 2.1(+1.8-0.71

8# s 8 - ? 3.3 m 0.2 0 + 91 f l - =100 5.4 m 0.1 ( 4 ) - 91 /3 - =100

STABLE 0 + 96 IS=31.8 4 3.31 y 0.05 I - 96 92Bo.A J ,8+=100 142 d 2 6 - 96 92Bo.A J IT=99.38 2; e=0.62 2 2.0 Py 0.4 0 + 96 IS=0.162 3; a=100; 2/3 + ? 1.05 h 0.03 3 (+) 91 ,8+=100 31 m 1 0 + 96 ,8+=10(/

2.40 m 0.04 91 ,8+=100 44 s 4 0 ÷ 96 ,8+~100; a=0.024 7 9 s 2 (3 + ) 91 92Sc16 T ,8+=99.5 3; a--0.5 3

4.9 s 0.3 (7 + ) 92Sc16 T ,8+~100; ot--0.47 27

898 ms 9 0 + 91 96Pa01 T a=83 5; ,8+=17 5 136 ms 23 low 91 96Pa01 TJ tr=?;/3'+ ?

96Uu.I TD a=100

175Ho --42800# 600# 175Er --48500# 400# 175Tm --52320 50 175yb --54704.3 2.8 175ybm --54189.4 2.8 514.869 0.007 175Lu --55174.3 2.6 175Hf --54490 3 175Ta --52490# 10(1# 175W --49580# 200# t75Re --45280# 450# 175Os --39980# 300# 1751r --33270# 340# 175pt --25830# 310# 175Au --17190# 240# * 175Au m --17090# 130# 100# 200# * 175Hg --8000# 320#

• 175Au T : average 96Pa01=185(30) 83Sc24=200(22) • 175Aum T : erroneously 200 ms in AME'95. Was correct in AME'93 • 175Hg T : avel'age 96Uu.1=13(+6-4) 96Pa01=8(8)

5# s 7 / 2 - # 1 .2 m 0 . 3 9 / 2 + #

15.2 m 0.5 (1/2 + ) 93 96Zh03 J 4.185 d 0.001 7 / 2 - 93 68.2 ms 0.3 I/2 - 93

STABLE 7/2 + 93 70 d 2 5/2 - 93

10.5 h 0.2 7/2 + 93 35.2 m 0.6 ( 1 / 2 - ) 93 5.89 m 0.05 ( 5 / 2 - ) 93 1.4 m 0.1 ( 5 / 2 - ) 93 9 s 2 ( 5 / 2 - ) 93

2.52 s 0.08 5 / 2 - # 93 195 ms 18 1 1 / 2 - # 93 96Pa01 T

5/2 + # 12 ms 4 5 / 2 - - # 93 96Uu.l T D : symmetrized from a--94(+6-2.5)%

1 3 - 7 96Zh03 TD ,8--=100

,8--=100 ,8--=100 IT=I00 IS=97.41 2 e=lO0 ,8+=100 ,8+=100 ,8+=100 ,8+=100 ,8+--99.15 28; ot=0.85 28 ,~--64 5; fl~ ? at=82 17; fl+ ?

a ?; ,8+ ? a=lO0

176Er --46310# 400# 176Tm --49380 100 176yb --53497.2 2.9 176ybm --52447.2 2.9 1050.0 0.3 176Lu --53391.0 2.6 176Lu m --53268.1 2.6 122.855 0.006 176Hf --54583.8 2.7 176Ta --51470 11)0 176Tam --51370 100 103.0 1.0 176Ta" --48650 110 2820 50 176W --50680# 200# 176Re --45110# 200# 176Os --41960# 200# 1761r --33990# 300# 176pt --28880# 200# 176Au -- 18380# 400# 176Hg -- 1 t720 40

20# s 0 + ,8-- ? 1.85 m 0.03 (4 + ) 90 94It.A T ,8-- =100

STABLE 0 + 96 IS=12.7 2; 2,8-- ?; a ? 11.4 s 0.3 ( 8 - ) 96 1T> 90; , 8 - < 1 0 37.8 Gy 0.2 7-- 96 IS=2.59 2; , 8 - = 100

3.635 h 0.003 1-- 96 91KI02 E ,8--~,100; ~---0.095 16 STABLE 0 + 96 IS=5.206 5

8.09 h 0.05 ( l ) - - 90 ~ - =100 l . l ms 0.1 (+) 90 IT=100 1.4 ms 0.1 20-- 94Dal 1 TE IT=100 2.5 h 0.1 0 + 96 e=100 5.3 m 0.3 3 (+) 90 ,8+=100 3.6 m 0.5 0 + 90 fl+=100 8 s 1 90 ,8+--97.9 4; a=2.1 4

6.33 s 0.15 0 + 90 ~ ?; a=38 3 1.25 s 0.30 90 or=?; ,8+=40# 25 ms 9 0 + 90 96Pa01 T a=?; f l+=l.4#

*176Ta" E : 2772 + x, from 94Dal l and x estimated 50(50) by NUBASE *176Hg ' T : average 96Pa01=18(10) 83Se24=34(+18-9); 20.5(+4.7-3.6) in post cut-off date 97Po.B * 176Hg D : ,8 + intensity is estimated by 96Ak.A; or=94(+6-27)% in post cut-off date 97Po.B

* m

* m

alt

act


Nuclide Mass excess Excitation Half-life J~ Ees Reference Decay modes and intensities (keV) energy(keV ) (%)

177Er --42500# 600# ~ s 1 / 2 - # / 3 - ?

177Tm --47470# 300# 82 s 13 (1/2 + ) 93 / 3 - =100

177yb --50993 3 1.911 h 0.003 (9/2 + ) 93 / 3 - = 100

177yhm --50662 3 331.5 0.3 6.41 s 0.03 (1/2 ) 93 IT=I00

177Lu --52391.9 2.6 6.734 d 0.012 7/2 + 93 /3-- =100

177Lu m --51421.7 2.6 970.1749 0.0025 160.4 d 0.3 2 3 / 2 - 93 fl--=78.3 6; IT=21.7 6

177Hf --52890.2 2.5 STABLE 7/2-- 93 IS= 18.606 4

177H1 ~t --51574.7 2.5 1315.4502 0.0011 1.08 s 0.06 23/2 + 93 1T=100

177Hf~J --50150.2 2.5 2740.0 0.2 51.4 m 0.5 3 7 / 2 - 93 1T=I00

177Ta --51724 4 56.56 h 0.06 7/2 '~ 93 /3+=100

177W --49720# 300# 135 m 3 ( 1 / 2 - - ) 93 /3+=100

]77Re --46320# 200# 14 m 1 ( 5 / 2 - ) 93 /3+=100

177Os --41880# 280# 2.8 m 0.3 ( 1 / 2 - ) 93 /3+=100

177Ir --36170# 450# 30 s 2 ( 5 / 2 - - ) 93 /3+~100; a--0.06 1

177pt --29390# 310# 10.0 s 0.4 ( 5 / 2 - - ) 93 93Me13 T /3+--94.4 4; a=5.6 4

177Au --2122(1# 230# 1.18 s 0.07 5 /2 - -# 93 /3+>60; a _ 4 0

177Hg --12730 110 130 ms 5 5 / 2 - # 93 a=85; fl+=15

177T1 --2910# 230# < 1 p.s 1/2+# 96Da.A D p=?; a ?

177Tlm --2210# 380# 700# 300# 9 / 2 - # p ?; ot ?

*177Tm T : symmetrized from 85(+10-15)

*177pt T : average 93Me13--9.8(0.4) 82Bo04=11(1)

*177T1 I : not found by 91Se01, setting an upper limit of 1 microsecond on half-life

*177TI I : p=27(+19-14)% with 7"--17(+6-4) ms and tr=73(+14-19)%, in post cut-off date 97Po.B

*177TI n' I : E=836(54) keV, p=51(8)% with T=230(+41-33)us and a=49(8)%, in

*177TIm 1 : post cut-off date 97Po.B

178Tm --44120# 400# 30# s f l - ?

178yb --49701 10 74 m 3 0 + 94 /3-- =100

178Lu --50346 3 28.4 m 0.2 1 (+1 94 /3--=100

178Lun~ --50222 4 123.7 2.6 RQ 23.1 m 0.3 9 ( - I 94 92Bo.A J /3 - =100

178Hf --52445.2 2.5 STABLE 0 + 94 IS=27.297 4

178H1~1 --51297.8 2.5 1147.423 0.005 4.0 s 0.2 8 - 94 IT=t00

178Hl ~r --49999.5 2.5 2445.69 0.11 31 y 1 16 + 94 94Ki.A E IT=100

178Ta --50530 I(i0 * 9.31 m 0.03 1 + 94 /3+=100

178Tan' --50533 10 0 100 BD * 2.36 h 0.08 ( 7 ) - 94 /3+=100

178Tan --49060 100 1470 100 59 ms 3 (15 - - ) 94 96Ko13 T IT=I00

t78W --50440 100 21.6 d 0.3 0 r 94 e=100

178Re --45780 210 13.2 m 0.2 (3 + ) 94 fl+=100

178Os --43460 200 5.0 m 0.4 0 + 94 /3+=100

1781r --36250# 360# 12 s 2 95 /3+=100

t78pt --31940# 470# 21.1 s 0.6 0 ~" 94 /3+--'92.3 3; oe=7.7 3

178Au --22380# 400# 2.6 s 0.5 94 /3+--<60; a > 4 0

178Hg --16323 15 268 ms 15 0 + 94 96Pa01 T a=?; /3+ =~'~#

178T1 --4450# 210# 60# ms a ?; /3+ ?

• 178Ta m E : 140(90) keV derived from new data on masses. To be changed in next AME

• 178Tan E : 1470.6 keV above 178Tam, from ENSDF. Should become E=1610(90) in next AME

• 178Tan T : average 96Ko13=58(4) 79Du02=60(5)

• 178TalZ E : 3 isomers ate known above the ga'ound-state. The third one is ( 2 1 - ) , 290(12) ms at

• 178Ta" E : 2902 keV above the ( 7 ) - isomer, all from 96Ko13.

• 178Hg T : average 96Pa01=287(23) 91Se01=250(25) and 79Ha10=260(30)

• 178Hg D : /3+ intensity is estimated by 96AEA


Nuclide Mass excess Excitation Half-life j,n- Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

179Tm --41600# 500# 20# s 1/2+# / 3 - ?

179yb --46420# 300# 8.0 m 0.4 1 1 / 2 - ) 94 f l - = 1 0 0

179Lu --49067 6 4.59 h 0.06 7/2 (+1 94 /3--=100

179Lure --48475 6 592.4 0.4 3.1 ms 0.9 1/2 (+) 94 IT=I00

179Hf --50472.9 2.5 STAaLE 9/2 + 94 1S=13.629 6

179Ht~' --50097.9 2.5 375.0367 0.0025 18.67 s 0.04 1/2-- 94 IT=I00

179Ht~ --49367.1 2.5 1105.84 0.19 25.05 d 0.25 2 5 / 2 - 94 IT=I00

179"1~a --50362 6 1.82 y 0.03 7/2 + 94 e=100

179Tan~ --49044 6 1318.0 0.4 9.0 ms 0.2 (25/2 + ) 94 IT=100

179Tan --47721 6 2640.9 0.6 52 ms 3 (37/2 + ) 94 IT=I00

179W --49302 16 37.05 m 0.16 ( 7 / 2 ) - 94 /3+=100

179W" --49080 16 221.926 0.008 6.40 m 0,07 11/2)-- 94 1T~I00; /3+--0.28 3

179Re --46590 50 19.5 m 0.1 (5/2) + 95 /3+=100

179Os --42890# 230# 6.5 m 0.3 1 1 / 2 - ) 94 fl+=100

179Ir --38050# 400# 79 s 1 ( 5 / 2 ) - 95 /3+=100

179pt --32160# 300# 21.2 s 0.4 1 / 2 - 94 fl+,~,100; a--0.24 3

179Au --24770# .MO# 7.1 s 0.3 5 / 2 - # 94 fl+=78.0 9; a=22.0 9

179Hg --16970# 310# 1.09 s 0.04 5 / 2 - # 94 ot~,-~53; fl+=?; f l+p~0.15

179T1 --7950# 140# 190 ms 70 (1/2 + ) 94 ABBW J a ~ 1 0 0 ; f l + ?

179Tln' --7400# 2411# 560# 210# 1.1 ms 0.4 ( 9 / 2 - ) 94 96Pa01 T a,~100; IT ?

*179T1 T : symmetrized from 160(+90-40) J : fi'om a decay to 175Aura

*179Tlm T : aver'age 96Pa01=0.7(+0.641.4) 83Sc24=1.4(0.5)

gt

180yb --44400# 400# 2.4 m 0.5 0 + 94 f l - = 1 0 0

180Lu --46690 70 5.7 m 0.1 5 ~ 94 95Me03 J / 3 -=100

180Lu'~l --46680 70 13.9 0.3 1 s 3-- 95Me03 EJT IT ?

180Hf --49789.5 2.5 STABLE 0 + 94 IS=35.100 7

180Hfm --48648.0 2.5 1141.48 0.04 5.5 h 0.1 8 - 94 IT~,-~,100; /3 -=0 .3 1

180Ta --48935 3 8.152 h 0.006 1 + 94 e=86 3; , 6 - =14 3

180Tam --48860.3 2.9 75.2 1.3 RQ STABLE >l .2Py 9 - 94 1S=0.012 2

180W --49643 5 STABLE > l . lPy 0 + 94 IS=0,120 1; a ?; 2/3 + ? *

180Win --48114 5 1529.04 0.03 5.47 ms 0.09 8 - 94 IT= 100

180Re --458411 31) 2.44 m 0.06 ( 1 ) - 94 /3+=100

180Os --44390# 180# 21.5 m 0.4 0 + 94 /3+=100

1801r --37960# 190# 1.5 m 0.1 (4, 5) + 94 fl+=l{~0

180pt --34270# 200# 52 s 3 0 + 94 /3+~100; a ~ 0 . 3

180Au --25710# 300# 8.1 s 0.3 94 /3+<98.2; a > l . 8

tSOHg --20190# 200# 2.56 s 0.02 0 + 94 93Wa03 T /3+=52 4; 0t--48 4

180T1 --9140# 450# 720 ms 110 94 o,--75#; /3+=25#; f l+SF~l.(~e-4 *

180pb 5 ms 3 0 + 96To08 TD a=100 *

• lS0w T : lower limit is for a decay **

• ISOTI T : symmetrized from 700(+120-90) **

• tSOpb T : symmetrized from 4 (+4 -2 ) **


Nuclide Mass excess Excitation Half-life J~ Eas Reference Decay modes and intensities (keV) energy(keV) (%)

181yb --40850# 400# 1# m 3 / 2 - # /3-- ?

181Lu --44740# ~ 3.5 m 0.3 (7/2 + ) 91 / 3 - = 100

181Hf --47413.9 2.6 42.39 d 0.06 1 / 2 - 91 / 3 - =100

181Ta --48441.1 2.9 STABLE 7/2 + 92 1S--99.988 2

181W --48253 5 121.2 d 0.2 9/2 + 91 e=100

181Re --46515 14 19.9 h 0.7 5/2 + 91 /3+=100

tSIOs --43520 200 105 m 3 1 / 2 - 92 /3+ =100

181Os" --43470 200 48.9 11.2 2.7 m 0.i ( 7 / 2 ) - 92 95Ro09 E /3~'=100

1811r --39460 210 4.90 m 0.15 ( 5 / 2 ) - 93 /3+=100

181pt --34300# 280# 51 s 5 1 / 2 - 93 95Bi01 D /3+~100; 0,--0.074 10

181Au --27990# 450# 14.5 s 0.4 ( 3 / 2 - ) 92 95Bi0l TJD /3+=?; a=2.7 5

181Hg --20670# 310# 3.6 s 0.3 1/2 ~ - I 92 72Ho18 D /3+=64 4; 0,=36 4; . . .

181TI --12200# 380# 3.4 s 0.6 1/2+# 91 92Bo.D TD a = ? ; f l + ?

181Tlm --11600# 430# 600# 200# EU 2.7 ms 1.0 9 /2 - - # 84Sc.A T c~=?;/3 + ?

181pb --3060# 160# & 45 ms 20 5 /2 - -# 96To01 T 0t=?;/3+=2#

181pbm non existent RN & 13/2+# 91 96To01 I

*181Au T : in agreement with 79Ha10=13(31, but differing noticeably from earlier

*lSIAu T : 68Si01=11.5(1.0) and 68De01=11.3(0.71

*lSIHg D : . . . ; /3+p=0.014 4; /3+ct=9e~6 3 D : /3+p from 72Ho18; /3+a from 75Ho02

*181Tlm I : not confirmed by 96To01. Provisionally accepted

*lSIpb T : supersedes 89To01=50(+40-30) from same group

*181pbm 1 : proved by 96To01 not to exist

182Lu --41720# 300# 2.0 m 0,2 (0, 1,2) 95 / 3 - =100

182Hf --46060 7 9 My 2 0 + 95 / 3 - =100

182Hfnt --44887 7 1172.88 0.18 61.5 m 1,5 8 - 95 / 3 - = 5 8 3; IT=42 3

182Ta --46432.7 2.9 114.43 d 0,03 3 - 95 / 3 - =100

182Tam --46416.4 2.9 16.263 0.003 283 ms 3 5 + 95 IT=I00

182Ta° --45913.1 2.9 519.572 0.018 15.84 m 0.1(I 1 0 - 95 IT=I00

182W --48246.2 2.9 STABLE 0 + 95 IS=26.498 29

182Re --45450 100 * 64.0 h 0.5 7 ~ 95 /3+=100

182Re m --45386 20 60 100 BD * 12.7 h 0.2 2 + 95 /3+=100

182Os --44538 25 22.10 h 0.25 0 + 95 e=100

182Ir --39000 140 15 m 1 (3 ~ ) 95 95Sa42 J /3+=100

182pt --36080 200 2.2 m 0.1 0 + 95 /3+~,100; 0t---0.038 2

182Au --28300# 360# 15.5 s 0.4 5+# 95 95Bi01 T /3+~100; a---0.13 5

182Hg --23520# 470# 10.83 s 0.06 0 + 95 71Ho07 D /3+=84.8 8; ct=15.2 8; /3+p<le-5

182T1 --1_~100# 400# * 2.0 s 0.3 2 - -# 95 92Bo.D T /3+>96; or<4

182Tim --13300# 410# t00# 100# * 2.9 s 0.5 (7 + ) 91Bo22 TJ ot.~,100; /3+ ?

182pb --6822 17 60 ms 40 0 + 95 oL=?; /3+=2#

• 182Au T : average 95Bi0t=14.5(l .3)(for /3+), 15.3(l.01(for a ) and 92Ro21=15.6(0.4)

• 182Hg D : and ot=13.3(0.5)% in post cut-off date 97Ba21

• 182TI m T : average 91Bo22=3.1(1.0) 92Bo.D=2.8(0.6)

• 182pb T : symmetrized from 55(+40-35) D : /3+ intensity is estimated by 96Ak.A



183Lu --39520# 300# 58 s 4 (7/2 + ) 91 /9-=100 183Hf --43290 30 1.067 h 0.017 ( 3 / 2 - ) 91 /9 -=100

183Ta --45295.6 2.9 5.1 d 0.1 7/2 + 91 /9 -=100

183W --46365.6 2.7 STABLE > l l 0 P y 1 / 2 - 93 IS=14.314 4

183Win --46056.1 2.7 309.500 0.003 5.20 S 0.06 11/2 + 93 IT=100

183Re --45810 8 70.0 d 1.4 5/2 + 91 e=100

183Re m --43902 8 1907.6 0.3 1.04 ms 0.05 (25/2 + ) 91 IT=I00

183Os --43680# 100# 13.0 h 0.5 9 /2 + 91 fl+ =100

)83Os m --43510# 100# 170.71 0.05 9.9 h 0.3 1 / 2 - 91 /9+=85 2; IT=15 2

183Ir --40230# 140# 58 m 5 5 / 2 - 91 61Di04 T fl+~,100;, a=0.05#

183pt --35650# 230# 6.5 m 1.0 1 / 2 - 93 95Bi01 D f l+~100 ; a=0.0096 5

183ptm --35620# 230# 34.50 0.08 43 s 5 ( 7 / 2 ) - 93 fl+,~100; ct<4e-4; 1T ?

183Au --30160# 400# 42.7 s 1.2 5 / 2 - 91 95Bi01 TD /9+~100; a--0.8 2

183Hg --23700# 300# 9.4 s 0.7 1 / 2 - 95 /8+=74.5 15; ot=25.5 15; . . .

183Hg" --23460# 300# 240# 40# 5# s 13/2+# /9+ ?

183T1 --16120# 390# 6.9 s 0.7 (1/2 + ) 91 92Bo.D T ,B+=?;ot=2#

183T1 m -- 15660# 380# 460# 100# 60 ms 15 ( 9 / 2 - - ) 91 a<0.01; IT ?

183pb --7520# 310# * 300 ms 80 ( 1 / 2 - ) 91 a ~ 9 4 ; / 9 + , ' ~ 6

183pbm --7450# 310# 70# 40# EU * 500# ms 13/2+# 89To01 D a=?; fl+ ? • 1831r T : average 61Di04=55(7) 61La05=60(6)

• 183Au T : average 95Bi01-~14.6(1.9) 70Ma24=42.0(1.2) J : from 94Pa37

• 183Hg D : . . . ; /9+p=5.6e-4. 8 D : /9+p in ENSDF adopted data set is not correct

• 183pbm D : Tentative assignment (of. AME'95) for the 6781 ot line

* m

184Lu --36170# 400# 20 s 3 (3 + ) 90 95Kr04 TJ /9--=100

184Lure non existent RN 20 s high 95Kr04 I

184Hf --41500 40 4.12 h 0.05 0 + 90 /9 -=100

184Hf°' --40230 40 1272.4 0.4 48 s 10 8 - 95Kr04 TE /9 -=100

184Ta --42840 26 8.7 h 0.1 (5 - - ) 90 / 9 - =100

184W --45706.0 2.7 STABLE > 300Py 0 + 90 IS=30.642 8

I84Re --44223 5 38.0 d 0.5 3 ( - ) 90 fl+=100

184Rein --44035 5 188.01 0.04 169 d 8 8 (+) 90 IT=75.4 l l ; e=24.6 11

184Os --44254.5 3.0 STABLE >56Ty 0 + 90 IS=0.020 3; a ?; 2/9 + ?

184Ir --39690 270 3.09 h 0.03 5-- 90 /9+=100

184pt --37360# 180# 17.3 m 0.2 0 + 90 95Bi01 D f l+~100; tr--0.0017 7

184ptm --35520# 180# 1839.4 1.6 1.01 ms 0.05 8-- 90 IT=I00

)g4Au --30_'*,00# 190# & 12 s 2 5 + 90Ed01 TD /9+=100 184Aum --30230# 190# 68.6 0.1 & 49.9 s 2.4 2 + 90 94Ib01 El fl+=?; IT=30 10; et--0.013 3

184Hg --26180# 200# 30.6 s 0.3 0 + 90 fl+--98.89 6; ot=l . l l 6

184T1 --16990# 300# * 10# s 2 - # fl+ ?

184Tlm --16890# 310# 100# 100# * 9.7 s 0.6 7 + 92Bo.D T ,8+---9"/.9 7; a=2.1 7

184pb --10990# 200# 550 ms 60 0 + 90 ct=?; fl+ ? • 184Os T : lower limit is for a decay

• 184Au J : from 94Ib01 T : post cut-off date 97Za03=21(1)

• 184Aum T : average 95Bi01=45.8(1.8) 72Fi12=53.0(1.4) 70Ha18--47(3)

• 184Aum D : IT intensity is from 93Ro.B; at intensity from 95Bi01

• 184Aum T : post cut-off date 97Za03=48(1)

* m

,~g ,gt


Nuclide Mass excess Excitation Half-life f i r Ees Reference Decay modes and intensities ( keV ) energy ( keY ) ( % )

t85Hf --38400# 300# 3.5 m 0.6 3 / 2 - # 95 , 8 -=100

185Ta --41396 14 49.4 m 1.5 7 /2+# 95 / 3 -=100

185W --43388.4 2.8 75.1 d 0.3 3 / 2 - 95 / 3 -=100

185WJ" --43191.0 2.8 197.43 0.115 1.597 ra 0.004 11/2 ~ 95 941t.A T IT=100

185Re --43821.4 2.8 STABLE 5/2 + 95 IS=37.40 2

185Os --42808.6 2.8 93.6 d 0.5 1/2 95 e=100

1851r --40440# 200# 14.4 h 0.1 5 / 2 - 95 /3+=100

185pt --36560 210 70.9 m 2.4 (9/2 + ) 95 /3~ ~100; a--0.0050 20 *

t85pt" --36460 210 103.4 0.2 33.0 m 0.8 ( 1 / 2 - ) 95 /3~=?; IT<2

185Au --31850 210 4.25 ra 0.06 5 / 2 - 95 /3+ ~10(I; a--0.26 6

185Au m non existent RN 6.8 m 0.3 1 1 / 2 - # 95 77Bo.A I /3+<100; IT ?

185Hg --26100# 280# 49.1 s 1.0 1 / 2 - 95 /3+=94 1; or=6 1

185Hgm --26000# 280# 103.8 1.0 21.6 s 1.5 13/24" 95 87Ki.A E 1T=54 10; /8+=46 10; a ~ 0 . 0 3 *

185T1 --19470# 400# 19.5 s 0.5 I / 2 + # 95 /3+=?; a ?

185T1 m --19020# 400# 452.8 2.0 1.83 s 0.12 9 / 2 - # 95 77Sc03 E IT~I00 ; a=0.10 3; /3 + ?

185pb --11570# 310# * 4. l s 0.3 1/2 # 95 a~,-~,100; ,8+ ?

185pbm --11510# 310# 60# 40# * 6.1 s 1.1 13/2+# 80Sc09 T a~.~100; /34 ?

185Bi --2140# 230# * 2# ms 9 / 2 - # 96Da06 J p ?; ot ? *

185Bi m --2040# 200# 100# 100# * 44 /zs 16 (1/2 + ) 96Da06 TJD p=?; at ?

*185pt D : if the 4444110) keV a line is from ground-state; otherwise o,---0.0111014)% from isomer

*185Hgm E : ENSDF gives 99.3(0.5) plus "8-keV uncertainty", but missed 87Ki.A work

.585Bi T : estimated from 9 / 2 - isomers in odd Bi and TI isotopes

I86Hf --36400# 3110# 5# m 0 + / 3 - ?

186"pa --38610 60 10.39 m 0.03 2, 3 89 941t.A T /3 =t00

186W --42511.3 2.9 STABLE >590Py I) + 89 95Da.3 T IS=28.426 37; 2 ,8 - ?; at ? *

186Re --41929.8 2.8 3.7183 d 0.001l 1 ( - 5 89 94Sc39 T /3---93.1 2:~r=6.9 2

186Rem --41780 4(1 150 40 200 ky 50 (8 ~) 89 IT=?; / 3 - < 1 0

186Os --42999.3 2.9 2.0 Py 1.1 0 + 89 IS=1.58 10; o'=100

5861r --39168 20 • 16.64 h 0.03 5 + 89 /3+=100

586Ir" --39167 20 0.8 0.4 * 1.92 h 0.05 2 - 89 91Be25 ET /3 ~ ~100; 1T ? *

186pI --37790 30 2.08 h 0.05 0 + 89 91Be25 T /3+=100; a .~ l . 4e~ - *

186Au --316711 140 10.7 m 0.5 3 - 89 95Bi01 D /3~ =100; ot--0.0008 2

186Aura non existent RN < 2 m 83Po10 1

186Hg --28450 200 1.38 m 0.10 0 ~ 89 /3+ ~100; o'---0.016 5

186Tr --19981)# 370# * > 20 S ( 2 - - ) 89 771j01 TD /3+ ?; o'--0.006 2 *

t86TIm --198811# 370# 1 1 ~ 50# * 27.5 s 1.0 7 + 89 /3+=100

186T1" --19510# 370# 470# 50# 2.9 s 0.2 1 0 - 91Va04 T IT=I00 *

186pb --14620# 470# 4.82 s 0.03 05 89 94Wa23 T a=? ; /3 t --44# *

186Bi --3280# 450# * 3# ms 3 ~ # a ?; /3~ ? *

186Bim --3030# 430# 250# 250# * 10 ms 4 10 84Sc.A TD or=?;/3~ ? •

• 186W T : lower limit is for 2 /3 - decay **

• 186h'm T : average 91Be25=1.90(0.05) 70Fi.A=2.0(0.1) **

• 186pt T : average 91Be25=2.10(0.05) 72Fi12=2.0(0.1) **

• 186T1 J : from 91Va04 **

• 186Tln E : 373.9(0.5) keV above 186Tlm, from 91Va04 **

• I86ph T : average 94Wa23=4.83(0.03) 80Sc09=4.79(0.05) **

• 186pb D : ,8+ intensity is estimated by 96Ak.A **

• t86pb D : post-cut-off date 97An.l o'=501251% and 97Ba25 oz-=45(201% **

• 186Bi T : 15.11(1.7) ms for tr decay in post cut-off date 97Ba2.1 **

• 186Bi" T : 9.8(1.3) ms lbr o" decay in post cut-off date 97Ba21 **


Nuclide Mass excess Excitation Half-life . f f Ens Reference Decay modes and intensities (keV) energy(keV) (%)

89

187Ta --36880# 300# 2# m 7 /2+# , 8 - ? 187W --39906.7 2.9 23.72 h 0.06 3 / 2 - 92 fl--=lO0 187Re --41217.9 2.8 43.5 Gy 1.3 5/2 + 91 IS--62.60 2; ,8 -=100; ,~<0.0001

187Os --41220.5 2.8 STABLE 1/2-- 92 IS=1.6 1 187Ir --39718 7 10.5 h 0.3 3/2 + 91 ,8+=100 187 lt'm --39532 7 186.15 0.04 30.3 ms 0.6 9 / 2 - 91 IT= 100 187pt --36740# 180# 2.35 h 0.03 3 / 2 - 91 /3+=100 187Au --33010# 150# 8.4 m 0.3 1/2 + 91 ,8+~100; a=0.003#

¿87Aura --32890# 150# 120.51 0.16 2.3 s 0.1 9 / 2 - 91 IT=I00 187Hg --28150# 240# * & 1.9 m 0.3 3 / 2 - 91 ,8+=100; a > l . 2 e ~ . 187Hg'n --28050# 230# 100# 70# * & 2.4 m 0.3 13/2 + 91 ,/3+=100; a>2 .5e-4 187T1 --22200# 400# 51 s (1/2 + ) 91 /3 +<100; a ? 187T1" --21870# 400# 332 4 AD 15.60 s 0.12 ( 9 / 2 - ) 91 IT=?; a=?; /3 + ? 187pb --14880# ~ * & 15.2 s 0.3 ( 3 / 2 - - ) 91 95La10 J f l+=? ; a=? 187pbm --14820# 300# 60# 40# * & 18.3 s 0.3 (13/2 + ) 91 ,8+=98.0; o~=2.0 187Bi --6090# 380# * 35 ms 4 9 / 2 - # 94 or>50; ,8+ ? 187Bi m --5940# 390# 150# 100# * 0.8 ms 0.6 1/2+# a > 5 0 ; f l + ?

188Ta --33800# 300# 188W --38669 4 188Re --39018.1 2.8 188Rein --38846.0 2.8 172.069 0.009 188Os --41138.5 2.8 188Ir --38329 7 188Irar --37360 30 970 30 188pt --37823 6 188Au --32520# 100# 188Hg --30220# 180# 188T1 --224.',0# 220# 188T1 m --22330# 230# 100# 50# 188T1" --22060# 230# 370# 50# 188pb --17640# 200# 188Bi --7290# 300# 188Bim --7100# 3_30# 190# 150#

20# s . 8 - ? 69.4 d 0.5 0 + 90 , 8 - =100 16.98 h 0.02 1 - 90 , 8 - =100 18.6 m 0.1 ( 6 ) - 90 1T= 100

STABLE 0 + 90 IS=13.3 2 41.5 h 0.5 1 - 90 /3 + =100 4.2 ms 0.2 7+# 90 ABBW E IT~I00 ; ,8+ ? 10.2 d 0.3 0 + 90 e=100; ot=2.6e-5 3 8.84 m 0.06 1 ( - ) 96 /3+=100 3.25 m 0.15 0 + 96 ,8+=100; a=3.7e-5 8

• 71 s 2 ( 2 - ) 90 ,8+=100 • 71 s 1 (7 + ) 90 ,8+=100

41 ms 4 ( 9 - ) 90 IT~100; /6 .+ ? 25.5 s 0.1 0 + 96 92Wa14 T fl+=?; a~=8.5 13

• & 44 ms 3 3+# 90 a=?;,8+ ? • & 210 ms 90 (10- - ) 90 or=?;,8 + ?

* 1881rm E : less than 100 keV above 923.5 level, from ENSDF *188Tln E : 268.8(0.5) keV above 188Tim, from 91Va04

*188pb D : ot intensity is from 96Bi17 *188Bi T : post cut-off date 97Wa05--46(7) *188Bim T : post cut-off date 97Wa05=218(50)

189W --35480 200 11.5 m 0.3 ( 3 / 2 - - ) 91 ,8--=100 189Re --37979 9 24.3 h 0.4 5/2 + 91 13--=1(10 189Os --38987.8 2.8 STABLE 3/2-- 91 IS=16.1 3 189Os m --38957.0 2.8 30.814 0.018 5.8 h 0.1 9 /2-- 91 IT= 100 1891r --38455 13 13.2 d 0.1 3/2 + 91 e=100 189 h~'n --38083 13 372.18 0.04 13.3 ms 0.3 11/2-- 91 IT= 100 189ha~ --36122 13 2333.3 0.4 3.7 ms 0.2 (25/2) + 91 IT=I00 189 Pt -- 36485 11 10.87 h 0.12 3/2-- 92 ,8+ =100 189Au --33640# 200# 28.7 m 0.3 1/2 + 92 fl+=100; ot<3e-5

189Aura --33390# 200# 247.23 0.17 4.59 m 0.11 1 1 / 2 - 92 f l+~100 ;1T=? 189Hg --29690# 280# * 7.6 m 0.1 3 / 2 - 96 /3+=100; a< 3e - 5 189Hgm --29570# 290# 120# 80# * 8.6 m 0.1 13/2 + 96 fl+=100; a< 3e - 5 189T1 --24510# 350# 2.3 m 0.2 (1/2 +) 91 ,8+=100 189Tlm --24230# 350# 283 6 AD 1.4 m 0.1 9/2 ( - ) 91 85Bo46 J ,8+~-~100; IT<4

189pb --17810# 270# * & l# m 3 / 2 - # ,8+ ? 189pbm --17720# 280# 90# 60# * & 51 s 3 13/2 + 91 ABBW J ,8+ >99; a ~ 0 . 4 189Bi --9780# 400# 680 ms 30 ( 9 / 2 - - ) 91 95Ba75 J a > 5 0 ; f l + < 5 0 189Bim --9560# 400# 217 25 AD 7.0 ms 0.2 (1/2 + ) 91 95Ba75 TJ a>50; /5'+<50

* 189W T : 11.7(0.5) m in post cut-off date 97Ya03 *189pbm J : fi'om a decay to 185Hgm

*189Bi T : post cut-off date 97Wa05=728(401 ms *189Bim T : post cut-off date 97An.1=4.8(0.5) and 97Wa05=5.2(0.61 and E=182(8)keV from 97Wa05

#t


Nuclide Mass excess Excitation Half-life j-n- Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

190W - 3 4 3 0 0 220 30.0 m 1.5 0 + 90 /3 -=100

Xg0Rc --35570 210 3.l m 0.3 ( 2 ) - 90 /3 -=100

190Rein --35360 220 210 50 3.2 h 0.2 ( 6 - ) 90 95Au04 E /3-=54.4 20; 1T=45.6 20

19°Os --38708.0 2.8 STABLE 0 + 90 IS=26.4 4

190Osm --37002.6 2.8 1705.4 0.2 9.9 m 0.1 (10)-- 90 IT=I00

1901r --36710 2(10 11.78 d 0.10 ( 4 - ) 96 96Ga30 J ~+=100

]90lrn' --36680 200 26.1 0.1 1.120 h 0.003 ( 1 - ) 96 90Ga30 ETJ IT=f00

190It" --36330 200 376.4 0.1 3.087 h 0.012 ( l l ) - 96 96Ga30 ETD /3+=91.4 2; IT=8.6 2

190pt --37325 6 650 Gy 30 0 + 96 IS--0.01 l; tr=100; 213 + ?

190Au --32883 16 * 42.8 m 1.0 I - 90 /34=100; or< le~6

190Aura --32680# 150# 200# 150# * 125 ms 20 (11 - - ) 90 IT~I00 ; /3+ ?

190Hg --31410# 150# 20.0 m 0.5 0 + 96 /3+=100; a< 5e - 5

lg0TI --24410# 430# * 2.6 m 0.3 (2)-- 90 fl I- =100

190Tl" --24240# 340# 1711 500 BD * 3.7 m 0.3 (7 + ) 90 /3+=lffl

l ~ p b - 2 0 3 3 0 200 1.183 m 0.017 0 + 90 96Ri12 T 13+=99.1 2; a--0.9 2

190Bi --10700# 370# 6.3 s 0.1 (3 + ) 90 91Va04 DJ a=77 21; /3+=?

190Bi'n -- 10490# 370# 210# 50# 6.2 s 0.1 ( 111- ) 90 91Va04 DJ a=70 9; /3+=30 9

190po --4560# 470# 1.7 ms 0.8 0 t 96Ba35 T a~,100; /~;--0.1#

• lqOpb D : see also 92Wa14 a=0.40(0.04)%

• PJOBi D : symmetrized from a=90(+10-301%

• lgOPo T : symmetrized from 2.0(+0.5-1.0) D : fl+ intensity is estimated by 96Ak.A

• lg0Po T : and post cut-off date Of/An.l=1.9(+0.6-0.4) and 97Ba25=2.4(+0.4-0.3)

191Re --,34350 II 9.8 m 0.5 (3/2 + , I /2 + ) 95 , 8 - = 100

19lOs --36395.4 2.8 15.4 d 0.1 9 / 2 - 95 /3 -=100

191osm --36321.0 2.8 74.382 0.003 13.10 h 0.05 3/2-- 95 IT=I00

1911r --36709.1 2.9 STABLE 3/2 + 95 IS=37.3 5

191 lrm --36537.8 2.9 171.24 0.05 4.94 s 0.03 11/2-- 95 lT=100

1911rn --34590 40 2120 40 5.5 S 0.7 95 ABBW E IT= 100

191Pt --35691 5 2.802 d 0.025 3 / 2 - 96 ~=100

191Au --33860 50 3.18 h 0108 3/2 + 95 /3+=100

101Au m --33590 50 266.2 0.5 920 ms 110 ( 1 1 / 2 - ) 95 IT=100

t91Hg --30680 90 49 m 10 3/2 ( - I 95 86U102 J fl+=100

191Hgm --30540# 100# 140# 50# 50.8 m 1.5 13/2 + 95 /3+=100

191TI --26190# 220# 20# m ( I / 2 + ) 95 fl+ ?

19IT1 m --25890# 220# 297 7 BD 5.22 m 0.16 9/2 ( _ ) 95 /3+=100

191pb --20310# 21(1# * 1.33 m 0.08 ( 3 / 2 - - ) 95 f l+~100; a=0.013 5

191pbm --20220# 220# 90# 60# * 2.18 m 0.08 13/2 t+) 95 88Me.A J ,8+,~100; a ~ 0 . 0 2

191Bi --12990# 4(}0# 12 s 1 ( 9 / 2 - - ) 95 o,=60 20; /3+--40 20

191Bi n, -- 12750# 400# 242 7 AD I50 ms 15 (1/2 + ) 95 ot=75 25; /3 + ~ 2 5

191po --4980# 300# 17 ms 5 3 / 2 - # 95 ct~,-~100; fl+ ?

• 1911rn E : estimated less than 150 keV above 2047.1 level, from ENSDF

.191Po T : symmetn'ized from 15.5(+6-3.5); post cut-off date 97Ba25=27(+22-8)


Nuclide Mass excess Excitation Half-life J~ Ens Reference Decay modes and intensities (keV) energy(keV) (%)

192Re --31710# 200#

192Os --35882 3

192Os m --33867 3 2015.39 0.10

192Ir --34835.8 2.9

192Ifm --34779.1 2.9 56.74 0.09

192hJ~ --34680.6 2.9 155.16 0.12

192pt --36296 3

192Au --32779 16

192Au m --32644 16 135.4 0.3

192 Au" --32347 16 431.6 0.5

192Hg --32070# 280#

192TI --25950# 200#

192Tlm --25790# 210# 160 50

192pb --22580# 180#

192Bi -- 13630# 220#

192Bi m -- 13420# 230# 210# 50#

192po --7900# 200#

*192Os T : lower limit is for 0~,-2/3-- decay

16 s 1 91 / 3 - =100

STABLE >9.8Ty 0 + 91 IS--41.0 3; 2/3-- ?: a ?

5.9 s 0.1 ( 1 0 - ) 91 IT>87; /3- -<13

73.831 d 0.008 4 (+7 91 /3-=95.24 4; ,~--4.76 4

1.45 m 0.05 1 ( - ) 91 I T ~ 100; /3---0.0175

241 y 9 (9 + ) 91 91KeZZ J IT=I00

STABLE 0 + 91 IS=0.79 6

4.94 h 0.09 1 - 91 /3+=100

29 ms (5) + 91 IT=100

160 ms 20 ( 11-- ) 91 IT=I00

4.85 h 0.20 0 + 96 6=100; a~<4.e41

9.6 m 0.4 ( 2 - ) 96 /3+=100

10.8 m 0.2 (7 + ) 96 91Va04 E /3+=100

3.5 m 0.1 0 + 96 92Wa14 D /3+-~100; or=0.0061 5

34.6 s 0.9 (2 + , 3 + ) 91 91Va04 T /3+=82 9; ot=18 9

39.6 s 0.4 ( 1 0 - ) 91 /3+--90.8 20; 0t--9.2 20

33.3 ms 1.3 0 + 91 96Bi17 TD a=?; /3+=1#

*192pb D : a : average 92Wa14=0.0062(6)% 79To06=0.0057(10)%

*192po T : average 96Bi17=33.2(1.4) 81Le23=34(3)

193Os --33396 4

193Ir --34536.3 2.9

19311~ -- 34456.1 2.9 80.22 0.02

193pt --34479.7 2.9

193 Pt'n --34329.9 2.9 149.78 0.03

193Au --33411 9

193Au 'n --33121 9 290.17 0.04

193Hg --31071 19

193 Hgn~ --30930 19 140.76 0.05

193T1 --27430# 250#

193 Tlm --27060# 250# 369 4

193pb --22280# 190#

193pbm --22150# 200# 130# 80#

193Bi -- 15780# 350#

193Bi m -- 15470# 350# 308 7 AD

193po --8290# 280# *

193pore --8150# 280# 140# 80# AD *

193At 180# 400#

30.5 h 0.4 3 / 2 - 97 f l - =100

STABLE 3/2 + 97 IS=62.7 5

10.53 d 0.04 1 1 / 2 - 97 IT=100

50 y 9 1/2-- 97 e=100

4.33 d 0.03 13/2 + 97 IT=I00

17.65 h 0.15 3/2 + 97 /3+=100; t r< le -5

3.9 s 0.3 1 1 / 2 - 97 I T ~ 100; /3+ ~0.03

3.80 h 0.15 3 / 2 - 97 fl+=100

11.8 h 0.2 13/2 + 97 fl+=92.9 9; IT=7.1 9

21.6 m 0.8 1/2 I+) 97 fl+=100

2,11 m 0.15 9 /2 ( - ) 97 87Bo44 J 1T=75; /3+=25

5# m 3 /2 - -# 97 /3 + ?

5.8 m 0.2 13/2 (+1 97 88Me.A J /3+=100

67 s 3 ( 9 / 2 - ) 97 /3+--95 3; or=5 3

3.2 s 0.7 (1/2 + ) 97 a--90 2 0 ; / 3 + ~ 1 0

360 ms 50 3 / 2 - # 97 t~,~100;/3+ ?

260 ms 20 ( 13/2 + ) 97 ABBW J ot~,-~ 100;/3+ .9

40 ms 9 / 2 - # 95Le.A TD ot=100

*193T1 m E : less than 13 keV above 362.5 level, from ENSDF

*193pb T : T=4.0 m reported in Karlsmhe charts 1981 and 1995. Not traceable * 193pore J : from a decay to 189 pb m :It air


Nuclide Mass excess Excitation Half-life J~ Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

194Os --32435 4 6.0 y 0.2 0 + 96 /3 -=100 194Ir --32531.9 2.9 19.28 h 0,13 1 - 96 /3 -=100 194 Irn' --32405 9 147.078 0.005 31.85 ms 0.24 (4 + ) 96 IT=100 1941r'~ --32180 70 350 70 BD 171 d 11 (10, 11) {-#) 96 /3-=1011 194pt --.34778.6 2.9 STABLE 0 + 96 IS=32,9 6 194Au --32287 12 38.02 h 0.10 1 - 96 /3+=100 194Aura --32180 12 107.4 0.5 600 ms 8 (5 + ) 96 IT=I0(I

104Au" --31811 12 475.8 0.6 421) ms 10 ( I I - - ) 96 IT=I00 194Hg --32247 23 440 y 80 0 + 96 e=100 194T1 --26960# 210# * 33.0 m 0.5 2-- 96 /3+=1011; ot<le-7 194TW --26660# 290# 300# 2011# * 32.8 m 0.2 (7 + ) 96 /3+=100 194pb --24250# 150# 12.0 m 0.5 0 + 96 /3+=100; ot=7.3e~5 29

l ~ B i --16070# 430# * 95 s 3 (3 + ) 96 /3+~100; o,,----0.46 25 P~lBim --15970# 440# 100# 70# * 125 s 2 ( 6 ~ , 7 ~ ) 96 /3+,"~100; ot ? 194Bin --15800# 340# 270 .51X1 AD * 115 s 4 (10- - ) 96 /3+~100; 0--0.20 7 1¢14po --10910 200 392 ms 4 0 + 96 a~ 100 ; /3+ ? l(~At --960# 400# * 41) ms 3+# 96 a,~.,~100; /3+ '? I~Atm --710# 370# 250# 150# * 250 ms 1 0 - # 96 a~l(KI; 1T ?

195Os --29690 500 6.5 m 3 / 2 - # 94 /3 -=100 1951r --31692.4 2.9 2.5 h 0.2 3/2 + 94 /3-=11111 19517n --31582 20 110 20 BD 3.8 h 0.2 1 1 / 2 - 94 /3---95 5; IT=5 5 195pt --32812.4 2.9 STABLE 1/2-- 94 IS=33.8 6 195ptm --32553.1 2.9 259,30 0.08 4.02 d 0.01 13/2 t 94 IT=100 195Au --32586 3 186.10 d 0.05 3/2 F 94 e=100 195Au m --32267 3 318.58 0,04 30.5 s 0.2 11/2-- 94 1T=I00 195Hg --31080 50 9.9 h 0.5 1 / 2 - 94 /3+=1111) 195Hgm --30900 50 176.07 0.04 41.6 h 0.8 13/2 + 94 1"1"--54.2 20; /3-}=45.8 20 195T1 --28270# 1_30# 1.16 h 0.05 1/2 t 96 /3+=100 195T1"~ --27790# 130# 482.63 0.17 3.6 s 0.4 9 / 2 - 96 IT=I0() 195pb --23780# 410# 15 m 3 / 2 - 96 /3 F =1~1 195pbm --23580# 410# 202,9 0.7 15,0 m 1.2 13/24 96 91Gr12 E /3+=1{]0 195Bi --17930# 220# 183 s 4 ( 9 / 2 - ) 96 /3+~100; ~--0.03 2 195Bi m --17530# 220# 399 6 AD 87 s 1 11/2 + ) 96 /3+=67 17; ct=33 17 195po --11140# 220# 4.64 s 0.09 ( 3 / 2 - ) 94 o~=75 15; /3÷=25 15 195pore --10950# 220# 1911# 80# 1.92 s 0.02 (13/2 + ) 94 a~911; /3+,."~'~,~10; IT<0.01 195At --3210# 400# * 140 ms ~) 9 / 2 - # 94 95Le.A TD a=?;/3+<25,# 195At m --3230# 400# --20 60 AD * 420 ms 80 ( 1 / 2 ; ) 95En.A TJD o,.~.,~100; /3 + ?

• 195Atm T : 95En.A=390(+I00~0) supersedes 95Le.A=6~I(+320-160) from same gl'oup

196Os --28300 40 34.9 m 0.2 0 + 95 /3--=100 1961r --29450 40 52 s 1 ( 0 - ) 95 /3 - =1110 196h~t --29~130 100 420 110 BD 1.40 h 0,02 ( 10, 11 - ) 95 / 3 - ~,~-, 100; IT<0.3 196pt --32662.9 2.9 STABLE 0 + 96 1S=25.3 6 196Au --31157 4 6.183 d 0.010 2 - 95 /3+=93.05 10; /3--=6.95 10 196Aura --31072 4 84.660 0.020 8.1 s 0.2 54 95 IT= 100 196Au" --30561 4 595.66 0.04 9.6 h 0.1 1 2 - 95 IT= 1011 196Hg --31843 4 STABLE >2.5Ey 0 + 95 90Bu28 T IS--0.15 1; 2/3 4 ? 196TI --27470# 140# 1.84 h 0.{)3 2-- 95 /3+=100 196T1" --27080# 140# 394.2 0.5 1.41 h 11.02 (7 + ) 95 /3~ =95.5; IT=4.5 l%pb --25420# 140# 37 m 3 04 95 /34 =100; a_<3e-5 l%Bi --18060# 210# 5.1 m 0.2 (3 + ) 97 /3+~100; ct---0.(X)ll5 34 196Bi" --17900# 210# 167 3 AD 0.6 s 0.5 (7 +) 97 IT=?; /3 + ? 196Bi" -- 17790# 210# 270 4 AD 4.00 m 0.05 ( 1 0 - ) 97 /3~=74.2 25; IT=25.8 25~ . . . 1961>o --135110# 180# 5.8 s 0.2 0 ÷ 95 93Wa04 D a'=94 5; /3+=6 5 196At --4000# 230# * 301) ms 100 3+# 95 or=?;/3~--4# 196Arm --3800# 270# 200# 150# * 1 0 - # 1T ?

l%Rn 21541# 2110# 4.1 ms 2.4 0 + 95No.A TD a~10(1; /3+ ? • 196Bin D : . . . ; 01---O.00038 10

• 1%11o T : and 5.511/.1) s in post cut-off date 97Pu01 • l%At T ; 253(9) ms in post cut-off date 97Pu01 • 196Rn T : symmetrized from 3.11+3.1-1.6); updated 3 (+7-2) in post cut-off 97Pu01



1971r --28283 20 5.8 m 0.5 3/2 + 96 , 8 - =100 1971rm --28168 21 115 5 8.9 m 0.3 11/2-- 96 ,8- -~100; IT--0.25 10 197pt --30438.1 2.9 19.8915 h 0.0019 1/2- 96 , 8 - = 100 197ptm --30038.5 2.9 399.59 0.20 95.41 m 0.18 13/2 + 96 IT--96.7 4; ,8 -=3 .3 4 197 Au -- 31157.0 2.9 STABLE 3/2 + 96 IS : 100. 197Au ns --30747.8 2.9 409.15 0.08 7,73 s 0.06 1 1 / 2 - 96 IT=100 197Hg --30557 4 64.14 h 0.05 1/2- 96 e=100 197Hgn~ --30258 4 298.93 0.08 23.8 h 0.1 13/2 + 96 IT--91.4 7; ~=8.6 7 197T1 --28380 -30 2.84 h 0.04 1/2 + 96 fl+ =100 197TI m --27770 30 608.22 0.08 540 ms 10 9 / 2 - 96 IT=IO0 197pb --24800# 100# 8 m 2 3 / 2 - 96 ,8+=100 197pb'~ --24480# 100# 319.31 0.11 43 m 1 13/2 + 96 ,8+=81 2; IT=I9 2; a < 3 e ~ l 197Bi -- 19620 240 9.3 m 0.5 ( 9 / 2 - ) 96 ,8+ =11~0; ~=ie~ .#

197Bi" --19110# 250# 510# 50# 5.04 m 0.16 (1/2 + ) 96 ot=55 40; ,8+--45 40; IT<0.3 1971>o --13450# 190# 53.6 s 1.0 ( 3 / 2 - ) 96 ,8+ ?; a--44 7

197po" -- 13210# 200# 230# 90# 25.8 s 0,1 (13/2 + ) 96 a=84 9; ,8+ ?; IT----0.01# t97At --6250# 350# * 350 ms 40 (9/2-) 96 a--96 4; ,8+--4 4 197At" --6200# 350# 50 70 AD * 3.7 s 2.5 (1/2 + ) 96 o,~100; ,8 + ?; IT<0.004 197Rn 1550# 280# 66 ms 16 3 / 2 - # 96En02 T a~ 100 ; ,8+ ? 197Rn m 1790# 280# 240# 90#" AD 21 ms 5 13/2+# 96En02 T ot~,~100; ,8+ ?

• 197Rn T : average 96En02=65(+25-14) 95Mo14=51(+35-15) • 197Rnm T : average 96Eo02=19(+8~.) 95Mo14=18(+9-5)

1981r --25820# 200# 8 s 1 95 ,8--=100 198pt --29923 4 STABLE >320'Fy 0 + 95 52Fr23 T IS=7.2 2; 2 ,8- ?; ot ? 198Au --29598.0 2.9 2.69517 d 0.00021 2 - 95 f l - =10[) 198Aura --28786 3 811.7 1.5 2.27 d 0.02 ( 1 2 - ) 95 IT=100 198Hg --30970.5 2.9 STABLE 0 + 95 IS=9.97 8 198T1 --27510 80 5.3 h 0.5 2 - 95 ,8+=100 198Tim --26970 80 543.5 0.4 1.87 h 0.03 7 + 95 fl+=54 2; IT=46 2 198Tin --26770 80 742.3 0.4 32.1 ms 1.0 ( 1 0 - ) 95 IT=100 198pb --26100# 90# 2.40 h 0.10 0 + 96 ,8+=100 198Bi -- 19540 180 10.3 m 0,3 (2 + , 3 + ) 95 fl+ =100 198Bi n' --19390# 190# I50# 50# 11.6 m 0.3 (7 + ) 95 ,8+=100 198Bi n --19150# 190# 390# 50# 7.7 s 0.5 ( 1 0 - ) 95 IT=I00 198po -- 15520# 150# 1.76 m 0.03 0 + 96 a=57 2; ,8+--43 2 198At --6750# 430# * 4.2 s 0.3 (3 + ) 96 95Bi.A D a>94; ,8+ ? 19SAtin --6380# 340# 370 500 AD * 1.0 s 0.2 ( 1 0 - ) 96 95Bi.A D a>86; fl+ ? 198Rn --1140 200 64 ms 2 0 + 96 95Bi17 T a=?; ,8+=1# 198Rn n~ non existent EU 50 ms 9 95 a=?; fl+=?; IT=?

• 198pt T : lower limit is for 0v-2,8- decay • 198Bi~ E : 248.5(0.5) keV above 198Binf, from 92Hu04

*198Rnm I : a, decay assigned to isomer by ENSDF, not accepted by NUBASE ~¢gt

199Ir --24420 40 20# s 3 /2+# , 8 - ?

199pt --27408 4 30.80 m 0.21 5 / 2 - 94 , 8 - = I 0 0 199ptm --26984 4 424 2 13.6 s 0.4 (13/2) + 94 IT=100 199Au --29111.0 2.9 3.139 d 0.007 3/2 + 94 , 8 - = 100 199Hg --29563.3 2.9 STArtLE 1/2-- 94 IS=16.87 10 199 Hg" --29030.8 2.9 532.48 0.10 42.6 m 0.2 13/2 + 94 IT=I00 199T1 --28120 100 7.42 h 0.08 1/2 + 94 ,13+=100 199Tim --27370 1114) 749.7 0.3 28.4 ms 0.2 9 / 2 - 94 1T= 100 199pb --25230 70 90 m 10 3/2-- 94 ,8+=100 t99Pb" --24800 70 429.5 2.7 12.2 m 0.3 13/2 + 94 ABBW E 13"--93; / /+=7 199Bi --20890 120 27 m 1 9 / 2 - 94 ,8+=100 199Bim --20250# 130# 640# 50# 24.70 m 0.15 (1/2 + ) 94 fl+ =?; IT<2; o~,0.01 199po --15280# 4L0# 5.48 m 0.16 ( 3 / 2 - ) 94 //+--92.5 3; ot=7.5 3 199pore --14970# 410# 311.9 2.8 AD 4.17 m 0.04 13/2 + 94 /3+=73.5 10; a=24 1; IT=2.5 199At --8730# 220# 7.2 s 0.5 ( 9 / 2 - - ) 94 a=89 6; ,8+ ? 199Rn --1580# 230# 620 ms 30 ( 3 / 2 - ) 94 or=?; ,8+=6# |99Rnm --1320# 230# 250# 110# 320 ms 20 (13/2 + ) 94 a=?; ,8+=3#

*199pbm E : 424.83 y to level lower than 9.3 keV, from ENSDF *199At D : symmetrized from ot---92(+3-8)%


Nuclide Mass excess Excitation Half-life j ,x Ens Reference Decay modes and intensities (keV) energy(keV) (%)

2°°pt --26618 20

2°0Au --27280 50

20°Aura --26320 50 960 70 BD

200Hg --295211.2 2.9

2°°TI --27064 6

200Tl'n --26310 6 753.6 0.2

2COpb --26254 13

2°°Bi --20360 9()

200Bim --20260# 110# 100# 70#

200Bi" --19930 9(1 428.20 0.10

200po -- 17010# 140#

200At -- 9040# 210#

200Atm --8930# 210# 113 3 AD

200Atn --8700# 210# 344 3 AD

200Rn --4030# 180#

200Fr 6050# 240# *

200F~mr 6250# 280# 200# 150# *

• 200At T : average 96Ta18=44(21 92Hu04--4311)

• 2GOAtn E : 230.9(0.2) keV above 200Atn~, from ENSDF

• 200Rn T : average 96Ta18=0.9610.03) 84Ca32=1.06(0.021

• 200Fr T : symmetrized from 19(+13-6)

• 2GOFr'n T : symmetrized from 5701+270-1401

12.5 h 0.3

48.4 m 0.3

18.7 h 0.5

STABLE

26. l h 0,1

34.3 ms 1.0

21.5 h 0.4

36.4 m 11.5

31 m 2

0 r 95 f l - = 1 0 0

I t - ) 95 f l - =100

1 2 - 95 / 3 - = 8 2 2; IT=I8 2

0 + 95 IS=23.10 16

2 - 95 /3+=100

7 ~" 95 IT= 100

0 ~ 95 e=lO0

7 + 95 /3+=100

(2 + ) 95 e>90; IT<I0

41X) ms 50 ( 1 0 - ) 95 IT=HI)

11.5 m 0.1 0 t 95 /3+=88.9 3; ot=l l . l 3

43.2 s 0.9 (3 + ) 95 96Ta18 T a=57 6; /3+-~3 6

47 s 1 (7 + ) 95 a--43 7;/34 =?; IT ?

3.5 s 0.2 ( 1 0 - ) 95 IT~,~84; a ,~ 10.5; ~,~,4.5

1.03 s 0,05 II I 95 96Ta 18 T ate98; / 3 + ~ 2

24 ms 10 3+# 96En01 TD a=100

6511 ms 210 1 0 - # 95Mo14 TD a ~ 1 0 0 ; IT ?

2°lpt - 2 3 7 6 0 511

2Ol Au --26416 4

2°1rig --27679.1 2.9

2°1T1 --27196 15

2°lTlm --26277 15 919.50 0.09

201Pb -- 25290 30

201 pbn~ -- 24660 30 629.14 0.17

201Bi --21450 30

201Bi'n --20600 ,30 846.34 0.21

201Po -- 16570# 100#

201po m -- 16150# 100# 424.2 2.5 AD

201 At -- 10720 240

201Rn --4160# 200#

201Rn m --3880# 200# 280# 110#

201Fr 3710# 350#

2.5 m 0.1 ( 5 / 2 - ) 94

26 m 1 3/2 + 94

STABLE 3/2-- 94

72.912 h 0.017 1/2 + 94

2.035 ms 0.007 ( 9 / 2 - - ) 94

9.33 b 0.03 5/2 - 94

61 s 2 13/2 + 94

108 m 3 9 / 2 - 94

59.1 m 0.6 1/2 + 94

15.3 m 0.2 3 / 2 - 94

8.9 m 11.2 13/2 + 94

85 s 3 ( 9 / 2 - ) 94 96Ta18 T

7.0 s 0.4 ( 3 / 2 - ) 94 96Ta18 T

3.8 s 0.1 113/2 + ) 94 96Ta18 T

61 ms 12 ( 9 / 2 - ) 94 96En01 T

.201Bi" D : a decay is observed. Its branching ratio is estimated 0.3%# in ENSDF

*201At T : average 96Ta18=83(2) and two results in ENSDF=89(3)

*201Rn T : average 96Ta18=7.1(0.8) 71Ho01=7.0(0.4)

*201Fr T : average 96En01=69(+16-11) 80Ew03--48(15)

/3 -=100

, 8 - = 1 0 0

IS=13.18 8

e=100

IT=I00

/3+=100

1T>99;/3+ <1

/3+ =100; or< l ev i

~=92.9#; IT<6.8; a=?

/3+--'98.4 3; ot=l.6 3

IT=56 14; e=41 10; a~,~,2.9

a=71 7;/3+=29 7

at=?; /3+=20#

a=?; /3+=10#; IT--O.01#

ot ~-, 100; /3+<1


Nuclide Mass excess Excitation Half-life j,n- Ens Reference Decay modes and intensities (keV) energy(keV) (%)

202pt --22600# 300# 44 h 15 0 + 92Sh12 T / 3 -=100

202Au --24420 170 28.8 s 1.9 ( 1 - ) 87 / 3 - =100

202Hg --27362.1 2.9 STABLE 0 + 87 IS=29.86 20 *

202'I'1 --25997 15 12.23 d 0.02 2 - 87 ]T~=I00

202pb --25948 10 52.5 ky 2.8 0 t" 87 e ~ 100; a < l #

2ff2pb" --23778 10 2169.84 0.09 3.53 h 0.01 9 - 87 IT=90.5 5; e=9.5 5 *

202Bi --20800 50 1.72 h 0.05 5 + 87 /3+=100; o t<le-5 *

202po --17980# 90# 44.7 m 0.5 0 + 87 /3+=?; a=2.0 2 *

202At -- 10760 180 * 184 s 1 (2 +, 3 + ) 87 92Hu04 TJ /3+=?; a=12.0 8 *

202Atr" --10710# 190# 50# 50# * 182 s 2 (7 + ) 87 92Hu04 TD IT ? ; /3 + ?; 0,,=8.7 15

202Atn --10320# 190# 440# 50# 460 ms 50 ( 1 0 - ) 92Hu04 TJD IT~I00 ; /3+---0.25#; a=0.096 11 *

202Rn --6320# 150# 9.94 s 0.18 0 + 87 96Ta18 T a=?; f l + = l s # *

202Fr 3060# 430# * 290 ms 30 (3 + ) 87 96En01 T t~=?;/3+=3# *

202FiS" 3430# 340# 360 500 AD * ~ ms 40 ( 1 0 - ) 87 92Hu04 J a=?; f l+=3#

202Ra 2.6 ms 2.1 0 + 96Le09 TD a=100 .

• 202Hg D : lower half-life limit for 24Ne decay T>3.7 Zy, from 90Bu28 **

• 202pbm E : 2169.83(0.07) keV in post cut-off date ENSDF'97 **

• 202Bi J : re-evaluation to a possible 6 + is discussed in 96Ca02 **

• 202po D : a=1.92(7)% in post cut-off date ENSDF'97 **

• 202At D : ot=18(3)% in post cut-off date ENSDF'97 **

• 202At" E : 391.7(0.5) keV above 2ff2Atm. from 92Hu04 **

• 202Rn T : avecage 96Ta18=10.3(0.4) 71Ho01=9.85(0.20) **

• 202Rn D : /3+=14(3)% in post cut-off date ENSDF'97 **

• 202Fr T : average 96En01=230(+80~0) 95Bi.A=300(40) J : from 92Hu04 **

• 202Ra T : symmetrized from 0.7(+3.34).3) **

203 Au

203 Hg

203T1

203 Pb

203 pb m

203 pb n

203Bi

2o3 Bim

203 Po

203 pot))

203At

203Rn

203Rnm

203Fr

203Ra

203 Ra m

.203Rn

--23159 4 53 s 2 3 /2 + 93 /3 -=100

--25283 3 46.612 d 0.018 5 / 2 - 93 /3--=100

--25775.3 2.9 STABLE 1/2 + 93 IS=29.524 14

--24801 7 51.873 h 0.009 5 / 2 - 93 e=100

--23976 7 825.20 0.09 6.3 s 0.2 13/2 + 93 IT=I00

--21852 7 2949.47 0.22 480 ms 20 29/2-- 93 IT=I00

--21547 21 11.76 h 0.05 9 / 2 - 93 /3+=100; a ~ l e - 5

--20449 21 1098.14 0.07 303 ms 5 1/2 + 93 IT=100

--17310 70 36.7 m 0.5 5 / 2 - 93 /3+~100; a=0.11 2

--16670 70 641.49 0.17 45 s 2 13/2 + 93 I T ~ 100; a=0.04#

--12250 120 7.4 m 0.2 9 / 2 - 93 /3+=69 3; a=31 3

--6230# 410# 43.5 s 2.1 (3/2, 5 / 2 ) - 93 96Ta18 T a=66 9; /3+=34 9

--5860# 410# 363 4 AD 26.7 s 0.5 13/2 I+l 93 87Bo29 J a=?; /3+=20# 980# 230# 550 ms 20 ( 9 / 2 - ) 93 a ~ 9 5 ; / 3 + ~ 5

8580# 230# 4 ms 3 ( 3 / 2 - ) 96Le09 TJD a ~ 1 0 0 ; / 3 + ?

8870# 230# 290# 120# 41 ms 17 (13/2 + ) 96Le09 TJD a,-~100;/3'+ ?

T : average 96Ta18=42(3) 71Ho01--45(3)

*203Rn m T : from 96Ta18

*203Ra T : symmetfized from 1.1(+5.04).5)

*203Ram T : symmetrized from 33(+22-10)



204Au --20770# 2110# 39.8 s 0.9 ( 2 - ) 94 /3--=100 204Hg --24707 3 STABLE 0 + 94 IS=6.87 4; 2 8 - ? 204TI --24359.8 2.9 3.78 y 11.02 2 - 94 /3-=97.10 12; e=2.°AI 12 204pb --25123.5 2.9 STABLE > 140Py 0 + 94 IS=I.4 l 204pb" --22937.7 2.9 2185.79 0.115 67.2 m 0.3 9 - 94 IT=I00 204Bi --20674 26 11.22 h 0.10 6 + 94 ,8+=100 204 Bim --19869 26 805.5 0.3 13.0 ms 0.1 1 0 - 94 lT=100 204 Bi# -- t7841 26 2833.4 1.1 1.07 ms 0.03 (17 + ) 94 IT=100 204p0 --18344 13 3.53 h 0.02 0 ~ 94 /3+--99.34 l; a--0.66 1 204At --11870 90 9.2 m 0.2 7 ~ 94 /3+=96,2 2; a=3.8 2 204At#~ --11280 90 587.30 0.20 108 ms 10 ( 1 0 - ) 94 IT=100 204Rn --8040# 140# 1.24 m 0.03 0 + 95 o,=73 1; /3+ ? 204Fr 550# 210# 1.7 s 0.3 (3 + ) 94 95Bi.A D a--96 2; /3+ ? 204Fr~n 610# 210# 54 6 AD 2.6 s 0.3 (7 + ) 94 95Bi.A D a=90 2; /3+ ? 204Fr~ 880# 210# 330 6 AD 1.7 s 0.6 ( 1 0 - ) 94 94Le05 T ot=74 8; IT=26 8 204Ra 6030# 180# 60 ms 11 0 + 95Le04 T a~ 100 ; /3+--0.3#

*204Fr'~ T : symmetrized from 1.4(+8-4) *204Ft'° E : 276.1 keV above 204Fr#', from 95Bi.A D : a intensity is from 95Bi.A

*204Ra T : average 95Le04=45(+55-21) 96Le09=59(+12-9) *204Ra D : /3+ intensity is estima~d by 96Ak.A

205Au --18990# 300# 31 s 2 3/2 + 94We02 T /3 -=100 205Hg --22304 5 5.2 m 0.1 1 / 2 - 93 /3 -=100 205Hgm --20747 5 1556.53 0.24 1.10 ms 0.04 113/2 + ) 93 IT=I00 205TI --23834.8 3.0 STABLE 1/2 ~ 93 1S=70.476 14 205pb --23783.7 2.9 15.3 My 0.7 5 / 2 - 93 ,~=100 205pbm --22769.9 2.9 1013.839 0.013 5.54 ms 0.10 13/2 + 93 IT=I00 205Bi --21075 8 15.31 d 0.04 9 /2-- 93 /3+=100 205po --17544 29 1.66 ia 0.02 5 / 2 - 93 f l+~100; o<--0.04 l 205 Po')f --16083 29 1461.20 0.21 58 ms l 1 9 / 2 - 93 IT=I00 205At --13010 30 26.2 m 0.5 9 / 2 - 93 /3+--911 2; a=10 2 205Rn --7760# 110# 2.8 m 0.1 5 / 2 - 93 ,8+=77 4; 0,=23 4 205Fr --1240 240 3.85 s 0.10 ( 9 / 2 - ) 93 ora l00; ,8+<1 205Ra 5760# 210# 220 ms 40 ( 3 / 2 - ) 93 96Le09 TJ a=?; ,84 ? 205Ram 6050# 200# 290# 120# 180 ms 50 113/2 + ) 96Le09 TJD a=?; IT ?

*205Ra T : average 96Le09=-210(+60-40) 87He10=2201601 *205Ra m T : symmetrized from 170(+60-40)

206Hg --211960 21 8.15 m 0.10 0 + 90 f l - = 1 0 0 206T1 --22267.1 3.0 4.199 m 0.015 0 - 90 f l - = 1 0 0 206Tim --19624 3 2643.11 0.19 3.74 m 0.03 ( 1 2 - ) 90 IT=100 206pb --23800.6 2.9 STABLE 0 + 90 IS=24.1 l 206Bi --20043 8 6.243 d 0.003 6 (+) 90 ,8+=100 206po --18197 l0 8.8 d 0.1 0 + 90 fl+--94.55 5; a=5.45 5 206At --12480 50 30.0 m 0.6 (5) + 90 ,8+=99.11 8; a=0.89 8 206Rn --9170# 90# 5.67 m 0.17 0 ÷ 90 a=62 3; fl+=38 3 206Fr -- 1410 180 * 15.9 s 0.2 (2 + , 3 + ) 90 92Hu04 JD /3+ =?; a--42 24 2 ~ F r " --1360# 190# 50# 50# * 15.9 s 0.3 (7 + ) 92Hu04 TD a - ~ 2 24; ,8+ ?; IT ? 206Fd) --830# 190# 580# 50# 700 ms 100 ( 1 0 - ) 90 92Hu04 J IT,~,100; a=0.3 1 2116 Ra 3520# 150# 240 ms 20 0"- 90 a=100 206Ac * 26 ms 10 (3 + ) 96Uu.A TJD a=100 206Acre 330# 200# * 38 ms 14 (10 - - ) 96Uu.A TJD a=lO0

• 206Fr D : a=84(2)% for mixture of 206Fr and 206Frm, in 92Hu04. Value replaced by • 206Fr D : uniform distribution 0%-84% for each isomer *206Fr" E : 531 keV above 2"06Frm, from ENSDF .206Ac T : symmetrized from 2 2 ( + 1 3 ~ ) *206Acre T : symmetrized from 321+19-91

g¢



2°7Hg --16230 150 2°7TI --21044 6 2°7 Tim --19696 6 1348.1 0.3 207 Pb -- 22467.1 2.9 207phm --20833.7 2.9 1633.368 0.005 207Bi --20069 4 207po --17160 7

207 pom -- 15777 7 1383.15 0.06 207 At -- 13250 2 l 207 Rn -- 8640 70 207Fr --2930 120 207Ra 3470# 420# 207 Ra" 4030# 410# 560 50 AD

2°7Ac 11270# 230# *207Ram T : average 96Le(D=63(16) 87He10=55(10) .2°7Ac T : symmetrized from 22(+40-9)

2.9 m 0.2 (9/2 + ) 94 4.77 m 0.02 1/2 + 94 1.33 s 0.11 1 1 / 2 - 94

STABLE 1/2-- 94 806 ms 6 13/2 + 94

31.55 y 0.05 9/2-- 94 5.80 h 0.02 5/2-- 94 2.79 s 0.08 19/2-- 94 1.80 h 0.04 9/2 - 94 9.25 m 0.17 5 / 2 - 94 14.8 s 0.1 9 / 2 - 94

, 8 - = 100 ,8-=100 I T ~ 100; , 8 - < 0 . 1 # IS=22.1 1 rr=100 /3+ = l i d ,8+,'~IID; a--0.021 2 lT=100

,8+--91.4 10; a=8.6 10 ,8+=79 3; a=21 3 a--95 2;/5'+=5 2

1.3 s 0.2 ( 5 / 2 - , 3 / 2 - - ) 94 a ~ 9 0 ; ` 8 + ~ 1 0 57 ms 8 ( 13/2 + ) 94 96Le09 T IT=85#; a=?; /3+ =0.55# 42 ms 27 9 / 2 - # 94Le05 TD a=100

206Hg --13100# 300# 208T1 -- 16762.6 2.9 208pb --21763.6 2.9 208Bi -- 18884 4 208 Bim --17313 4 1571.1 0.4 208po -- 17483 3 208At -- 12498 26 208Rn --9658 13 20aFt --267O 8O 20~Ra 1650# 140# 208Ac 10700# 210# 208 Acre 11210# 210# 510 22 AD

*2~Hg T : symmetrized from 42(+23-12) .208Ac T : symmetrized from 95(+24-16)

49 m 18 0 + 3.053 m 0.004 5 (+) 86

STABLE 0 + 96 368 ky 4 (5) + 86 2.58 ms 0.04 ( 1 0 ) - 86

2.898 y 0.002 0 + 86 1.63 h 0.03 6 + 86

24.35 m 0.14 0 + 86 59.1 s 0.3 7 + 86 1.3 s 0.2 0 + 86 l i d ms 20 (3 + ) 96

28 ms 7 ( 1 0 - ) 96

*208Acre E : if a decay is to (7 + ) 204Frm instead of (10 - - ) as assumed in AME'95, *208Acre E : then E=234(22) keV T : symmetdzed from 25(+9-5)

94Zh02 TD `8-=100

`8 -=100 IS=52.4 1 B+=IID IT=liD a ~ l i D ; /3+=0.00223 23

,8+--99.45 6; a=0.55 6 a=62 7; ,8+=38 7 0:--90 4; `8+=10 4

a=?; `8+ =5# or=?; `8+=I# a=?; IT<10#; `8+=1#

209TI -- 13647 10 209pb -- 17629 3 209Bi -- 18272.9 3.0 209po -- 16380 3 209At -- 12893 8 209Rn --8964 29 209 Fr -- 3800 30 209Ra 1810# 130# 209Ac 8910 240 209Th

• 209Ac T : symmetdzed from 91(+21-14) • 209Th T : symmetrized from 3.8(+6.9-1.5)

2.161 m 0.007 (1/2 + ) 91 94Ar23 T `8 -=100 3.253 h 0.014 9 /2 + 91 `8 - = l i d

STABLE 9/2-- 91 IS=liD. 102 y 5 1 / 2 - 91 ot~l iD; `8+=0.48 4

5.41 h 0.05 9 / 2 - 91 ,8+--95.9 5; a--4.1 5 28.5 m 1.0 5 / 2 - 91 /31+=83 2; o~=17 2 50.0 s 0.3 9 / 2 - 91 a=89 3; `8+=11 3 4.6 s 0.2 5 / 2 - 91 oz ~90; `8+ ~ 1 0 95 ms 18 ( 9 / 2 - ) 91 94Le05 T a=?; `8+=1# 7 ms 5 5 / 2 - # 961k01 TD a=?; `8+ ?

210TI --9254 11 21°pb -- 14743 3 21°Bi -- 14806.1 3.0 210Bim --14535 3 271.31 0.11 210po -- 15968.2 2.9 210At --11987 8 210Rn --9613 10 210Fr --3355 22 210Ra 420# 90#

210Ac 8620 190 210Th 14000# 150#

• 2101"1 D : symmetrized from `8-n=0 . iD7(+7-4)% • 21°Th T : symmetrized from 9 (+17-4 )

1.30 m 0.03 (5 + ) 92 `8 - =liD; `8 - n=0.009 6 22.3 y 0.2 0 + 92 /3-=100; ot=l.9eq5 4

5.013 d 0.005 1 - 92 f l - = l i D ; a=13.2.e-5 10 3.04 My 0.06 9 - 92 a=100

138.376 d 0.002 0 + 92 or=liD 8.1 h 0.4 (5) + 92 fl+ ~.IID; a=0.175 20 2.4 h 0.1 0 + 92 a=96 1; `8+-~1 1

3.18 m 0.06 6 + 92 a=60 30; ,8+--40 30 3.7 s 0.2 0 + 92 a ~ 9 6 ; `8+~4 350 ms 50 7+# 92 a ~ 9 6 ; `8+ ~ 4 17 ms 11 0 + 95Uu01 T ore?; fl+ ?

a~


Nuclide Mass excess Excitation Half-life ./n- Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

211pb --10496.6 3.0 36.1 m 0.2 9/2 + 91 f l - = 1 0 0 211Bi --11869 6 2,14 m 0,02 9 / 2 - 91 a ~ 1 0 0 ; B-=0 .276 4 211po --12447.7 3.0 516 ms 3 9/24 9I a=100 211pore --10985 6 1462 5 AD 25.2 s 0.6 (25/2 + ) 91 a~ 100 ; 1T--9.016 4 21tAt --11662 4 7.214 h 0.007 9 / 2 - 96 a=58.20 8; o~--41.80 8 211Rn --8770 7 14.6 h 0.2 1 / 2 - 96 .0+=72.6 17; o~=27.4 17 2 l iF t --4164 21 3.10 m 0.02 9 / 2 - 91 or>80; .0+<20 2 l iRa 830 70 13 s 2 5/2 I - I 91 a>93; /3+<7

211Ac 7120 130 250 ms 50 9 / 2 - # 91 a ~ 1 0 0 ; /3+<0.2 211Th 13840# 420# 48 ms 20 5 / 2 - # 95Uu01 T a=?; /3+ ?

*211T~ T : symmetrized from 37(+28-11 )

212pb --7556.7 2.7

212Bi -81311.5 2.9 2t2Bim --7880 30 250 30 AD 212Bin --5930# 200# 2200# 200# 212po -- 10384.5 2.9 212pore --7474 13 2911 12 AD 212At - -863i 4 212Arm --8409 8 222 7 AD 212Rn --8673 4 212Fr --3544 26 212Ra --202 14 212 Ac 7280 90 212Th 12030# 140# 212pa 4# ms 7+#

*212Bin E : 1910 keV. if 100% .0 decay goes to 2922 level in 212po, and if logft for *212Bin E : this transition is 5.1 (see ENSDF). or higher .212Ac J : ENSDF would assign 7 + , if the observed ot feeds the 208Fr 7 + ground-state *212Th T : symmetrized from 30(+20-10) *212pa T : a decay observed in post cut-off date 97Mi03 with half-life=5.1(+6.1-1.9) ms

10.64 h 0.01 0 + 92 f l - =100 60.55 m 0.06 1 ( - I 92 89HaA D .0-=64.06 6; a=35.94 6; fl-ct---0.014 25.0 m 0.2 (9 - - ) 92 7.0 m 0.3 > 16 92 299 ns 2 IY ~ 92 45.1 s 0.6 (184 ) 92

3 t4 ms 2 1 I - ) 92 119 ms 3 ( 9 - ) 92

23.9 m 1.2 0 + 92 20.0 m 0.6 5 + 92 13.0 s 0.2 0 + 92 930 ms 50 6+# 92 36 ms 15 0 + 92

0t--67 1; f l - -=33 1; B-o r=30 1 ,0-- ~100; IT ? a=100 a~ 100 ; IT=0.07 2 a~,-~l(~O; fl+<O.03; /3-- <2e~5 a>99; IT<I a=i00; 213 + ? .0+ =57 2; 0t=43 2 a=?; .0+=15# a=?; /3+ =3# a ~ 100;/3+ --0.3# a=100#

2t3pb --3260# 100# 10.2 m 0.3 ( 9 / 2 4 ) 92 213Bi --52411 8 45,59 m 0.06 9 / 2 - 92 213Po --6667 4 4.2 ,us 0.8 9/2 ~ 92 213At --6594 6 125 ns 6 9 /2-- 92 213Rn --5712 7 25.0 ms 0.2 (9/2 + ) 92 213Fr --3563 8 34.6 s 0.3 9 / 2 - 92 213Ra 322 ~1 2.74 m 0.06 1 / 2 - 92

2t3Ra"~ 2090 30 1768 6 AD 2.1 ms 0.1 1 7 / 2 - # 92 213At 6120 60 8Ol ms 50 9 / 2 - - # 92 213Th 12070# 130# 140 ms 25 5 / 2 - # 92 213pa 19730 2541 7 ms 3 9 / 2 - #

*213Ra" E : derived fi'om differeace in a decay energy; from AME'95 evaluation.

/3-=1110 /3-=97.91 3; 0,=2.09 3 a=100 a=100 tr=100 a=99.45 3; fl~ ~1.55 3 a=80 5; B ~ ? 1T~-,99; ~x~ 1 a=?; /3+ ? a=?;/3+ ?

95Ni05 TD a=100

*213Ram E : ENSDF evaluation: less than 10 keV above 1769.7 level, thus 1775(3) keV *213Ra m E : Next AME should make use of both pieces of information. *213pa T : symmetrized from 5.31+4.0-1.6)

214pb --188.11 2.5 26,8 m 0.9 0 ~ 95 214Bi --1212 11 19.9 m 0.4 1 - 95 89Ha.1 D 214po --4484 3 164.3 ,us 2.0 0 + 95 214A! --3394 5 558 ns t0 1 -- 95 214Rn --4335 10 270 ns 20 04 95 214Fr --974 9 5.0 ms 0.2 / 1 - ) 95 214Fl~t --85{) 9 123 6 AD 3.35 ms 0.05 ( 8 - - ) 95 214Ra 85 II 2.46 s 0.03 0 + 95 214Ac 6420 50 8,2 S 0.2 5+# 95 214Th 10670# 9 ~ IO') ms 25 0 ~ 95 214pa 193211 190 17 ms 3 95 95Ni05 D

/3 -=100

/ 3 - ~ 1 0 0 ; a---41.021 1; fl-ot--O.003 a=100 a= 100 tr=100; 2/3 + ?

a=100 a.~.lt~; /3+=0.059 4 a > 8 9 3; /3~ <'11 3 a=100 a=100

G. Audi e t a l . / N u c l e a r Phys i c s A 624 (1997) 1 - 1 2 4 9 9

Nuclide Mass excess Excitation Half-life f r Eas Reference Decay modes and intensifies (keV) energy(keV) (%)

215pb

215Bi 1710 100 215po --545.3 2.9 215At --1266 7 215Rn --1184 8 215 Fr 304 8 215Ra 2519 8 215Ac 6010 50 2ISTh 10920 70 215pa 17790 140

36 s 1 5/2 + # 96Ry.B T fl-- =100 7.6 m 0.2 9 / 2 - # 92 ,8--=100

1.781 ms 0.004 9 /2 + 92 a=100; ,8-=2.3e~- 2 100 /zs 20 9 / 2 - 92 a=lO0

2.30 p,s 0.10 9 /2 + 92 ct=lO0 86 ns 5 9 / 2 - 92 a=lO0

1.59 ms 0.09 (9/2 + ) 92 a=100 170 ms 10 9 / 2 - 92 a~,100; ,8+=0.09 2 1.2 s 0.2 ( 1 / 2 - ) 92 a=100 15 ms 4 9 / 2 - # 92 96An21 T ot=100

216Bi 5780# 100# 216po 1774.7 2.7 216At 2244 4 216Rn 240 8 216Fr 2969 13 216Ra 3277 9 216Ac 8124 27 216Th 10294 16 216pa 17800 110

*216Bi T : also 90Ru02=3.6(0.4), outweighed *2t6At J : 1 - in post cot-off date ENSDF'97

2.17 m 0.05 1 - # 96Ry.B T , 8 - = 100 * 145 ms 2 0 + 87 a=100; 2 ,8- ? 300 /zs 30 I ~-) 87 a ~ 1 0 0 ; ,8 -<0 .006 ; ~<3e-7 * 45 /zs 5 0 + 87 a=100

700 ns 20 ( 1 - - ) 87 a=lO0; fl+ <2e-7# 182 as 10 0 I- 87 a=100; , < l e - 8 330 /.~s 30 ( 1 - - ) 87 a=100; ~+=7e-5#

28 ms 2 0 + 87 a ,~ 100; ,8+=0.006# 105 ms 12 87 96An21 T a=?; ,8+=20# *

*2t6pa D : a=?; ,8+ =2%# in post cut-off date ENSDF'97

217Bi

217po 5830# 100# 217At 4387 8 217Rn 3646 5 217Fr 4300 7 217Ra 5874 10 217Ac 8693 13 217Th 12170 30 217pa 17040 80 217pare 1890(I 80 1860 70 AD

*217Fr T : average 90An19=16(2) 70Bo13=22(5)

97 s 3 9 / 2 - # 96Ry.B T 1.47 s 0.05 5 /2+# 91 96Ry.B T 32.3 ms 0.4 9 / 2 - 91 540 /zs 50 9/2 + 91 16.8 /zs 1.9 9 / 2 - 94 90An19 T 1.63 brs 0.17 (9/2 + ) 91 90Ao19 T 69 as 4 9 / 2 - 91 252 ,tzs 7 (9/2 + ) 91 3.4 ms 0.2 9 / 2 - # 91 96An21 T 1.5 ms 0.2 29/2+# 91 96An21 T

*217Ra T : average 90An19=1.7(0.3) 70Bo13=1.6(0.2)

218po 8351.6 2.5 218At 8087 12 218Rn 5204 3 218Fr 7045 5 218Fr m 7131 7 218Ra 6636 11 218Ac 10830 50 218Th 12359 14 218pa 18640 70 218U 21880# 100#

86 5 AD

3.10 m 0.01 0 + 96 1.5 s 0.3 1 - # 96 35 ms 5 0 + 96 1 . 0 ms 0.6 1 - 96

22.0 ms 0.5 96 25.6 /zs 1.1 0 + 96 1.08 /zs 0.09 1 -- # 96 109 ns 13 0 + 96 116 /zs 17 96 96An21 T 6 ms 5 0 + 96

*218pa T : average 96An21=110(20) 79Sc09=120(+40-20) ,218U T : symmetrized from 1.5(+7.3-0.7)

219po

219At 10520 80 219Rn 8825.7 2.8 219Fr 8608 7 2t9Ra 9379 9 219Ac 11560 50 219Th 1446(I 50 219pa 18520 70 2tgu 23210 80

• 219U T : symmetrized from 42(-t-34-13)

2# m 7 /2+# 56 s 3 5 / 2 - # 92

3.96 s 0.01 5/2 + 92 20 ms 2 9 / 2 - 92 10 ms 3 (7/2) + 92

11.8 ~s 1.5 9/2-- 92 1.05 ~s 0.03 9 /2+# 92 53 os 10 9/2-- 92 55 ~s 25 9 /2+# 93An07 T

, 8 - = 100 a>95; ,8-- <5 a ~ l O 0 ; ,8--=0.012 4 a=lO0 a=100 * a=lO0 *

a=?; ,8+ <_2 a=lO0 a=lO0 ot~lO0; IT ?

a ~ 1 0 0 ; ,8--=0.020 2 a~-,100; ,8--=0.1 a=lO0 a=lO0 a~,100; IT ? a=100; 2fl + ? a=100

a=100 a=100 * a=lO0 *

a ? ; B - ?

a ~ 9 7 ; f l - ~ 3 a=lO0 a=100 a=100 a= 100; fl+ =le-6# a=lO0; ,8+ =le-7# a= 100; ,8+ =5e-9# a=lO0 *

1 0 0 G. Audi et al. /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-life j r r Ens Reference Decay modes and intensities (keV) energy(keV ) (%)

220At 14250# 110# 220Rn 10604.3 2.7

220Fr 11469 5 220Ra 10260 10 220 Ac 13740 50

22°Th 14655 22 220 Pa 20380 60

220U 2,'1,020# 200#

*220At D : ot intensity is from 89Bu09

* 2 ~ R a T : average 90An19=17(2) 61Ru06=23(5) .220Ac T : average 90An19=26.4(0.2) 70Bo13=26.1(0.5)

3.71 m 0.04 3 ~ -#) 89Li04 TJ /3----92 2; a=8 2 55.6 s 0.1 0 + 87 a=100; 2 /3- ?

27.4 s 0.3 1 + 87 a ~ 1 0 0 ; /3-=0.35 5 17.8 ms 1.9 0 + 87 90An 19 T a=lO0

26.36 ms 0.19 ( 3 - ) 87 90An19 T a=lO0; /~+=5e-4# 9.7 ,us 0.6 0 + 87 a=lO0; ~=2e-7# 7811 ns 160 87Fa.A TD ct=100

60# ns 0 ~ a 7; B ~ ?

J : from 96Li05

221 At 16900# 300# 221Rn 14400# 100# 221Fr 13270 8 221Ra 12955 7

221 mc 145111 5(I 221Th 16927 10 221 Pa 20370 50 221U 24550# 110#

2.3 m 0.2 3 / 2 - - # 90 25 m 2 7/2 ~+1 90 4.9 m 0.2 5/2-- 90 94Bo28 D

28 s 2 5 /2 + 90 94Bo28 D 52 ms 2 9 / 2 - # 90

1.68 ms 0.06 (7/2 + ) 90 5.9 ,us 1.7 9 / 2 - 90

700# es 9 /2 + #

/ 3 -=100 / 3 - = 7 8 1; a=22 1 ct~-q00; / 3 - < 0 . l ; 14C=8.8e-11 11 a=100; 14C=1.2e-10 9

a=lO0

a=lO0 a=lO0 a ? ; / 3 + ?

222 At 20800# 300#

222Rn 16366.8 2.5

222Fr 16342 21 222Ra 14309 5 222 Ac 16607 6 *

222Acn~ 16810# 150# 200# 150# * 222Th I719(I 13

222pa 22100# 70# 222U 24280# 100#

54 s 10 96 3.8235 d 0.0003 0 + 96

14.2 m 0.3 2 - 96

38.0 s 0.5 0 + 96 5.0 s 0.5 1 - 96 1.05 m 0.07 high 96 2.8 ms 0.3 0 + 96

3.2 ms 0.3 96 95Ni.A T 1.4 /xs 0.7 0 q 96

• 222Ac m D : derived from 0.7% < 13 + < 2%, in ENSDF • 222pa T : average 95Ni.A=3.3(0.3) 79Sc09=2.9(+0.64).4)

• 222pa T : 70Bo13=5.7(0.5) at variance, not used • 222U T : symmetrized from 1.0(+1.0-0.4)

/ 3 -=100 a=100

/ 3 - =100 a=100; 14C=3.0e-8 10

a----99 1;/3+=1 1 a=?; IT< i0; /3+=1.4 4 a=100; e< 1.3e-8#

a=100

a=100; /3+ < 1e-45#

223At 23600# 400# 50 s 7 3 / 2 - # 92 223Rn 20,'~00 # 300# 23.2 m 0.4 7/2 92 223Fr 18379.0 2.7 21.8 m 0.4 3/2 ( - ) 92

223 Ra 17230.0 2.8 11.435 d 0.004 3/2 + 92 223Ac 17816 7 2.10 m 0.05 ( 5 / 2 - ) 92 223Th 19371 10 600 ms 20 (5/2) + 92 223pa 22320 70 5.8 ms 0.8 9 / 2 - # 92 95Ni.A T 223U 25820 70 21 ,as 8 7 / 2 + # 91Anl0 T

• 223pa T : average 95Ni.A=5.0(I.0) 70t3o13=6.5(1.0) • 223U T : symmetrized fix~m 18(+10-5)

/3--=100 / 3 -=100 , 6 - ~ 100; a=0.006 a=lO0; 14C=6.de-8 4

a=99; ~=1 a=100 a=t00; /3 + <0.001# a=100

224Rn 22440# 3~)# 107 m 3 0 + 87 224 Fr 21640 50 3.30 m 0.10 1 ( - I 87 224Ra 18818.0 2.7 3.66 d 0.04 0 + 96

224Ac 20221 5 2.9 h 0.2 0 - 87 224Th 19989 12 1.05 s 0.02 0 + 87 22,1Pa 23860 50 844 ms 19 5 -- # 87 96Li05 T 224 U 257tXI 25 950 u s 280 0 + 92To02 T

• 224Fr J : 1 - and T=3.33 m in post cut-off date ENSDF'97 • 224Ra D : 14C (not 12C). ¢otrceted in post cut-off date ENSDF'97 • 224pa T : average 96Li05=790(60) 96Wi.A=850(20) • 224U T : average 92To02=1000(400) 91An10=-700(+500-200)

/ 3 -=100 /3-- =100 a=100; 14C--4.3e-9 16

/3+=90.9 17; a=9.1 17; /3--<1.6#

a=100; 2/3 + ? a,~, 100; fl+ =0.1# ot=100

,,ic ,,ic

~ t

G. Audi et al . /Nuclear Physics A 624 (1997) 1-124 1 0 1


225Rn 26490# 300# 4.5 m 0.3 7 / 2 - 90 /3 -=100 225Fr 23853 10 4.0 m 0.2 3 / 2 - 90 /3 -=100 225Ra 21987 3 14.9 d 0.2 1/2 + 90 /3--=100 225Ac 21630 8 10.0 d 0.1 ( 3 / 2 - ) 90 93Bo26 D a=100; 14C=6.0e-10 13 225Th 22301 7 8.72 m 0.04 (3/2) + 90 tr ~90; e ~ 1 0 225 Pa 24330 70 1.7 s 0.2 5/2 - # 90 or= 100 225U 27370 50 94 ms 12 5 /2+# 90 94An02 T a=100 225Np 31580 70 > 2 ,us 9 / 2 - # 94Ye08 TD ot=lO0

.225 Rn T : 4.66(0.04) m in post cut-off date 97Bu03

.225U T : average 94An02=68(+45-20) 92To02=95(15) 89He13=80(+40-10)

226Rn 28770# 400# 7.4 m 0.1 0 + 96 226Fr 27330 90 49 s 1 1 - 96 226Ra 23662.3 2.5 1.600 ky 0.007 0 + 96 90We01 D 226Ac 24303 4 29.37 h 0.12 (1) {-#) 96 226Th 23186 5 30.57 m 0.10 0 + 96 226pa 26019 12 1.8 m 0.2 96 226U 27330 19 150 ms 30 0 + 96 96Uu.B T 226Np 32720# 90# 35 ms 10 96

• 226Ra D : I4C: average 90We01=2.3(0.8)e-9 86Ba26=2.9(1.0)e-9 85Ho21=3.2( 1.6)e-9 • 226U T : average 96Uu.B=130(30) 90An22=200(50)

/3 -=100 / 3 - =100 a=100; 14C=2.6e-9 6; 2 /3- ? / 3 - = 83 3; ~=17 3; a=0.006 2 a=100 ot=74 5; ~'+ =26 5 t~=100 a= 100

227Rn 32980# 420# 227 Fr 29650 100 227Ra 27172.3 2.5 227 Ac 25846.1 2.7 227Th 25801.3 2.8 227pa 26821 8 227U 29007 17 227Np 32560 70

• 227Th J : post cut-off date 97Mu08 JTr=l/2+

22.5 s 0.7 92 2.47 m 0.03 1/2 + 92 42.2 m 0.5 3/2 + 92

21.773 y 0.003 3 / 2 - 92 18.72 d 0.02 (1/2 + ) 92 38.3 m 0.3 ( 5 / 2 - ) 92 1.1 m 0.1 (3/2 + ) 92

510 ms 60 5 / 2 - # 92

/ 3 - = 100 /3--=100 /3-=100 /3-=98.62 36; a=1.38 36 a=100 ot=85 2; e=15 2 a=100; /3+<0.001# ot~ 100; fl+--0.05#

228Rn 35480# 470# 228Fr 33280# 200# 228Ra 28936.0 2.5 228Ac 28890.1 2.6 22gTh 26763.1 2.7 228pa 28911 5 228U 29218 16 228Np 33700# 200# 228 Pu 36070 30

• 228Ac D : post cut-off date ENSDF'97: t~ Was misassigned, removed; J'n=3+ • 228Th T : 1.9116(0.0016) in post cut-off date ENSDF'97 • 228pa J : 3 + and a=2.0(0.2)% in post cut-off date ENSDF'97 • 228Np D : /3+ SF---0.020(9)% defined by 94Kr13 relative to e, thus 0.012(6)% of total • 228Np D : a=40(+8-6 )% /3+---60(+6-8)% derived from f l+ / a= l . 5 (4 ) , in 94Kr13 • 228Np J : 0 + in ENSDF is a misprint. Corrected in post cut-off date ENSDF'97

65 s 2 0 + 89Boll TD /3 -=100 39 s 1 2 - 87 /3 -=100

5.75 y 0.03 0 + 87 /3-- = 100 6.15 h 0.02 3 (+) 94 /3--=100; of=5.Se~ 22 *

1.9131 y 0.0009 0 + 87 93Bo20 D ot=100; 200=1.13e-l l 22 * 22 h 1 (3 + ) 87 /3+---98.15 17; a=1.85 17 * 9.1 m 0.2 0 + 87 ot >95; e<5

61.4 s 1.4 87 94Kr13 TD /3+=59 7; a=41 7; fl+SF---0.012 6 * > 2 ,Us 0 + 94An02 TD a ~ 1 0 0 ; fl+=0.1#

229Fr 35790# 360# 229Ra 32430 60 229 Ac 30670 50 229Th 29579.9 2.9 229Thin 29579.9 2.9 0.0035 0.0010 229 Pa 29890 9 229U 31201 8 229Np 33760 90 229pu 37390 70

50.2 s 0.4 1/2 + # 90 92Bo05 T / 3 - =100 4.0 m 0.2 5/2 t+~ 90 /3 -=100

62.7 m 0.5 (3/2 + ) 90 / 3 - =100 7.34 ky 0.16 5/2 + 90 a=I00 70 h 50 3/2 + 94He08 T IT ?

1.50 d 0.05 (5/2 + ) 90 e,~100; ot---0.48 5 58 m 3 (3/2 + ) 90 /3+~,80; ot~,20 4.0 m 0.2 5 / 2 - # 90 or>50; fl+ <50 > 2 /zs 3 /2+# 94An02 TD a=100

*229Thin D : IT decay has been observed in post cut-off date 97Ir.1 as ultraviolet y-ray emission

1 0 2 G. Audi et al./Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Hall-life f i r Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

230Fr 39600# 450# 19.1 s 0.5 93 / 3 - =100 23°Ra 34540 30 93 m 2 0 + 93 , 0 - =100 230Ac 335611 100 122 s 3 ( 1 + ) 94 , 0 - =100

230Th 30857.2 2.0 75.38 ky 0.30 0 + 93 tt=100; SF<Se-II ; 24Ne=5.6e-ll t0

2~pa 32167 3 17.4 d 0.5 ( 2 - ) 93 ,0+---91.6 13 ; /3 -=8 .4 13; a--0.0032 1 230U 31603 5 2(/.8 d 0 + 93 a=100; SF<L4e-10#; 2/3 + ? 230Np 35220 50 4.6 m 0.3 93 /3+ <97; a>_3 230pu 36930 24 > 200 ms 0 + 93 90An22 T or=?;/3+ ?

231Fr 42300# 520# 231Ra 3840(1# 300# 231Ac 35910 100 231Th 33810.5 2.0 231Pa 33421.0 2.6 231U 33803 4 231Np 35610 50 Z~I Pu 38430# 100# 231 Am 42440# 300# 10# s

*231pa D : . . . ; 24Ne=13.4e-10 17; 23F=10.0e-13 +5.04).7

17.5 s 0.8 1/2+# 94 / 3 - = 100 103 s 3 1/2+# 94 , 0 - = 100 7.5 m 0.1 (1/2 + ) 94 / 3 - = 100

25.52 h 0.01 5/2 + 94 /3 - =100; a~ , le-8 32.76 ky 0.11 3 / 2 - 94 92Pv05 D a=100; SF<3e-10; . . .

4.2 d 0.1 (5/2)/+#1 94 94Li12 D e~100; a--0.004 1 48.8 rn 0.2 (5/2) (+#) 94 ,0+--98 1; or=2 1 3# m 3/2+# ,0+ ?; a ?

,0+ ?; a ?

232Fr 46250# 640# 232 Ra 40700# 360# 232Ac 39140 100 232Th 35443.7 2.0 232 Pa 35939 8 232U 34601.5 2.7 232Np 37350# 100# 232pu 38358 19 232Am 4_'3400#

5 s 1 90Me 13 T ,0--=100 250 s 50 0 + 91 ,0-- =100

119 s 5 (1 + ) 91 ,0--=100 14.05 Gy 0.06 0 + 91 95B018 D IS=I00.; a=100; SF=IIe-10 3; . . . 1.31 d 0.62 ( 2 - ) 91 / 3 - ~100; ~=0.003 1 68.9 y 0.4 0 + 91 90Bo16 D ot=100; 24Ne=8.ge-10 7; . . . 14.7 m 0.3 (4 + ) 91 /3+ .,~ 100; a~0 .003 34.1 m 0.7 0 + 91 ABBW D t,=?; a = l l # 1.31 m 0.04 91 /3+=?; or=2#;/3+SF=0.069 10

• 232Th D : . . . ; 24Ne+26Ne<2.78e-10; 2,0-- ? • 232U D : . . . ; 28Mg<5e-12; SF<Ie-12 • 232U D : 2~Ne: average, as adopted by 91Bo20. of 2 results from their group • 232pu D : derived from 1.6%# < ot < 20%#, in ENSDF

233Ra 44710# 470# 233Ac 41500# 300# 233Th 38728.6 2.0 233pa 37483.5 2,3 233U 36913.4 2,8 233 Np 37940 50 233 Pu 40040 50 233 Am 43290# 220# 233Cm 47320# 400#

• 233U D : . . . ; 28Mg<l.3e-13

30 s 5 l / 2 + # 90Me13 T / 3 - = 100 145 s 10 (1/2 + ) 90 f l - =100

22.3 m 0.1 1/2 + 90 f l - =100 26.967 d 0.002 3 / 2 - 90 13- =100 159.2 ky 0.2 5 /2 + 96 91Pr02 D ct=100; SF<6e-9; 24Ne=7.2e-ll 9; . . . * 36.2 m 0.1 (5/2 + ) 90 ,0+=100; a_0 .001 20.9 m 0.4 5 /2+# 90 fl+,~100; a---O.12 5 2# m /3 + ?; a ? 1# m 3/2+# /3+ ?; a ?

2"MRa 47090# 540# 234Ac 45100# 400# 234Th 40609 4

z',4 Pa 40336 5 234pare 40414 4 78.0 3.0 234U 38140.6 2.0 2~Np 39950 9 234pu 40338 7

234Am 44520# 210# 234Cm 46800# 300# 2# m 0 +

• 234U D : . . . ; SF=I.73e-9 10; 28Mg=l .4e- l l 3; 24Ne+26Ne--9e-12 7

30 s 10 0 + 94 /3-- =100 44 s 7 94 /3-- =100

24.10 d 0.03 0 + 94 / 3 - =100 6.70 h 0.05 4 + 94 78Ga07 D f l - = 100 ; SF<3e-10 1.17 m 0.03 ( 0 - ) 94 78Ga07 D f l - ~ 1 0 0 ; IT=O.16 4; SF<Ie-10

245.5 ky 0.6 0 + 94 IS=0.0055 5; ot=100; . . . 4.4 d 0.1 (0 + ) 94 /3+ =100 8.8 h 0.1 0 + 94 ~,~94; a~,~6

2.32 m 0.08 94 90Ha02 D ,0+~100; ot=:0.039 12; /3+SF=0.0066 18

,0+ ? ; a ?


Nuclide Mass excess Excitation Half-life f i r Ens Reference Decay modes and intensifies (keV) energy(keV) (%)

235Ac 47600# 420# 235Th 44251/ 50 235 Pa 42320 50 235U 40914.1 2.0 235um 40914.2 2.0 0.0768 0.0005 235Np 41037.8 2.1 235pu 42179 21 235Am 44740# 210# 235Cm 48060# 220# 235 Bk 52700# 400#

• 235U D : . . . ; 24Ne+25Ne=Se-lO 4

40# s 1/2+# / 3 - ? 7.1 m 0.2 (1/2 + ) 93 / 3 - = 100

24.5 m 0.2 ( 3 / 2 - ) 94 /3 -=100

703.8 My 0.5 7 / 2 - 93 IS=0.720 1; a=100; SF=7e-9 2; . . . * 25 m 1/2 + 93 IT=100

396.1 d 1.2 5/2 + 94 ~ 1 0 0 ; ot---0.00260 13 25.3 m 0.5 (5/2 + ) 93 f l+~100; oc---0.0027 5

15 m 5 5 / 2 - # 93 96Gull T f l+~100; a, ? 5# m 5 /2+# 93 /3+ ?; ot ? 20# s /3+ ?; ot ?

236Ac 51400# 500# 236Th 46310#

Z~6 Pa 45M0 2(;0 236U 42440.6 1.9 236Np 43370 50 2-~6 Npn' 4M30 7 60 236pu 42893.5 2.7

2~Am 46170# 100# 236Cm 47880# 200# 236Bk 53400# 400#

50

2# m / 3 - ? 37.5 m 0.2 0 + 91 / 3 - = 100 9.1 m 0.1 1 ( - ) 91 / 3 - = 1 0 0 ; / 3 - SF---6e-8 4

23.42 My 0.03 0 + 91 oz=100; SF--9.6e-8 6 * 154 ky 6 ( 6 - ) 91 e=87.3 5; f l - =12.5 5; or---0.16 4 * 22.5 h 0.4 1 91 e=52 1 ; /3 - - -48 1

2.858 y 0.0118 0 + 91 90Og01 D a=100; SF=I.36e-7 4; . . . 30# m 91 /3+ ?; a ? 10# m 0 + 91 fl+ ?; ot ? 1# m /3+ ?; a ?

• 236pa D : / 3 - SF decay questioned by 90Ha02 • 236U D : and Ne+Mg < 4e-10%, from 89Mi.A • 236pu D : . . . ; 28Mg=2e-12; 2fl + ?

237Th 50200# 360# 237 Pa 47640 100 237 U 45386.1 2.0 237Np 44867.5 2.0 237pu 45087.8 2.3 237pure 45233.3 2.3 145.544 0.010 237 Am 46550 50 237Cm 49270# 210# 237Bk 53210# 300# 237Cf 57820# 500# 2.1 s 0.3 5 /2+#

• 237Np D : and cluster (Z=I0-14) < 1.8e-12%, from 92Mo03

5.0 m 0.9 5 / 2 + # 93Yu03 TD /3--=100 8.7 m 0.2 11/2 + ) 95 / 3 - = 100

6.75 d 0.01 1/2 + 95 / 3 - =100 2.144 My 0.007 5/2 + 95 89Pr.l D a=100; SF_<2e-10; 3°Mg<4e-12 * 45.2 d 0.1 7 / 2 - 95 ,e~l~O; a--0.0042 4 180 ms 20 1/2 + 95 IT=I00

73.0 m 1.0 5 / 2 / - ) 95 /3+~100; a--0.025 3 20# m 5 /2+# 95 /3+ ?; a ? 1# m 7/2 + # i f - ?; t~ ?

95La09 'rD ot ?; SF~,-~10; ~ ?

238Th 52390# 360# 238pa 50760 60 238U 47303.7 2.0 238Np 47450.7 2.0 238pu 46158.7 2.0 238 Am 48420 50 238Cm 49380 40 238 Bk 54270# 290# 238Cf 57200# 400#

• 238U D : . . . ; SF=5.45e-5 7; 2 /3-=2.2e-10 7

20# m 0 + 13- ? 2,3 m 0.1 ( 3 - ) 88 85Ba57 D /3-=100; /3-SF<2.6e~6

4.468 Gy 0.003 0 + 88 86Lo.A D IS---99.2745 15; a=100; . . . 2.117 d 0.002 2 + 88 /3 -=100 87.7 y 0.3 0 + 95 89Wa10 D a=ll~O; SF=I.9e-7 1; . . . 98 m 2 1 + 88 fl+=100; a=l .0e~[ 4 2.4 h 0A 0 + 88 e>90 ; ot<10 2.4 m 0.1 92Kr.C TD at ?; ,8+ ?; /3+SF=0.048 2 21 ms 2 0 + 95La09 TD SF~_,I00; a ?; ~ ?

• 238U D : 2 f l -=2 .2 (7 )e -10% derived from 2 /3- halfqife T=2.0(0.6) Zy. in 91Tu02 • 238pu D : . . . ; 32Si,-~1.4e-14; 28Mg+30Mg~6e-15

239pa 53220# 239U 50568.7 2.0 239Np 49305.3 2.1 239pu 48583.5 2.0 239Am 49386.4 2.8 239Cm 51190# 100# 239Bk 54360# 290# 239Cf 58290# 230#

• 239Cf T : symmetrized from 391+37-12)

106 m 30 1 /2+# 95Yu01 TD f l - =100 23.45 m 0.02 5/2 + 92 /3-- =100

2.3565 d 0.0004 5/2 + 92 / 3 - =100 24.11 ky 0.03 1/2 + 92 a=100; SF=3,1e-10 6 11.9 h 0.1 (5 /2 ) - - 92 e~100; o~--0.010 1 2.9 h 1 7 / 2 - ) 92 /3+~100; a<0.1 3# m (7/2 + ) 92 ff~- ?; o~ ? 55 s 26 5 /2+# 92 81Mu12 D ct=7; 15 + ?


Nuclide Mass excess Excitation Half-life .fir Ens Reference Decay modes and intensities (keV) energy(keV) (%)

240pa 56800# 300# 240U 52709 5 2'lONp 52321 15

2'1° Np"* 52341 21 24°pu 50121.3 1.9 2~Am 51500 14 240Cm 51715.7 2.7 "?AO B k 55660# 150# 2AOcf 58030# 200# 240Es 64200# 400#

20 15

2# m / 3 - ? 14.1 h 0.1 0 + 96 /3-=100; o~< le-10

* 61.9 m 0.2 (5 + ) 96 /3 -=100 * 7.22 m 0.02 1 (+t 96 81Hs02 E / 3 - ~ 1 0 0 ; IT=O.11 3

6.564 ky 0.011 0 + 96 89Pr.l D ot=100; SF=5.7e~. 2; 34Si<1.3e-13 50.8 h 0.3 ( 3 - ) 96 /3+=100; o t~ l .9e~. 27 d 1 0 + 96 t ~ 1 0 0 ; e<0.5; SF=3.9e~ 8

4.8 m 0.8 96 /3~ ?; ot=10#; fl+SF=0.0020 13 1.06 m 0.15 0 + 96 95La09 D a,~98; SF~2; /3+ ? 1# s ot ?;/3+ ?

*2'lOBk D : symmetrized from /3+SF=0.0013(+18-7)%

241U 56200# 3(~0# 5# m 7 /2+# / 3 - ? 241Np 54260 70 13.9 m 0.2 (5/2 + ) 94 /3 -=100 2A'Ipu 52951.0 1.9 14.35 y 0.10 5/2 + 96 /3--.-"¢100; a=0.00245 2; SF<2Ae-14 241Am 52930.2 2.0 432.2 y 0.7 5/2-- 94 a=100; SF=4.3e-10 18; 34Si<7Ae 14 241Cm 53697.6 2.3 32,8 d 0.2 1/2 + 94 t,=99.0 1; ot=l.0 1 241Bk 56100# 200# .'~ m (7/2 + ) 94 a ?;/3+ ?

241Cf 59350# 260# 3.8 m 0.7 7 / 2 - # 94 / 3 + ~ 7 5 ; o t ~ 2 5 241Es 63960# 300# 10 s 5 ( 3 / 2 - ) 96Ni09 TJD o,=?;/3+ ?

*HIEs T : symmetrized from 8 ( + 6 4 )

242U 58610# 200# 242Np 57410# 210# 242 Npm 57410 200 O# 50# 242pu 54713.0 2.0 242Am 55464.0 2.0

242 Amm 55512.6 2.0 48.63 0.05 7A2 Am" 57660 80 2200 80 242Cm 54799.2 2.0 242Bk 57800# 200# 242Cf 59330 40 242Es 64920# 330# 242 Fm 68400# 400#

• 242Cf D : SF < 0.014% from 95La09 • 242Es T : average 96Sh.A=25(2) 96Ni09=16(+6~.)

16.8 m 0.5 0 + 85 /3 -=100 * 5.5 m 0.1 (6) (+#) 85 /3 -=100 * 2.2 m 0.2 ( 1 + ) 85 / 3 - =100

373.3 ky 1.2 0 + 96 86Lo.A D a=100; SF=5.49e-4 8 16.02 h 0.02 1 - 96 /3--=82.7 3; e=17.3 3 141 y 2 5 - 96 ITml00; o~--0.459 12; SF=I.5e-8 6 14.0 ms 1.0 (2, 3) 96 95Ba.A J SF,.~I00; IT--?

162.8 d 0.2 0 + 96 86Lo.A D a=100; SF=6.33e~ 13; 2/3 + ? 7.0 m 1.3 2 - # 85 80Ga07 D /3+=100;/3+SF<3e-5

3.49 m 0.12 0 + 85 81Mu12 D or=80 20;/3+ ?; SF<0.014 23.9 s 2.8 96Ni09 TD a=?; ~'+=?; /3+ SF--0.6 800 #s 200 0 + 85 SF=?; oL ?

• 242Es D : /3+SF=0.6% assuming ot and/3+ are equal, from 94Ke.B; a from 96Ni09

243Np 59870# N ~ 243pu 57750 3 243Am 57168.3 2.2 243Cm 57177.2 2.2 243Bk 58686 5

~ 3 C f 60940# 140# 243Es 64860# 290# 243Fm 69410# 240#

• 243Fm T : symmetrized from 180(+80-40)

1.85 m 0.15 ( 5 / 2 - - ) 93 /3--=100 4.956 h 0.003 7 /2 + 93 13-=100 7.37 ky 0.04 5 / 2 - 93 a=100; SF=3.Te-9 2 29.1 y 0.1 5/2 + 93 o~100; ~--0.29 3; SF=5.3e-9 9 4.5 h 0.2 ( 3 / 2 - ) 93 /3+~100; old0.15 10.7 m 0.5 (1/2 + ) 93 /3+~86; o ~ 1 4 21 s 2 3 / 2 - # 93 /3 + '<70; a > 3 0

210 ms 60 7 / 2 - # 93 ABBW D ~t=60 40; /3+ ?; SF--0.57#

• 243Fm D : et---40(20)% if ct branching of 239Cf is 10(1%, see ENSDF

244Np 63200# 300# 244pu 59800 5

24'lAm 59875.9 2.1 244Atom 59961.6 2.2 85.8 0.9 RQ 244Cm 58447.8 1.9

244Cmm 59488.0 1.9 1040.181 0.011 244Bk 60703 14 244Cf 61470 3 244Es 66110# 180# 244Fm 69000# 280#

2.29 m 0.16 ( 7 - ) 87Mo29 TJD /3--=100 80.8 My 1.0 0 + 96 92Mo25 D ora l00; SF=0.123 6; 2 /3- <7.3e-9 10. l h 0.1 ( 6 - - ) 96 /3--=100 26 m 1 ~ 96 / 3 - ,~100; e=0.0361 13

18.10 y 0.02 0 + 96 ot=100; SF=t.347e~. 8 34 ms 2 6 + 96 IT=t00

4.35 h 0.15 ( 1 - ) 87 /3+ ~,-'~100; oz=O.O06 2 19.4 m 0.6 0 + 87 a ~,-~, 100; • ~,.~ 1 37 s 4 87 80Gaff'/ D 13 + ?; ct=5 3; /3+SF--O.OI 3.3 ms 0.4 0 + 87 SF~99; ot~ 1

• 244pu T : and T (2 /3 - ) > 1.1 Ey, from 92Mo25; thus 2/3- < 7.3 e-9% • gA4Es D : symmetrized from a----A(+3-2)%

~t

:,it :,it*



2ASpu 63098 14 245Am 61893 4 245Cm 60999.4 2.7

2ASBk 61809.6 2.5 245Cf 63380# 100# 245Es 66430# 200# 245Fm 70210# 280#

~5Md 75470# 380# 245Mdm 75570# 360# 100# 100#

*245Mdm T : symmeu'ized from 350(+230-160)

10.5 h 0.1 (9/2--) 93 2.05 h 0.01 (5/2) + 93 8.5 ky 0.1 7/2 + 93

4.94 d 0.03 3 / 2 - 93 45.0 m 1,5 (5/2 +) 93 1.1 m 0.1 ( 3 / 2 - ) 93 4.2 s 1.3 l /2 + # 93

* 900 us 250 1 / 2 - # * 400 ms 200 (7/2 + )

,8-=100 ,8-=100 o'=100; SF=6.1e-7 9 e~100; a=O.12 1 ,8+ =64 3; a=36 3 /3+--60 10; a=40 10 et=?; /5'+--4.2#; SF=0.13#

96Ni09 TJD SF=?; a ?

96Ni09 TJD a=?; ,8+ ?

246pu 65389 15 246Am 64989 18 246Am"~ 65019 15 30 10 2A6Cm 62612.7 2.2 246Bk 63960 60 246Cf 64085.7 2,2 246Es 67970# 220# 246Fm 70120 40 246Md 76320# 390# :?A6Mdm 76530# 390# 210 70 EU

10.84 d 0.02 0 + 90 '8-- =100 39 m 3 ( 7 - ) 90 /3-=100

25.0 m 0.2 2 ( - ) 90 84So03 E ' 8 -~100 ; IT<0.01 4.73 ky 0.10 0 + 90 e~,.~100; SF=0.02614 5 1.80 d 0.02 2 ( - ) 90 '8+~100; o,<0.2 35.7 h 0.5 0 + 90 o'=100; SF=2.0e~. 2; e<5e-4 7.7 m 0.5 4--# 90 '8+=90.1 18; o'=9.9 18; fl+SF=0.003 1.1 s 0.2 0 + 90 96Ni09 D ~=?; '8+ >10; SF-=4.5 13; ,8+SF=10 5 1.0 s 0.4 96Ni09 TD ct=?; ,8+ ? 1.0 s 0.4 93Ho.A TD ct=?; ,O + ?

*2A6Mdm I : No longer considered to exist. Kept for consistency with AME'95

2A7pu 69000# 300# 7ATAm 67150# 100# 247Cm 65528 4 247 Bk 65483 6 247Cf 66129 8 247 Es 68600# 30# 247Fm 71560# 150# 247 Fmnt

247 Md 76200# 370# 247Md m 76250# 350#

non existent EU

50# 100# Nm * 1.12 s 0.22 (7/2 +)

2.27 d 0.23 1/2+# 93 ,8-=100 23.0 m 1.3 5/2# 93 ,8- =100 15.6 My 0.5 9 / 2 - 93 oz=100 1.38 ky 0.25 ( 3 / 2 - ) 93 a~lO0; SF ? 3.11 h 0.03 7/2+# 93 .~.~,100; a=0.035 5 4.55 m 0.26 7/2+# 93 ,8+~-,93; o'~7; SF,'~,9e-5# 35 s 4 5/2+# 93 a>_50; fl+ --<50 9.2 s 2.3 93 67Fl15 I tz,~100; IT ?

* 270 ms 160 I / 2 - # 93 93Ho.A TEl SF=?; o" ? 93Ho.A TD o'=100; SF=0.0001#

• 247Fm m I : existence of this isomer is discussed in ENSDF • 247Md T : symmetrized from 230(+190-120)

248 Am 70560# 200# 248Cm 67386 5 2ASBk 68070# 70# 248 Bkm 68103 21 2A8cf 67233 5 2ASEs 70290# 50# 248 Esn~

248Fm 71897 12 248 Md 77230# 24O#

30# 70#

non existent RN

10# m 90 340 ky 4 0 + 90

* > 9 y (6 + ) 90 * 23.7 h 0.2 1 ( - ) 90

333.5 d 2.8 0 + 90 27 m 4 2--#.0+# 90 41 m 36 s 3 0 + 90 7 s 3 90

89Ha27 I

B - =100 o'--91.74 3; SF=8.26 3; 2 f l - ? at>70 ,8-=70 5; e=30 5; o'=0.001 oral00; SF=0.0029 3 ,8+ ~,~100; a~0.25; ~+SF=3e-5

o'--99 1; ~+~1; SF,~0.05

~+ =80 10; o'=20 10; ,8+ SF<0.05

249Am 73100# 300# 249Cm 70744 5 7AgBk 69843 3

7AgCf 69719.4 2.8 249 Es 71170# 30# 249Fm 73610# 140# 249Md 77320# 220# 249No 81810# 340#

2# m 64.15 m 0.03 1/2 (+) 90 320 d 6 7/2 + 90 351 y 2 9/2-- 90

102.2 m 0.6 7/2 (+) 90 2.6 m 0.7 (7/2 + ) 90 24 s 4 7/2# 90

5/2 + #

' 8 - ? '8-=100 ' 8 -~100 ; a--0.00145 8; SF=47e-9 2 ot=lO0; SF=5.2e-7 2 '8+~100; a=0.57 8 /3+=85#; a=? a>60; fl+ ?

B+ ? ; a ?

~t


Nuclide Mass excess Excitation Half-life ,or Ens Reference Decay modes and intensities ( keV ) energy( keV ) ( % )

2~Cm 72983 11 9# ky 0 I- 90 SF~80; ot~ 11; / 3 - ~ 9 250Bk 72946 4 3.217 h 0.005 2 - 90 /3 -=100 25°Cf 71166.1 2.2 13.08 y 0.09 0 + 90 ora l00; SF--0.077 3 250Es 73270# 100# * 8.6 h 0.1 (6 + ) 90 /3+ >97; 0"<3 250Esm 73470# 180# 200# 150# * 2.22 h 0.05 1 ( - I 90 a~99; 0"<1 250Fm 74068 12 30 m 3 0 + 90 0">90; e<10; SF~0.0(I06 250Fmm 75570# 300# 1500# 300# 1.8 s 0.1 7, 8# 90 IT>80 25OMd 78700# 300# 52 s 6 90 /3+---93 3; a=7 3; /3+ SF---O.02 250No 81500# 200# 250 /.t,s 50 0 + 90 SF~100; 0'--0.05#; /3+----0.00025#

ZSlCm 76641 23 16.8 m 0.2 (1/2 + ) 90 /3-=11~1 25IBk 75221 11 55.6 m 1.1 ( 3 / 2 - ) 90 /3-=100; a ' ~ l e 5 251Cf 74128 5 900 y 40 1/2 + 90 0"=100 251Es 74504 6 33 h 1 ( 3 / 2 - ) 90 ~,-~100; o,--0.49 12 25tFm 75979 8 5.30 h 0.08 ( 9 / 2 - ) 90 /3+---98.20 13; o~=1.80 13 251Md 79100# 200# 4.0 m 0.5 90 /3~ >90; a < 1 0 251No 82870# 180# 800 ms 300 7/2 j # 90 or=?; SF<I0#; /3+=10 251Lr 87900# 300# / ~ ?; o, ?

252Cm 79060# 300# < 2 d 0 + 90 / 3 - =100 252Bk 78530# 200# 1.8 m 0.5 9(1 92Kr.A TD /3--=?; ot ? 252Cf 76028 5 2.645 y 0.008 0 + 90 o~--96.908 8; SF=3.092 8 252Es 77290 50 471.7 d 1.9 ( 5 - ) 90 a=76 4; e=24 2; / 3 - ~ 0 . 0 1 252Fm 76811 6 25.39 h 0.05 0 + 90 ora l00; SF--0.0023 2; 2/3 + ? 252Md 80700# 200# 2.3 m 0.8 90 /3+>50; 0"<50 252No 82871 13 2.30 s 0.22 0 + 90 0"=73.1 19; SF=26.9 19; ./3+<1 252Lr 88800# 300# 1# s 90 or=90#; /3+=10#; SF<I#

253Bk 80930# 360# 10# m 91Kr.A I 253Cf 79295 6 17.81 d 0.08 (7/2 + ) 90 253 Es 79007 3 20.47 d 0.03 7/2 + 90 253Fm 79341 5 3.00 d 0.12 1/2 + 90 253Md 81300# 210# 6.9 m 0.9 7 / 2 - # 90 90Ka.A TD 253No 84440# 250# 1.7 m 0.3 ( 9 / 2 - ) 90 253Lr 88730# 230# 1.5 s 0.5 90 253Db 93780# 450# 13 ms 5 (7/2) (+#1 90 95Ho.B TJ

• 253Bk I : possible identification, in 91Kr.A. Needs confirmation • 253Md T : symmetrized from 6.4(+1.2-0.41 • 253Lr T : symmetrized from 1.3(+0.6-0.3) • 253Db T : symmetrized from 11(+6-3)

/3 - ? * /3 - ~,-"~100; a'=0.31 4 0"=100; SF=8.7e~ 3 e=88 1; o'=12 1

/3+=?; a ? * or=?;/3+=20#; SF=0.001# a=90 10; SF ?;/3+=1# * SF~50; o,~50 *

2 ~ B k 84390# 300# 2# m 254Cf 81335 12 60.5 d 0.2 0 + 90 254Es 81986 4 275.7 d 0.5 (7 ~ ) 90

254Esm 82070 4 83.8 2.5 AD 39.3 h 0.2 2 + 90 254Fm 80898 3 3.240 h 0.002 0 + 90 254Md 83580# 100# * 10 m 3 ( 0 - ) 90 254Mdm 83630# 140# 50# 100# * 28 m 8 ( 3 - ) 90 254No 84718 18 55 s 3 0 + 90

2~Nom 85220# 100# 500# 100# 280 ms 40 90 2~Lr 89970# 340# 13 s 2 90 254Db 93300# 290# 23 /Ls 3 0 ~" 90 95Ho.B T

• 2~Es D : . . . ; S F < 3 e ~ • 254Esm D : . . . ; ~=0.078 6; SF<0.045

• 2-~INo D : symmetrized from SF=0.25(+20-111%

B - - ?

SF~,-~,I00; o,--0.31 2; 2fl-- ? o'=100; e < l e ~ # ; fl--=l.74eqS; . . . * / 3 - = 98 2; IT<3; ot--0.33 1; . . . * a~ 100 ; SF--0.0592 2 13 + ~ 100; a ? /3 + ~ 100; a ? 0"=?; /3+=10 4; SF=0.31 16 * IT>80; at ? 0"=78 6; /3~ =22 6; SF<0.1 SF,~ 100; ot ~0 .3

*:,,g

G. Audi et al . /Nuclear Physics A 624 (1997) 1-124 1 0 7

Nuclide Mass excess Excitation Half-life f ,r Ens Reference Decay modes and intensities ( keV ) energy ( keV ) ( % )

255Cf 84800# 200# 85 m 9 / 2 + # 90 ,8 -=100; SF<0.001#; a=le-5# 255Es 84083 11 39.8 d 1.2 7/2 + 90 ,8-----92.0 4; a=8.0 4; SF=0.0041 2 ZSSFm 83793 5 20.07 h 0.07 7/2 + 90 a=100; SF=2.4e-5 255Md 84836 7 27 m 2 ( 7 / 2 - ) 96 ,8+---92 2; a=8 2; SF<0.15# 255No 86845 12 3.1 m 0,2 ( I / 2 + ) 90 a--61.4 25; ff~-=38.6 25 255Lr 90140# 210# 22 s 4 90 a=?; ,8 + <30/#; SF<I# 255Db 94540# 210# 1.5 s 0.2 ( 9 / 2 - ) 90 SF=52 7; a---48 7 255ji 100040# 420# 1,7 s 0.5 90 a,~80; SF~,~-,20

• 255j1 T : symmetrized from 1.6(+0.6-0.4)

256Cf 87040# ,~}0# 256Es 87180# 100# * 256Esm 87180# 140# 0# 100# * 256Fm 85480 7 256Md 87610 50 256No 87817 8 256[,1" 92000# 220# 256Db 94248 27 256j1 100700# 360#

• 256No D : symmetrized from SF=0.53(+6-3)% • 256Db D : symmetfized from a=2.2(+7.3-1.8)% • 256ji T : symmetrized from 2.6(+1.4~0.8)

12.3 m 1.2 0 + 90 SF=100; , 8 - < 1 # ; a = l e ~ # ; 2 . 8 - ? 25.4 m 2.4 ( 1 + ) 90 , 8 - =100 7.6 h (8 + ) 90 89Hal0 D , 8 - ~-, 100; , 8 - SF--0.002

157.6 m 1.3 0 + 90 SF=91.9 3; a=8.1 3 78.1 m 1.8 ( 1 - ) 90 93Mo18 T.ID ,8+=89 3; a = l l 3 2.91 s 0.05 0 + 90 90Ho03 'I'D a,~,100; SF=0.55 5; ~<0.01# 28 s 3 90 a>80; ,8+ <20; SF<0.03 6,7 ms 0.2 0 + 90 SF=?; a=6 5 3.0 s 1.1 90 a < 9 0 ; SF<40; ,8+,~ 10

257Es 89400# 410# 257 Fm 88584 6 257 Md 88990 3 257 No 90220 30 257Lr 92780# 210# 257Db 96010# 270# 257j1 100470# 230#

• 257ji T : symmetrized from 1.3(+0.5-0,3)

2# h 90 , 8 - ? ; a ? 100.5 d 0.2 (9/2 + ) 90 a~ 100 ; SF=0.210 4 5.52 h 0.05 ( 7 / 2 - - ) 96 93Mo18 TD ~=84-.8 26; a=15.2 26; SF<I 25 s 2 (7/2 + ) 90 a ~ t 0 0 ; f l + < l

646 ms 25 (9/2 + ) 90 a,~,100; ,8+=0.01#; SF=0.001# 4.7 s 0.3 (1/2 + ) 90 95Au04 J a=79.6 20; ,8+=18 2; SF=2.4 3 1.4 s 0.4 90 a=82 11; SF=17 11; ,G+=I#

258Es

258Fm 90420# 200# 258Md 91683 5 * 258Mdm 91680# 200# 0# 200# * 258No 91470# 200# 258Lr 94900# 100# 258Db 96470# 200# 258jl 101940# 340# * 258j1" 102000# 350# 60# 100# * Z'i8 R f 105400# 410#

• 258Fm T : supersedes 86Hu05=370(43) from same group • 258Md D : derived from: "the sum of SF, ¢ and , 8 - decay branches <0.003%"in 93Mo18 • 258Md D : and T(SF)>150G00 y, from ENSDF. thus SF<Ie-4%# • 258Mdm D : SF<20% derived from 93Mo18 "the sum of SF and , 8 - decay branches < 30%" • 258j1 T : symmetrized from 4.4(+0.9-4).6) • 258j1 D : symmetrized from a---'67(+5-9)% and .8+=33(+9-5)% • 258Rf T : symmetrized from 2.9(+1.3-0.7)

90 B - ? ; a ? 360 /zs 20 0 + 90 89Hu.A T SF=I00 •

51.50 d 0.29 ( 8 - ) 90 93Mo18 TD a~,100; ,8+<0.0015; ,8,8-<0.0015 * 57.0 m 0.9 ( 1 - ) 90 93Mo18 TD *=?; SF<20; , 8 - <10#; a < l . 2 * 1.2 ms 0,2 0 + 90 89Hu09 T SF=100; a~ .001~, 2fl + '? 3.9 s 0.3 90 92Gr02 T a>95; fl+ <5 12 ms 2 0 + 90 SF,~87; a ~ 1 3

4.6 s 0.8 96 a=64 7; l~1~=36 7; SF<I# * 20 s 10 96 ¢,~ 100; IT ? 3.3 ms | .0 0 + 95Ho.B T SF~,-~100; a ? *

"zSgFm 93700# 280# 1.5 s 0.3 3 /2+# 90 SF=I00 259Md 93620# 200# 1.60 h 0.06 ( 7 / 2 - - ) 90 93Mo18 TD SF=?; a < l . 3 259No 94100# I00# 58 m 5 (9/2 + ) 90 a=75; ~=25; SF<IO 259 Lr 95940# 70# 6.3 s 0.4 90 92Gr02 T a,~,77; SF~,23; B + <0.5 259 Db 98390# 70# 2.7 s 0.4 7/2 + # 90 94Gr08 T a=93 4; SF=7 4; fl+ ~0 .3 Z';9jI 102210# 290# 1# s 90 a ? 259Rf 106800# 210# 580 ms 210 (1/2 + ) 90 a--90 10; SF<20

• 259Db T : avelage 94Gr08=1.7(+0.8-0.5) 81Be03=3.0(1.3) 73Dr10=3.2(0.8) • 259Db T : and 69Gh01=3.2(0.8) .259Rf T : symmea'ized from 480(+280-130)

1 0 8 G. Audi et al. /Nuclear Physics A 624 (1997) 1-124

Nuclide Mass excess Excitation Half-lil~ J ~ Ens Reference Decay modes and intensities (keV) energy(keV) (%)

260Fm I# ms

260Md 96550# 320# 27.8 d 0.8

260NII 95610# 200# 1(16 ms 8 0 + 90 260Lr 98340# 120# 3.0 rn 0.5 911 260Db 99140# 200# 20.1 ms (I.7 1) ~ 91)

260ji 103790# 230# 1.52 s 0.13 9(I 260Rf 106600 4(} 3.8 ms 0.8 0 + 90 260Bh 11 .'M60# 620# 90

*260Fm 1 : half-life ~ 4 ms and SF=I00 mode were reported in the 92Lo.B intemal *260Fro 1 : report. Not confirmed in subsequent experiment by same group (97Lo.A). *260Fm I : Discovery of this isotope is considered unproven. *260Md T : supet'sedes 86Hu01=31.8(0.5) of same group *260Rf T : symmetrized from 3.6(+0.9-0.6)

*~aSORf D : symmeaized from SF=50(+30-20)% and o,=5(1(+2(I-301%

04 9(I SF ? . 90 92Lo.B TD SF=?; or<5; e<5; / 3 - <3.5 *

SF=I00

o,=75 10; /3t ~15 ; S F < I 0 S F ~,-~,98; a~,~2

or_90; SF_<9.6 6; /3~ <2.5 SF=60 30; o,=40 30 a=100

261Md

261No 98500# 300# 3/24 #

261 Lr 99620# 200# 39 m 12 87Lo.A TD

261Db 101300# 110# 65 s 10 9 / 2+# 90 90He.A D 261Dbm 101300# 150# 0# 100# 5 s 3 /2+# 96Ho13 TD 261ji 104430# 230# 1.8 s 0.4 90

261Rf 108240# 280# 230 ms 30 7/2 +# 90 261Bh 113460# 240# 13 ms 4 9(I

*261Bh T : symmetrized li'om 11.8(+5.3-2.81

/ 3 - ? /3 ?; a ? SF=?; ct ?

a=?; /3+<14.0 1.4; S F < I 0

a=?; /3+ ? ot >50; SF<50 ot=95 5; SE<I0 0,--95 5; S F < I 0

262No 100150# 540# 5 ms 1 0 + 89Hu.A TD SF=?; / 3 - ? 262Lr 102180# 300# 3.6 h 0.2 89Hu.A TD /3+=?; ot ? 262Db 102390# 280# 2.06 s 0.19 0 + 90 96Lal l TD SF=I00; or<0.8 • 262 Db" 102990# 490# 600# 400# 47 ms 5 high 90 96Lal 1 1 SF=100 •

262j1 106330# 180# 34 s 4 90 SF=71 5; o=26 5; /3+=.'~# 262Rf 108500# 280# 10# ms 0 + 90 a ? ; /3 + ? 262Bh 114580# 380# 102 ms 26 9~) a > 8 0 ; SF'< 20 262Bh m 11490(1# 350# 320# 160# 8.11 ms 2.1 90 ot > 70; S F < 3 0

-262Db T : average 96La11=2.1(0.2) 94La22=1.2(+1.0-0.5) **

• 262Db D : SF=100 from 94La22; oz intensity limit is fl~m 96Lal I ** • 262Dbm 1 : assigned by 96Lal l to K-isomeric state , , .

263Lr 103760# 360# 0" ?

263Db 104830# 1911# 10 m 2 3 / 2 +# 93Gr.C TD SF=?; a=30

263j1 1117190# 170# 29 s 9 90 92Kr01 TD SF=56 14; a=?; ,8+=8 * 263Rf 110210# 120# * 81•1 ms 200 9 / 2 +# 90 SF~70 ; a ~ 3 0 263Rfm 110310# 100# 100# 70# Nm * 360 ms 120 3 /2+# 95Ho.A TJD 0"=?; IT ? • 263Bh 114710# 420# 200# ms ot ? 263Hn 119890# 37(1# 1# ms 7 / 2 +# a=100

• 263ji T : symmetrized from 27(+10-7) **

• 263j1 D : SF symmetrized from SF=57(+13-15)%; /3 ~ intensity is from 93Gr.C ** • 263Rf" T : symmetfiz~,d from 310(+160-80) **

264Db 106170# 4,50# 20# m 0 + 0" ? 264"ji 109430# 230# oz ? 264Rf 110780# 280# 40(0 ms 0 + 0" ? 264Bh 116190# 280# 700 ms 4011 95Ho04 TD 0"=?; fl+ ? 264Hn 119610 50 540 ,us ~ 0 + 9(I 95Ho.B T ct=lflO

• 264Bh T : symmetrized from 440(+600-1601

• 264Hn T : 95Ho.B (2 events 76 u s and 825 ,us) 87Mu15 ( 1 event 80/as) . Average of • 264Hn T : the 3 events : 327(+448 120) ,us, see 84Sc13

G. Audi et al./Nuclear Physics A 624 (1997) 1-124 1 0 9


265ji 110530# 280# a ? ~SRf 112770# 140# 16 s 9 3 /2+# 94La22 TD a_>50; SF ?

265Bh 116620# 380# 200# ms o~ ? 265Hn 121100# 300# 1.6 ms 9 /2+# 90 95Ho.B T a=100 7ASHnm 121500# 290# 400# 100# 1.2 ms 0.6 3 /2+# 95Ho.B T a~-,100; IT ?

265Mt 127210# 470# a ?

2~6Rf 113580# 290# 2~6Bh 118310# 350# 266Hn 121130# 410# 266Mt 128490# 350#

• 266Mt T : symmetfized from 3.& +6.1-1.3)

20 s 7 0 + 94La22 TD a > 5 0 ; SF ?

1# s a ? 20# ms 0 + a ?

6 ms 4 95 84Og03 D a=?; SF<5.5

267Bh 118990# 340# 15# s 267Hn 122750# 100# 50 ms 18 3 /2+# 267Hn m non existent EU 200 ms

267Mt 128110# 580# 267Xa 134090# 380# 10 ,us 8 9 /2+#

• 267Hn T : average 95Ho.A=60 ms (9 events) 95La20=19 ms (3 events)

• 267Hn m I : tentative only • 267Xa T : lifetime 4 /zs , thus 7"=2.8(+13.O-1.3). See 84Sc13

a ?

95Ho.A TD a=?; /3+ ? 95Ho.A TDI a=?; IT ?

a ?

95Gh04 TD a=?; /3 + ?

268Hn 123100# 410# 2# s 0 + 268Mt 129310# 320# 110 ms 70 268Xa 133700# 500# 0 +

*2/JSMt T : symmetrized from 70(+100-30)

95Ho04 TD

a ?

a=?; B + ? a ?

269Hn 124930# 420# 13 s 6 96Ho13 TD a=100

269Mt 129580# 550# 10# ms a ? 269Xa 135200# 290# 230 ~ 110 3 /2+# 95Ho03 TD a=?; /3 + ?

• 269Xa T : symmetrized from 170(+160-60)

270Mt 131080# 610# 2# s a ? 270Xa 134720# 650# 0 + a ?

a ?

95Ho.A TD a=?; fl+ ? 95Ho.A TD a=?; IT ?

271Mt 131550# 610# 271Xa 136070# 180# 1.2 ms 0.5 11/2- -# 271XanJ 136570# 350# 500# 300# AD 210 ms 170

*271Xa T : symmetrized from 1.1(+0.6-0.4) ,271Xa m T : symmetrized from 56(+270-26)

2.5 ms 1.3 0 + a ?

95Ho04 TD a=?; fl+ ? 222Xa 136290# 650# 272Xb 142960# 330#

• 272Xb T : symmetrized from 1.5(+2.0-0.5)

96Ho13 TD a=100 96Ho13 TD a,~,100; IT ?

a ?

273Xa 139020# 440# 170 ms 273Xa n' 139690# 670# 670# 510# 600 /as 400 273Xb

• 273Xa m T : estimated from 96La12=300(+1300-200) and 96Ho13=110

400 /zs 300 96Ho13 TD

274Xb 275 Xb 277 XC

• 277Xc T : symmetdeed from 240(+430-90)

a ? a ?

a=lO0

~t


References to the NUBASE table

R E G U L A R J O U R N A L S ( C O D E N ident if iers) A N D R E V I E W S

AAFPA ADNDA AENGA ANPHA APAHA ARISE ASJOA BRSPE CJPHA DANKA EULEE 1986-.. HYIND IANFA IJARA INUCA JINCA JPHGB JUPSA MPLAE NCIAA 1970-. NIMAE 1983-... NIMBE 1983-... NSENA NUIMA ...-1983 NUPAB 1967-... NUPBB 1967-... NUPHA 1957-66 PENUC PHRVA 1930-69 PHSTB 1970-... PPSOA PRLTA PRVCA 1970-... PRVDA 1970-... PSSAA PYLBB 1968-... PZETA RAACA RAEFB THISc YAFIA YTHLD ZENAA ZEPYA .. .- 1974 ZPAAD 1974-...

Annales Academiae Scientiarum Fennicae, series A VI Atomic Data and Nuclear Data Tables (USA) Atomnaya Energiya (USSR) Annales de Physique (France) Acta Physica Academiae Scientiarium Hungaricae Applied Radiation and Isotopes - IntJ. of Radiat. Appl. and Instrnm. - Part A (Great Britain) The Astrophysical Journal Bulletin of the Russian Academy of Sciences, Physics Canadian Journal of Physics Doklady Akademii Nauk SSSR Europhysics Letters (replaces JPSLB and NCLTA) Hyperfine Interactions Izvestiya Akademii Nauk SSSR, seriya Fizicheskaya International Journal Appl. Radiation and Isotopes (Eng) Inorganic Nuclear Chemistry Letters (Great Britain) Journal of Inorganic and Nuclear Chemistry (USA) Journal of Physics, G Nuclear Physics (Great Britain) Journal of the Physical Society of Japan Modern Physics Letters section A Nuovo Cimento A (Italy) Nuclear Instruments and Methods in Physics Research A (Netherlands) Nuclear Instruments and Methods in Physics Research B (Netherlands) Nuclear Sciences Eng. Nuclear Instruments and Methods (Netherlands) Nuclear Physics, section A (Netherlands) Nuclear Physics, section B (Netherlands) Nuclear Physics (Netherlands) Particle Emission from Nuclei, D.N. Poenaru and M.S. lva~cu eds. CRC Press Physical Review (USA) (not 1964 and 1965) Physica Scripta (Sweden) Proceedings of the Physical Society (Great Britain) Physical Review Letters (USA) Physical Review, section C (USA) Physical Review, section D (USA) Planet Space Sciences Physics Letters, section B (Netherlands) Pis'ma Zhurnal Eksperimental'noi i Teoreticheskoi Fysiki (USSR) Radiochimica Acta (Germany) Radiation Effects and Defects in Solids (Great Britain) Treatise on Heavy-lon Science, ed. D.A. Bromley Yadernaya Fizika (USSR) Chinese Journal of Nuclear Physics Zeitschrift fiir Naturforschung, part A (Germany) Zeitschrift fiir Physik (Germany) Zeitschrift fur Physik A (Germany)


R E P O R T S , P R E P R I N T S , THESIS , A B S T R A C T S , C O M M U N I C A T I O N S

AAAAA to be pd PrvCom AHW Mort PrvCom GAu Mon PrvCom JBI Mon PrvCom NDG Mon PrvCom Ref Th.- City AnRpt Institute AECL- AIEAD- CERN- CRN- CSNSM- GSI- INDC- IPNO-DRE ISOLDE- ITEP- JAERI- JYFL- LBL- LLNL- LNPI- ORNL- UCRL- Wallet Cards

To be published in journal AAAAA Private communication to A.H. Wapstra in given Month Private communication to G. Audi in given Month Private communication to J. Blachot in given Month Private communication to Nuclear Data Group in given Month Quoted by reference in question Dissertation from corresponding University Annual Report from Institute (or City) Chalk River Tandem Accelerator Super-Conducting Cyclotron report AIEA Data for Actinides European Organization for Nuclear Research, report Centre de Recherches Nucl6aires, Strasbourg Centre de Spectrom6tde Nucl6aire et de Spectrnm6trie de Masse Gemeinschaft Schwedonforschung, report International Nuclear Data Committee (IAEA), report Institut de Physique Nucldaire d'Orsay, report Isotope Separator on Line (CERN), report Institute of Theoretical and Experimental Physics, Moscow, report Japan Atomic Energy Research Institute Jyv~kyl~i University, report Lawrence Berkeley National Laboratory, report Lawrence Livermore National Laboratory, report Leningrad report Oak Ridge National Laboratory report University of California Radiation Laboratory report Nuclear Wallet Cards, NNDC-BNL, Brookhaven, ed. J.K. Tuli

C O N F E R E N C E P R O C E E D I N G S A N D A B S T R A C T S

P-Amsterdam P-Arles B -Arles P-Bernkastl

P-Birmingham P-Bombay P-Cargese P-Chicago P-Darmstadt P-Dubna P-Foros P-Friburg P-Helsingor P-Julich P-Miami P-Moscow P-Rosseau P-Seyssins P-StMalo P-StPeterbg P-Tokai P-Tokai

1996 2nd. North-West Europe Nuclear Physics Conference NWE'96 1995 Proc. Int. Conf. on Exotic Nuclei and Atomic Masses ENAM-95 1995 Abstracts ENAM-95 1992 Proc. 9th Int. Conf. Atomic Masses and Fund. Constants AMCO-9

and 6th Int. Conf. Nuclei far from Stability NUFAST-6 1985 Proc. Specialists Meeting on Delayed Neutron Properties 1985 Symposium on Quantum Electronics 1976 Proc. 3rd Int. Conf. Nuclei far from Stability NUFAST-3 CERN 76-13 1985 Proc. Meeting of the American Society for Nuclear Chemistry 1984 Proc. 7th Int. Conf. Atomic Masses and Fund. Constants AMCO-7 1989 Int. School-Seminar on Heavy-Ion Physics 1991 Proc. Intern. Conf. on Exotic Nuclei, South Crimea 1993 Proc. 8th Int.Symp. Neutron Capt. Gamma Ray Spectroscopy 1981 Proc. 4th Int. Conf. Nuclei far from Stability NUFAST-4 CERN 81-09 1992 Int. Conf. Nuclear Data for Science and Technology 1989 Symposium on Exotic Nuclear Spectroscopy 1983 Program of 33rd USSR Conference on Nuclear Spectroscopy 1987 Proc. 5th Int. Conf. Nuclei far from Stability NUFAST-5 AIP Conf.Proc.164 1994 Proc. Workshop on Nuclear Fission and Fission-Product Spectroscopy 1988 Proc. 3rd Int. Conf. Nucleus-Nucleus Collisions 1995 Low Energy Nuclear Dynamics, EPS XV Nucl. Phys. Div. 1992 Symposium on Nuclear Data, JAERI 1994 Symposium on Nuclear Data, JAERI


L I S T O F R E F E R E N C E S

ABBW Interpretation 52Fr23 PPSOA 65, 52Ka41 PHRVA 85, 52Wi26 PHRVA 85, 56Po16 ZENAA 11, 58Ri23 ZENAA 13, 61Di04 NUPHA 25, 61 Hi06 JUPSA 16, 61La05 DANKA 137, 61Ma05 PHRVA 121, 61Ru06 UCRL- 9511 65Ce02 PRLTA 15, 66Sc23 NUPHA 89, 67Es06 AAFPA 6, 67F115 AENGA 22, 68De01 NUPAB 106, 68De27 ZEPYA 216, 68Et01 PHRVA 168, 68Si01 NUPAB 109, 68To 19 J1NCA 30, 69Ch 18 PYLBB 29, 69Gh01 PRLTA 22, 69Wa15 J1NCA 31, 70Ba61 NUPAB 158, 70Bol 3 PRVCA 2, 70De08 JINCA 32, 70Es03 PYLBB 33, 70Fi.A CERN-70-29 70Hal8 NUPAB 148, 70Kr05 JINCA 32, 70Ma24 APAHA 28, 71Ho01 NUPAB 163, 71Ho07 PYLBB 34, 71To13 JINCA 33, 7 lWo02 JINCA 33, 72Ar02 NUIMA 102, 72Fi12 NUPAB 188, 72Ho18 NUPAB 187, 72Jo08 ZEPYA 251, 73A113 PRVCA 8, 73Bo13 PRVCA 7, 73Dr10 AENGA 35, 73Ka45 RAACA 19, 73Se08 PRVCA 8, 73To02 PRVCA 7, 74Ar27 IANFA 38, 74Bo05 PRVCA 9, 74Gr29 JINCA 36, 74Ke07 CJPHA 52, 74Ne10 PRVCA 10, 74Ro31 PRVCA 10, 74Ru08 NUIMA 120, 75Ga25 ANPHA 9,

G. Audi, O. Bersillon, J. Blachot, A.H. Wapstra 9 i 1 J.H. Fremlin, M.C. Walters and 95Tr07 368 M.I. Kalkstein, W.E Libby 687 R.G. Winter 143 W. Porschen, W. Riezler 904 W. Riezler, G. Kauw 248 R.M. Diamond et al.

1280 H. Hisatake 551 A.K. Lavrukhina et al.

1758 R.D. Macfarlane and T.P. Kohman C.P. Ruiz (thesis Berkeley)

300 J. Cemy et al. 401 D. Schwalm, B. Povh 261 K. Eskola 342 G.N. Flerov et al. 337 A.G. Demin et al. 103 I. Demedde

1249 R.C. Etherton et al. 231 A. Siivola

1649 L. Tomlinson and M.H. Hurdus 652 J. Chaumont et al.

1317 A. Ghiorso et al. 2679 T.E. Ward et al.

337 R.K. Bardin et al. 1841 J. Borggreen et al. 705 P. del Marmol et al. 287 J.E. Esterl et al.

M. Finger et al. 249 P.G. Hansen et al.

3713 J.-V. Kratz et al. 237 I. Mahunkaet al. 277 P. Homshcj et al. 591 P. Homshcj et al.

3609 L. Tomlinson et al. 587 K. Wolfsberg 253 R. Arlt et al. 369 M. Finger et al. 599 P. HomshCj et al. 425 H.W. Jongsma et al.

1011 D.E. Alburger et al. 1686 W.W. Bowman et al. 279 V.B. Druin et al.

1 H.M.A. Karim 258 R.G. Sextro et al.

2010 K.S. Toth et al. 1569 R. Arlt et al. 836 J.D. Bowman et al.

2409 B. Grapengiesser et al. 847 G. Kennedy et al. 320 K. Neubeck et al.

1181 E. Roeckle ta l . 333 G. Rudstam et al. 241 H. Gauvin et al.

75Ho02 PYLBB 55, 53 75Ho09 PYLBB 57, 147 75Ke08 PRVCA 12, 553 75Kr17 INUCA 11, 331 76Ah06 PRVCA 14, 211 76Ed.A P-Cargese 258 76He04 NUPAB 258, 83 76Lu02 PRVCA 13, 1544 76Ox01 ZPAAD 279, 289 76Vi02 PYLBB 60, 261 77Bo02 NUPAB 275, 229 77Bo.A Th.-Orsay 77Ca23 ZPAAD 283, 221 77De25 ZPAAD 283, 33 77Ge03 NUPAB 283, 45 77Ho25 NUPAB 288, 429 77Ij01 PRVCA 15, 2251 77Re05 PRVCA 15, 2108 77Ru04 JINCA 39, 753 77Sc03 PYLBB 66, 133 78Cal l ZPAAD 287, 71 78Cr03 ZPAAD 287, 45 78Ek05 HYIND 4, 165 78Fi02 PRVCA 17, 718 78Ga07 YAFIA 27, 894 78Ha08 PYLBB 73, 139 78Ro19 PYLBB 78B, 393 78Sc26 ZPAAD 288, 189 79Du02 NUPAB 315, 317 79En02 PRVCA 19, 1948 79Fo10 NUPAB 323, 205 79Hal0 NUPAB 318, 29 79Ho10 ZPAAD 291, 53 79Ho27 NUPAB 330, 429 79Ke02 ZPAAD 289, 407 79Ri09 ZPAAD 290, 311 79Sc09 NUPAB 318, 253 79To06 PRVCA 19, 2399 79Vi01 PRVCA 19, 177 80Al14 ZPAAD 295, 305 80Al15 ZPAAD 295, 331 80Ew03 ZPAAD 296, 223 80Ga07 YAFIA 31, 306 80Ho17 IJARA 31, 153 80Sc09 PYLBB 91, 46 81A103 PRVCA 23, 473 8lAy01 PRVCA 23, 879 81Be03 PRVCA 23, 555 81Bj01 NUPAB 359, 1 81Bo30 ZPAAD 302, 121 81De22 ZPAAD 300, 251 81De38 ZPAAD 303, 151 81Dr07 ZPAAD 302, 361 81Ew01 NUPAB 352, 13 81Ho10 ZPAAD 299, 281 81Ho.A P-Helsingor 190


E Homshcj et al. P. Homshcj et al. G.G. Kennedy et al. K.-L. Kratz et al. H. Ahrens et ai. M.D. Edmiston et al. R.G. Helmer et al. E. Lund et al. K. Oxom et al. D.J. Vieira et al. D.D. Bogdanov et al. C. Bourgeois C. Cabot et al. J. Deslauriers et al. J. Genevey-Rivier et al. P. HomshCj et al. M.A. ljaz et al. EL. Reeder et at. W. Rudolph et al. A.G. Schmidt et al. C. Cabot et al. J. Cran~on et al. C. Ekstrom et al. R.B. Firestone et al. Yu.P. Gangrskii et al. E. Hagberg et al. E. Roeckl et al. U.J. Sehrewe et al. E Dubbers et al. G. Engler et al. B. Fogelberg and E Carl6 E. Hagberg et al. S. Hofmann et al. J. Honkauen et al. U. Keyser et al. C. Ristori et al. K.-H. Schmidt et al. K.S. Toth et al. D.J. Vieim et al. G.D. Alkhazov et al. K. Aleklett et al. G.T. Ewan et al. Yu.E Gangrskii et al. H. Houtermans et al. U.J. Schrewe et al. D.E. Alburger et al. J. Ayst6 et al. C.E. Bemis,Jr. et al. T. Bjomstad et al. J. Bonn et al. S. Della Negra et al. J. Desluuders et al. S. Dfissi et al. G.T. Ewan et al. S. Hofmann et al. S. Hofmann et al.

113

114

81Hs02 PRVCA 23, 81Jo.A P-Helsingor 81Le23 PRVCA 24, 81Me17 RAACA 29, 81Mu12 ZPAAD 302, 81Ni08 RAACA 29, 81Sc17 NUPAB 368, 81Th04 PRVCA 23, 81Th06 NUPAB 367, 82A107 ZPAAD 305, 82Be20 NCIAA 33, 82Bo04 PRVCA 25, 82Ca16 PRVCA 26, 82En03 PRVCA 25, 82Ku15 ZPAAD 308, 82No06 ZPAAD 305, 82No08 ZPAAD 306, 82Ra13 ZPAAD 305, 82Sc15 PRVCA 25, 82To02 PYLBB 108, 83Ay01 NUPAB 404, 83En03 NSENA 85, 83Ga.A P-Moscow 83Ha06 NUPAB 395, 83La23 PYLBB 130, 83La27 ZPAAD 314, 83Ni05 ZPAAD 312, 83Po10 NUPAB 411, 83Re05 PRVCA 27, 83Sc24 ZPAAD 312, 83Sh06 ZPAAD 311, 83Woi0 PRLTA 51, 84Ay01 PYLBB 138, 84Ca29 PRVCA 30, 84Ca32 PRVCA 30, 84Gu19 NUPAB 426, 84La03 NUPAB 414, 84La27 PYLBB 146, 84Ni03 ZPAAD 316, 84Og03 RAACA 37, 84Sc06 ZPAAD 315, 84Sc13 ZPAAD 316, 84Sc.A GSI-84-3 84Sc.C P-Darmstadt 84So03 PRVCA 29, 84To07 PRVCA 30, 85Ah. 1 P-Bombay 85Al17 PRVCA 32, 85Ay01 PRLTA 55, 85Ay02 PRVCA 32, 85Ba57 ZPAAD 322, 85Bo46 PRLTA 55, 85Bo49 PYLBB 164, 85De08 JPHGB 11, 85Ho21 PYLBB 160, 85La03 PYLBB 150,

G. Audi et al . /Nuclear Physics A 624 (1997) 1-124

1217 H.-C. Hseuh et al. 265 B. Jonson et al.

2370 M.E. Leino et al. 93 D.H. Meikrantz et al.

7 G. Miinzenberg et al. 113 K. Nishiizumi et al. 153 D. Schardt et al.

2720 C. Thibanlt et al. 1 C. Thibault et al.

185 G.D. Alkahazov et al. 273 E. Belotti et al. 941 J.D. Bowman et al.

1778 M.D. Cable et al. 1830 H.A. Enge et al.

21 W. Kurcewicz et al. 289 E. Nolte and H. Hick 223 E. Nolte et al. 359 M.S. Rapaport et al.

3091 U.J. Schrewe et al. 169 E Touchard et al.

1 J. ,~yst8 et al. 139 T.R. England et al. 90 N. Ganbaatar et al.

152 E. Hagberg et al. 251 M. Langevin et al.

9 P.O. Larsson et al. 265 J.M. Nitschke et al.

65 M.G. Porquet et al. 3002 EL. Reeder et al.

21 J.R.H. Schneider et al. 71 K. Shizuma et al.

873 EK. Wohn et al. 369 J. ,~yst6 et al.

1276 M.D. Cable et al. 1671 E Calaprice et al.

37 D. Guillemand-Mueller et al. 151 M. Langevin et al. 176 M. Langevin et al. 249 J.M. Nitschke et al. 113 Yu. Ts. Oganessian 49 U.J. Schrewe et al. 19 K.-H. Schmidt et al.

J. Schneider Thesis 229 D. Schardt et al.

1556 P.C. Sood 712 K.S. Toth et al.

S.A. Ahmad et al. and 89Ot.1 1358 D.E. Alburger, J.B. Cumming 1384 J. Ayst6 et al. 1700 J. ,~yst6 et al. 457 A. Baas-May et al.

2269 J.A. Bounds et al. 22 U. Bosch et al.

L59 K. Deneffe et al. 375 E. Hourani et al.

71 M. Langevin et al. (see also 93Po.A)

85No03 PRVCA 31, 1937 85Pf.A P-Birmingham 75 85Re01 PRVCA 31, 1029 85Re.A P-Chicago 171 85Ti02 NUPAB 437, 342 85Wi07 ZPAAD 321, 179 86Ba26 PRVCA 34, 362 86Be35 NUPAB 460, 352 86Bo41 NUPAB 460, 373 86Cu01 PRLTA 56, 34 86Du07 ZPAAD 324, 487 86Gol0 ZPAAD 324, 117 86Hu01 PRLTA 56, 313 86Hu05 PRVCA 34, 1394 86La17 NUPAB 455, 149 86Lo.A AIEAD-261 86Ma42 PRVCA 34, 1117 86Po13 EULEE 2, 505 86Ru05 ZPAAD 324, 119 86To12 PYLBB 178, 150 86U102 ZPAAD 325, 247 86Wa17 RAEFB 94, 27 86Wi15 ZPAAD 325, 485 87AI.A LNPI-1309 87Bo29 HYIND 34, 25 87Bo36 NUPAB 473, 331 87Bo44 PRVCA 36, 2560 87Bu01 NUPAB 462, 305 87Eb02 NUPAB 464, 9 87Fa.A P-Rosseau 675 87Gi02 ZPAAD 326, 107 87Gr.A P-Rosseau 782 87Ha.A AnRpt Tohoku 43 87He10 EULEE 3, 895 87Ki.A P-Rosseau 517 87Li09 PYLBB 191, 245 87Lo.A AnRpt LLNL 135 87Mo29 ZPAAD 328, 417 87Mu15 ZPAAD 328, 49 87Ne.A P-Rosseau 126 87Po04 ZPAAD 327, 17 87Ra06 PRVCA 36, 303 87Ra12 NIMAE 26, 72 87Se07 NUPAB 467, 93 87To02 PRVCA 35, 310 87To05 PRVCA 35, 620 87Vi01 NUPAB 463, 605 88Ah02 NUPAB 483, 244 88Aj01 NUPAB 490, 1 88Ba42 ZPAAD 330, 341 88Be.A P-StMalo A1 88Bo06 NUPAB 477, 89 88Bo39 NUPAB 490, 287 88Du09 PYLBB 206, 195 88Ka20 PRVCA 38, 1857 88Kr10 ZPAAD 330, 229


E.B. Norman B. Pfeiffer et al. and 93Ru01 EL. Reeder et al. P.L. Reeder et at. and 93Ru01 P. Tidemand-Petersson et ai. P.A. Wilmarth et al. S.W. Barwick et al. A.V. Belozyorov et al. M.J.G. Borge et al. M.S. Curtin et al. J.P. Dufour et al. H. G6ktiirk et al. E.K. Hulet et al. E.K. Hulet et al. M. Langevin et al. (see also 93Po.A) A. Lorenz H. Mach et al. E Pougheon et al. (see also 93Po.A) E. Runte et al. K.S. Toth et al. G. Ulm et al. R.A. Warner and P.L. Reeder EA. Wilmarth et al. G.D. Alkhazov et al. and 89Ot.1 W. Borchers et al. and 89Ot.1 V. Borrel et al. J.A. Bounds et al. E Buchinger et al. J. Eberz et al. T. Faestermann et al. A. Gillitzer et al. R.C. Greenwood et al. H. Hama et al. E Hel3berger et al. P. Kilcher et al. C.E Liang et al. R.W. Lougheed et al. K.J. Moody et al. G. Miinzenberg et al. R. Neugart et al. F. Pougheon et al. M.S. Rapaport et al. and PrvCom GAu July 1988 H.L. Ravn et al. T. Sekine et al. K.S. Toth et al. K.S. Toth et al. K. Vierinen S.A. Ahmad et al. E Ajzenberg-Selove D. Barn6oud et al. R. BErand et al. U. Bosch et al. M.J.G. Borge et al. J.P. Dufour et al. O. Kawakami et al. K.-L. Kratz et al.

115

116

88Me.A 88Ni02 88Pe13 88Vi02 88Wi05 89Ar.A 89Ba22 89Ba.B 89Bol 1 89Bu09 89C102 89Gu03 89Hal0 89Ha27 89Ha. 1 89Ha.2 89He 13 89Ho 12 89Hu09 89Hu.A 89Ko02 89Ko07 89Kr12 89Le16 89Li04 89Mi.A 89Ni04 89Ot. 1 89Po10 89Pr. 1 89Re.A 89St06 89Tal 1 89To01 89Vi04 89Wa10 89Zh04 90AI 11 90An 19 90An22 90Au.A 90Ba02 90Ba.A 90Be 13 90Bo 16 90Bo39 90Bu28 90Ch37 90De43 90Ed01 90En08 90Gu02 90Ha02 90He.A 90Ho03 90Ka.A


Th.°Mainz R. Menges et al. and 89Ot.1 PRVCA 37, 2694 J.M. Nitschke et al. PRVCA 38, 931 H. Penttil~i et al. PRVCA 38, 1509 K.S. Vierinen et al. ZPAAD 329, 503 P.A. Wilmarth et al. P-Dubna A.G. Artukh et al. PYLBB 223, 273 A.S. Barabash et al. AnRpt CRN E Banmann et al. ZPAAD 333, 109 M.J.G. Borge et al. ZPAAD 333, 131 D.G. Burke et al. NUPAB 493, 293 E.T.H. Clifford et al. ZPAAD 332, 189 D. Guillemaud-MueUer et al. (see also 93Po.A) PRVCA 39, 1866 H.L Hall et al. NUPAB 500, 90 Y. Hatsukawaet al. PENUC Ill, 99 J.C. Hardy, E. Hagberg PENUC lII, 157 EG. Hansen, B. Jonson ZPAAD 333, I l I EP. HeBberger et al. ZPAAD 333, 107 S. Hofmann et al. PRVCA 40, 770 E.K. Hulet et al. P-Dubna E.K. Hulet (Livermore) PRVCA 39, 636 M.O. Kortelahti et al. ZPAAD 332, 229 M.O. Kortelahti et al. NUPAB 503, 113 A. Krasznahorkay et al. NUPAB 496, 477 M. Lewitowicz et al. JPHGB 15, L31 C.E Liang et al. P-Dubna 66 V.L Mikheev et al. ZPAAD 334, l l l J.M. Nistchke et al. THISc 8, 517 E.W. Otten NUPAB 500, 287 E Pougheon et al. PENUC II, 205 EB. Price, S.W. Barwick P-Miami EL. Reeder et al. PRVCA 39, 1963 C.A. Stone et al. ZPAAD 333, 29 J.L. Tain et al. PRVCA 39, 1150 K.S. Tothet al. NUPAB 499, l K.S. Vierinen et al. PRVCA 39, 1647 S. Wang et al. PRVCA 39, 1985 Z. Zhao et al. PRVCA 41, 2320 D.E. Alburger and G. Harbottle ZPAAD 337, 229 A.N. Andreyev et al. ZPAAD 337, 231 A.N. Andreyev et al. PrvCom GAu Feb G. Audi (Speg) PRVCA 41, 246 P.H. Barker et al. ITEP-131-90 A.S. Barabash et al. and 95Tr07 ZPAAD 336, 41 M. Bernas et al. PYLBB 241, 179 R. Bonetti et al. YAFIA 52, 358 D.D. Bogdanov et al. YAFIA 52, 305 E. Bukhner et al. PRVCA 42, 1796 R.M. Chasteler et al. NUPAB 519, 529 C. D6traz et al. HYIND 59, 83 R. Eder et al. NUPAB 521, l EM. Endt PRVCA 41, 937 D. Guillemaud-Muelleret al. (see also 93Po.A) PRVCA 41, 618 H.L. Hall et al. AnRpt LBL 65 R.A. Henderson et al. PRVCA 41, 631 D.C. Hoffman et al. AnRpt LBL 68 B. Kadkhodayan et al.


90Ko25 PRVCA 42, 1267 M.O. Kortelahti et al. 90Le03 ZPAAD 335, 117 M. Lewitowicz et al. 90Me12 ZPAAD 337, 45 E Meissner et al. 90Me13 ZPAAD 337, 109 K.A. Mezilev et al. 90Mi23 PRLTA 25, 3092 H.S. Miley et al. 90Mu06 NUPAB 513, 1 A.C. Mueller et al. 90Ne.A PrvCom A.Gizon R. Neugart 90Og01 PYLBB 235, 35 A.A. Ogloblin et al. 90Ri01 PYLBB 235, 30 K. Riisager et al. 90Ru02 JPHGB 16, 255 E. Ruchowskaeta l . 90Sh.A AnRpt LBL 114 A.A. Shihab-Eldin et al. 90Ta07 ZPAAD 335, 477 I. Tago et al. 90Tu.A Wallet Cards J.K. Tuli 90Va18 MPLAE 5, 1299 A.A. Vasenko et al. 90We01 PRVCA 41, 778 D. Weselka et al. 90Wi12 PRVCA 42, 954 J.A. Winger et al. 91Aj01 NUPAB 523, 1 F. Ajzenberg-Selove 91Anl0 ZPAAD 338, 363 A.N. Andreyev et al. 91Ay.A P-Foros J. ,~ystO et al. 91Be25 NUPAB 533, 113 A. Ben Brahamet al. 91Be33 PRLTA 67, 3661 M. Bemas et al. 91Bo20 PRVCA 44, 888 R. Bonetti et al. 91Bo22 ZPAAD 339, 311 A. Bouldjedriet al. 91Bo32 NUPAB 531, 353 V. Borrel et al. 91Ej02 PYLBB 258, 17 H. Ejiri et al. 91E104 JPHGB 17, S145 S.R. Elliott et al. 91Fi03 PRVCA 43, 1066 R.B. Firestone et al. 91Go19 NUPAB 531, 613 M.G. Gornov et al. 91Gr12 NUPAB 530, 401 J.C. Griffin et al. 91He04 ZPAAD 338, 7 K. Heiguchi et al. 91Hi02 PRVCA 43, 2591 J.C. Hill et al. 91Hi.A AnRpt LBL 69 M.M. Hindi et al. 91Ho16 NUPAB 530, 111 M.C.A. Hotchkis et al. 91Ju05 ZPAAD 340, 125 A. Jungclaus et al. 91KeZZ PrvCom NDG J. Kern et al. 91K102 PRVCA 44, 2801 N. Klay et al. 91Kr15 ZPAAD 340, 419 K.-L. Kratz et al. 91Kr.A AnRpt LBL 57 S.A. Kreek et al. 91Le15 ZPAAD 340, 107 M. Lewandowski et al. 91Mc.A ORNL-6660 p.63 J.H. McNeill et al. 91Mo10 PRLTA 66, 1571 M.E Mohare t al. 91Or01 PYLBB 258, 29 N.A. Orre t al. 91Pr02 PRVCA 43, 1781 P.B. Price et al. 91Se01 ZPAAD 338, 245 P.J. Sellin et al. 91To08 PRVCA 44, 1868 K.S. Toth et al. 91To09 ZPAAD 340, 343 K.S. Toth et al. 91Tu02 PRLTA 67, 3211 A.L. Turkevichetal . 91Va04 NUPAB 529, 268 P. Van Duppen et al. 91Zh24 PYLBB 260, 285 X.G. Zhoue t al. 91Zh29 YTHLD 13, 193 S. Zhou et al. 92Ay02 PRLTA 69, 1167 J. Aysto et al. 92Ba01 PRVCA 45, 69 D. Bazin et al. 92Ba.A AnRpt LBL 72 J.C. Batchelder et al. 92Be30 PRLTA 69, 2341 T. Bematowicz et al. 92Be.A IPNO-DRE-25 M. Bemas et al. 92Bo05 NUPAB 539, 249 M.J.G. Borge et al.

117

118

92Bo37 ZPAAD 344, 135 92Bo.A P-Bemkastl 213 92Bo.D P-Bemkastl 743 92Go10 PRVCA 46, R883 92Gr02 PRVCA 45, 1058 92Gr09 ZPAAD 341, 247 92Hal0 PRVCA 45, 1609 92Ha.C AnRpt Tsukuba 92Hu04 PRVCA 46, 1209 921d01 ZPAAD 341, 427 92Kr01 PRVCA 45, 1064 92Kr.A AnRpt LBL 58 92Kr.C AnRpt LBL 61 92Lil 1 PRVCA 46, 797 92Lo.B UCRL-JC- 109951 92Me10 ZPAAD 343, 283 92Mo03 PRVCA 45, 1392 92Mo15 ZPAAD 342, 273 92Mo25 PRVCA 46, 2624 92Pa05 PRLTA 68, 1287 92Po14 BRSPE 56, 666 92Pr05 PRVCA 46, 1939 92Ro21 HYIND 75, 457 92Sc03 NUPAB 539, 112 92Sc16 NUPAB 545, 646 92Sc.A P-Bernkastl 627 92Sc.B P-Julich 562 92Sh12 ZPAAD 342, 369 92Ta.A P-Tokai 267 92Te03 ZPAAD 342, 303 92Th02 NUPAB 536, 418 92Th06 NUPAB 548, 71 92Ti02 NUPAB 54 I, 1 92To02 PRVCA 45, 856 92Wa14 ZPAAD 342, 277 92We04 ZPAAD 343, 67 92Wo03 ARISE 43, 551 92Xu04 PRVCA 46, 510 92Ye04 PRVCA 46, 2620 93A103 ZPAAD 344, 425 93An07 ZPAAD 345, 247 93Ba61 PRVCA 48, 2593 93Be46 ZPAAD 346, 325 93BI.A AnRpt GSI 53 93Bo20 NUPAB 556, 115 93Bo26 NUPAB 562, 32 93Br22 NUPBB 31, 76 93Ch10 PRVCA 47, 1462 93Ga09 PRVCA 47, 2910 93Gr.C AnRpt LBL 76 93Ho.A AnRpt GSI 64 93Ja03 NUPAB 552, 340 93Ka12 PRVCA 47, 2452 93K102 PRVCA 47, 2502 93Kr05 ASJOA 403, 216 93Li18 PYLBB 312, 46


V. Borrel et al. W. Borchers et al. V.A. Bolshakov et al. J. G6rres et al. K.E. Gregorich et al. H. Grawe et al. E. Hagberg et al. T. Hayakawa et al. M. Huyse et al. N. Idrissi et al. J.V. Kratz et al. S.A. Kreek et al. S.A. Kreek et al. P. Lievens et al. R.W. Lougheed et al. F. Meissner et al. K.J. Moody et al. D.M. Moltz et al. K.J. Moody et al. R.D. Page et al. A.V. Potempa et al. P.B. Price et al. I. Romanski et al. W. Schmitz et al. W.-D. Schmidt-Ott et al. W.-D. Schmidt-Ott et al. U. Schotzig et al. S. Shi et al. A. Tanaka et al. O. Tengblad et al. K. Theine et al. K. Theine et al. D.R. Tilley et al. K.S. Toth et al. J. Wauters et al. M. Weber et al. D.H. Woods et al. S.-W. Xu et al. S.J. Yennello et al. G.D. Alkhazov et al. A.N. Andreyev et al. J.C. Batchelder et al. P. Bednarczyk et al. B. Blank et al. R. Bonetti et al. R. Bonetti et al. R.L. Brodzinski et al. Y. Chen et al. A. Garcfa et al. K.E. Gregorich et al. S. Hofmann et al. Z. Janas et al. A. Kawashima et al. G. Klotz et al. K.-L. Kratz et al. and PrvCom B. Pfeiffer to GAu August 1996 K. Livingston et al.

93Li34 93Li40 93Me13 93Mo 18 93Pel 1 93Po.A 93Ro06 93Ro.B 93Ru01 93Ru03 93Se04 93Se09 93Se.A 93So06 93To02 93To04 93"1"o05 93Va19 93Vu02 93Wa03 93Wa04 93Wi03 93Yu03 94An02 94Ar23 94Ar29 94Ba 15 94Ba50 94Ba54 94Be24 94Bl10 94Bo28 94Br 15 94Bu 18 94Cz02 94Dal 1 9413008 94Fa06 94Gr08 94He08 94He28 941b01 94It.A 94Ka39 94Ke.B 94Ki.A 94Ko.A 94Kr13 94Ku25 94La22 94Le05 94Lh02 94Li 12 94Lo04 94Ma50 94Mo.A

G.

PRVCA 48, 2151 PRVCA 48, 3113 PRVCA 48, 2089 NUPAB 563, 21 NUPAB 561, 416 PrvCom GAu Dec PRVCA 47, 1455 P-Friburg 231 ADNDA 53, 1 PRVCA 47, 2574 PRVCA 47, 1933 ZPAAD 346, 323 PrvCom GAu Feb PRVCA 47, 2941 PRVCA 47, 1804 PRVCA 48, 436 PRVCA 48, 445 P7_ETA 57, 631 PRVDA 48, 1009 ZPAAD 345, 21 PRVCA 47, 1447 PYLBB 299, 214 ZPAAD 346, 187 ZPAAD 347, 225 NIMAE 339, 168 EULEE 27, 29 PYLBB 322, 176 PRVCA 50, 1180 PRVCA 50, 1807 PYLBB 331, 19 PRVCA 50, 2398 NUPAB 576, 21 PRVCA 50, 480 ZPAAD 349, 3 ZPAAD 348, 267 PYLBB 328, 16 PRVCA 49, 1867 PRVCA 49, 2440 PRLTA 72, 1423 PRVCA 49, 1845 PRVCA 50, 2219 ZPAAD 350, 9 P-Tokai 185 ZPAAD 350, 183 AnRpt LBL 85 AnRpt CSNSM AnRpt AECL 3-1 PRVCA 50, 2288 NUPAB 577, 405c PRLTA 73, 624 ZPAAD 348, 151 ZPAAD 350, 97 PRVCA 49, 2230 NIMAE 339, 164 NIMAE 339, 158 PrvCom GAu Oct

Audi et al./Nuclear Physics A 624 (1997) 1-124

K. Livingston et al. K. Livingston et al. E Meissner et al. K.J. Moody et al. H. Penttil~i et al. E Pougheon J.D. Robertson et al. B. Roussi~re et al. G. Rudstam et al. D. Rudolph et al. EJ. Sellin et al. EJ. Sellin et al. H.L. Seifert et al. O. Sorlin et al. K.S. Toth et al. K.S. Toth et al. K.S. Toth et al. S.I. Vasilev et al. J.-C. Vuilleumier et al. J. Wauters et al. J. Wauters et al. J.A. Winger et al. S. Yuan et al. A.N. Andreyev et al. G. Ardisson et al. C. Arpesella et al. A. Balysh et al. P. Baumann et al. J.C. Batchelder et al. M. Bernas et al. B. Blank et al. R. Bonetti et al. A.M. Bruce et al. D. Bucurescu et al. S. Czajkowski et al. M. Dasgupta et al. M. Dombsky et al. L. Faux et al. K.E. Gregorieh et al. R.G. Helmer, C.W. Reich M. Hencheck et al. E Ibrahim et al. S. Itoh et al. H. Kaur et al. D.A. Keeney et al. J.B. Kim et al. V.T. Koslowsky et al. S.A. Kreek et al. K. Kume et al. Yu.A. Lazarev et al. M. Leino et al. G. Lhersonneau et al. C.E Liang et al. J.M. Los Arcos et al. R.H. Martin et al. D.M. Moltz

119

120

94Os04 PYLBB 338, 13 94Pal 1 PRVCA 49, 3312 94Pa12 PRLTA 72, 1798 94Pa37 NUPAB 580, 173 94Ru.l PSSAA 42, 227 94Sa31 PRVCA 50, 1170 94Sc22 ZPAAD 348, 241 94Sc35 ZPAAD 350, 99 94Sc39 NIMAE 339, 174 94Se01 PYLBB 321, 323 94Sh07 ZPAAD 348, 25 94Si.A INDC-039/LN 94St31 ZPAAD 347, 287 94Ti03 PRVCA 49, 2871 94Ts.A AnRpt JAERI 16 94Wa23 PRVCA 50, 2768 94Wa.A P-Seyssins 94We02 ZPAAD 347, 185 94Xu09 ZPAAD 350, 187 94Ye08 NIMAE 350, 608 94Yo01 PRVCA 49, 279 94Zh02 PRVCA 49, R592 94Zh26 ZPAAD 350, 7 95A1.A P-Arles 329 95Am.A P-Aries 537 95Ap.A PrvCom GAu May 95Ar08 PYLBB 345, 564 95Au04 NUPAB 595, 409 95Ba28 PRLTA 74, 3569 95Ba75 PRVCA 52, 1807 95Ba.A P-Arles 53 95Bi01 PRVCA 51, 125 95Bi17 PRLTA 75, 4571 95Bi.A P-Aries 545 95B106 PRLTA 74, 4611 95B123 PYLBB 364, 8 95Bo18 PRVCA 51, 2530 95Bo.B P-StPeterbg 95Br24 NUPAB 595, 481 95Bull NUPAB 587, 475 95Bu18 YAFIA 58, 195 95Ca.A AnRpt JYFL 33 95Ce01 NUPAB 581, 189 95Cz.A P-Aries 553 95Da09 PYLBB 344, 72 95Da37 PRVDA 51, 2090 95Da.3 YAFIA to be pd 95En07 ZPAAD 352, 351t 95En.A AnRpt JYFL 44 95Fa.A AnRpt GSI 21 95Fe12 ZPAAD 353, 9 95Ga.A P-Aries 595 95Gh04 NUPAB 583, 861c 95Gu01 NUPAB 583, 867c 95Gu10 PRVCA 52, 740 95Ha16 ZPAAD 352, 241


A.N. Ostrowski et al. R.D. Page et al. R.D. Page et al. G. Passler et al. W. RiJhm et al. C. Sfienz et al. R. Schneider et al. K. Schmidt et al. E. Sch6nfeld et al. D. Seweryniak et al. T. Shizuma et al. H. Siegert M.-L. Stolzenwald et al. R.J. Tighe et al. K. Tsukada et al. J. Wauters et al. W.B. Waiters, C.A. Stone C. Wennemann et al. Xu Shuwei et al. A.V. Yeremin et al. B.M. Young et al. L. Zhang et al. Zhou Shuhua et al. D.V. Aleksandrov et al. E Ameil et al. and GSI-Nachrichten 11-95 A. Aprahamian et al. V. Artemiev et al. G. Audi, A.H. Wapstra D. Bazin et al. J.C. Batchelder et al. H. Backe et al. C.R. Bingham et al. N. Bijnens et al. C.R. Bingham et al. and PrvCom GAu June 1995 B. Blank et al. B. Blank et al. R. Bonetti et al. H.G. Bohlen et al. J.B. Breitenbach et al. D. Bucurescu et al. S.E Burachas et al. and 95Tr07 P. Campbell et al. J. Cederktill et al. S. Czajkowski et al. and post cut-off date 97Be12 F.A. Danevich et al. D. Dassi6 et al. F.A. Danevich et al. and 95Tr07 Ch. Engelmann et al. T. Enqvist et al. T. Faestermann et al. V.N. Fedoseyev et al. A. Gadea et al. A. Ghiorso et al. A. Guglielmetti et al. A. Guglielmetti et al. T. Hayakawa et al.


95Hi02 PRVCA 51, 1736 T. Hild et al. 95Hi12 PRVCA 52, 2236 T. Hild et al. 95Ho03 ZPAAD 350, 277 S. Hofmann et al. 95Ho04 ZPAAD 350, 281 S. Hofmann et al. 95Ho.A GSI-Nachr. Feb S. Hofmann et al. 95Ho.B PrvCom GAu Mar S. Hofmann et al. and GSI Annual report 1995 95Ja16 PHSTB T56, 262 Z. Janas et al. 95Ja.A P-Aries 573 Z. Janas et al. 95Jo02 NUPAB 584, 489 A. Jokinen et al. 95Jo.A P-Aries 499 A. Jokinen et al. 95Ka17 ZPAAD 352, 11 H. Kaur et al. 95Ka.A B-Aries PD22 V.G. Kalinnikov et al. 95Ke04 NUPAB 586, 219 M. Keim et al. 95Kr03 PRLTA 74, 860 R.A. Kryger et al. 95Kr04 ZPAAD 351, 11 K. Krumbholz et al. 95Kr.A ISOLDE-News 01 K.-L. Kratz 95La09 NUPAB 588, 501 Yu.A. Lazarev et al. 95La10 NUPAB 589, 129 G.J. Lane et al. 95La20 PRLTA 75, 1903 Yu.A. Lazarev et al. 95Le04 PRVCA 51, 1047 M.J. Leddy et al. 95Le14 NUPAB 588, 197c M. Lewitowicz et al. 95Le.A P-Aries 505 M. Leino et al. and PrvCom GAa June 1995 95Le.B P-Aries 427 M. Lewitowicz 95Lh04 ZPAAD 352, 293 G. Lhersonnean et al. 95Me03 PRVCA 51, 1558 E Meissner et al. 95Mo14 ZPAAD 352, 7 K. Morita et al. 95Mo26 NUPAB 588, 203 D.J. Morrissey et al. 95Ni05 ZPAAD 351, 125 V. Ninov et al. 95Ni.A P-Aries 571 V. Ninov et al. and Abstracts PD19

95No.A P-Aries 363 T. Nomura 95Ok02 ZPAAD 351, 243 K. Okano et al. 95Os03 NUPAB 588, 185 A. Osa et al. 95Oz02 NUPAB 592, 244 A. Ozawa et al. 95Pa01 PRVCA 51, 78 E.S. Paulet al. 95Pe12 NUPAB 588, 259c Yu.E. Penionzhkevich 95Pf01 NUPAB 581, 205 M. Pfiitzner et al. 95Pf04 ZPAAD 353, 1 B. Pfeiffer et al. 95Pi03 NUPAB 584, 509 A. Piechaczek et al. 95Po01 PRVCA 51, 519 K.R. Pohlet al. 95Re.A P-Aries 587 P.L. Reeder et al. and PrvCom GAu June 1995 95Re.B P-Aries 757 I. Reusen et al. 95Ro06 JPHGB 21, L1 H.A. Roth et al. 95Ro09 ZPAAD 351, 127 B. Roussi~re et al. 95Sa42 NUPAB 592, 221 J. Sauvage et al. 95Sc03 NUPAB 582, 109 K. Scheller et al. 95Sc28 NUPAB 588, 191c R. Schneider et al. 95Sc33 PHSTB 56, 67 R. Schneider et al. 95Sc.A AnRpt GSI 20 K. Schmidt et al. 95So03 NUPAB 583, 763c O. Sorlin et al. 95So.A P-Aries 603 O. Sorlin et al. 95Sz01 NUPAB 584, 221 J. Szerypo et al. 95Ti08 PRVCA 52, 2298 R.J. Tighe et al. 95Tr02 PYLBB 348, 331 W. Trinder et al. 95Tr03 PYLBB 349, 267 W. Trinder et al. 95Tr07 ADNDA 61, 43 V.I. Tretyak, Yu.G. Zdesenko 95Uu01 PRVCA 52, 113 J. Uusitalo et al.

121

122

95Wa.A 95Yu01 96Ak.A 96A130 96An21 96Ar. 1 96Ax01 96Ba35 96Ba37 96Ba46 96Ba80 96Bi07 96Bi17 96B111 96B121 96By03 96Ca02 96Da06 96Dal 1 96Da25 96Da.A 96Do23 96Dr07 96Dr.A 96En01 96En02 96Fa01 96Fa09 96Ga 17 96Ga24 96Ga30 96Ge07 96Ge 12 96Ge.A 96Gi08 96Gu I 1 96Gu. 1 96Ha45 96He25 96Ho 13 96Ho 16 96Hu.A 96Ik01 96Jal 0 96Jo06 96Ko13 96Kr05 96Lal 1 96La12 96Le09 96Lh04 96Lh.B 96Li05 96Me09 96Mn 19 96Ni09


P-Aries 725 G. Walter ZPAAD 352, 235 S. Yuanet al. PrvCom GAu Nov Y.A. Akovali PRLTA 77, 3319 A. Alessandrello et al. BRSPE 60, 119 A.N. Andreev et al. ZPAAD sbmt R. Arnold et al. PRVCA 54, 1511 L. Axelsson et al. PRVCA 54, 949 J.C. Batchelder et al. JPHGB 22, 487 A.S. Barabash et al. NUPAB 604, 115 A.S. Barabash et al. PRLTA 77, 5186 A. Balysh et al. PRVCA 54, R20 C.R. Bingham et al. ZPAAD 356, 3 N. Bijnens et al. PRVCA 54, 572 B. Blank et al. PRLTA 77, 2893 B. Blank et al. EULEE 33, 187 J. Byrne et al. NUPAB 598, 61 P. Campbell et al. PRLTA 76, 592 C.N. Davids et al. YAFIA 59, 5 EA. Danevich et al. ZPAAD 355, 433 EA. Danevich et al. PrvCom GAu Oct C.N. Davids PRVCA 54, 2894 T. D6rfler et al. NUPAB 601, 234 S. Drissi et al. PrvCom JB1 Sep S. Drissi ZPAAD 354, 1 T. Enqvist et al. ZPAAD 354, 9 T. Enqvist et al. PRVCA 53, 647 M. Fauerbach et al. NUPAB 602, 167 L. Faux et al. PRVCA 54, 1057 A. Galindo-Uribarri et al. ZPAAD 355, 253 A. Gadea et al. NUPAB 611, 68 P.E. Garrett et al. ZPAAD 356, 7 J. Genevey et al. NUPAB 611, 247 J. Geneveyet al. GSI-96-64 H. Geissel et al. (invited talk at EMIS-13) NUPAB 605, 301 A. Gizon et al. ZPAAD 355, 111 J. Guoeta l . PRVDA 55, 54 M. Giinther et al. NIMBE 114 , 131 P. Haas et al. ZPAAD 356, 229 M. Hellstr6m et al. ZPAAD 354, 229 S. Hofmannet al. PRLTA 77, 1020 P. Hoff et al. AnRpt GSI 30 Z. Hu et al. PRVCA 54, 2043 H. Ikezoe et al. PRVCA 54, 423 M. Jaeger et al. PRVCA 53, 3150 I.P. Johnstone and L.D. Skouras PRVCA 54, R459 EG. Kondev et al. PRVCA 53, 1971 R.A. Krygeret al. PRVCA 53, 2893 M.R. Lane et al. PRVCA 54, 620 Yu.A. Lazarev et al. ZPAAD 355, 157 M. Leino et al. PRVCA 54, 1592 G. Lhersonneau et al. AnRpt JYFL 27 G. Lhersonneau et al. ZPAAD 354, 153 C.F. Liang et al. PRLTA 77, 458 T. Mehren et al. PYLBB 367, 65 I. Mukha et al. ZPAAD 356, 11 V. Ninov et al.

96No.A AnRpt LBL 136 96Od01 ZPAAD 354, 231 96Og01 PRVCA 54, 1098 96Pa01 PRVCA 53, 660 96Pa.A PrvCom AHW Aug 96Pe25 PRVCA 54, 2760 96Pf01 PRVCA 53, 1753 96Po.A PrvCom GAu Dec 96Ri12 PRVCA 54, 2041 96Ry.B AnRpt JYFL 33 96Sa34 PRVCA 54, 2802 96Se01 PRVCA 53, 96 96Sh.A AnRpt LBL 74 96So.A PrvCom GAu May 96Ta04 PRVCA 53, 1557 96Ta18 PRVCA 54, 2926 96Ti. 1 NUPAB to be pd 96To01 PRVCA 53, 2513 96To05 ZPAAD 355, 345 96To08 ZPAAD 355, 225 96Ur02 PRVCA 54, 945 96Uu.1 ZPAAD to be pd 96Uu.A P-Amsterdam P47 96Uu.B AnRpt JYFL 42 96Wi.A AnRpt LBL 69 96Wo06 NIMAE 369, 534 96Wo.A P-Amsterdam D14 96Xu04 ZPAAD 356, 35 96Xu07 ZPAAD 356, 227 96Zh03 ZPAAD 353, 353 97A102 PRVCA 55, 474 97An.1 ZPAAD 358, 63 97Ba21 ZPAAD 357, 121 97Ba25 PRVCA 55, 2142 97Ba35 ZPAAD 357, 351 97Be12 NUPAB 616, 352c 97B103 NUPAB 615, 52 97B104 ZPAAD 357, 247 97Bu03 NUPAB 612, 91 97Cz02 NUPAB 616, 278c 97Da07 PRVCA 55, 2255 97Da.A PrvCom GAu May 97Gi.2 ZPAAD to be pd 97Ha04 NUPAB 613, 183 97Ha30 ZPAAD 358, 15 97Hu07 PRVCA 56, 1152 97Ir01 PRVCA 55, 1621 971r.1 PRLTA 79, 990 971s.A Th.-Munich Feb 97Ka07 ZPAAD 356, 363 97La13 PRVCA 55, 2127 97Le.A PrvCom GAu May 97Lil9 PRVCA 56, 1157 97Li. 1 ZPAAD to be pd 97Lo.A PrvCom GAu May 97Mi03 PRVCA 55, 1555


E.B. Norman et al. and post cut-off date 97No. 1 A. Odahara et al. T.J. Ognibene et al. R.D. Page et al. and 96Pa.A R.D. Page H. Penttil~i et al. R. Pfaff et al. F. Pougheon J.D. Richards et al. K. Rykaczewski H. Sakurai et al. D.R. Semon et al. D.A. Shaughnessy et al. O. Sorlin N. Takaoka et al. R.B.E. Taylor et al. D.R. Tilley et al. K.S. Toth et al. Y. Toh et al. K.S. Toth et al. W. Urban et al. J. Uusitalo et al. J. Uusitalo et al. and 97Le. A J. Uusitalo et al. P.A. Wilk et al. M.J. Woods et al. A. W6hr et al. Xu Shuwei et al. Xu Shuwei et al. X. Zhang et al. M. Alston-Garnjost et al. A.N. Andreyev et al. J.C. Batchelder et al. J.C. Batchelder et al. A.S. Barabash et al. M. Bemas et al. B. Blank et al. B. Blank et al. D.G. Burke et al. S. Czajkowski et al. C.N. Davids et al. C.N. Davids A. Gizon et al. E. Hagberg et al. T. Hayakawa et al. W.X. Huang et al. R.J. Irvine et al. G.M. Irwin and K.H. Kim S. Issmer D. Kast et al. G.J. Lane et al. M. Leino Z. Li et al. W. Liu et al. R.W. Lougheed S. Mitsuoka et al.

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97Mu08 PRVCA 55, 2267 97No.1 NUPAB 621, 92c 97Oi01 PRVCA 56, 745 97Po.A PrvCom GAu May 97Po.B PrvCom GAu Jul 97Pu01 ZPAAD 357, 3 97Sa14 NUPAB 616, 311c 97Sc. 1 ZPAAD to be pd 97Sh13 PRVCA 55, 1715 97So07 PRVCA 55, 2142 97Su06 NUPAB 616, 341c 97Ta10 PRVCA 56, 142 97Wa04 ZPAAD 357, 39 97Wa05 PRVCA 55, 1192 97Xu01 PRVCA 55, R553 97Ya03 ZPAAD 357, 353 97Za03 PRVCA 55, 2697


U. Miiller et al. E.B. Norman et al. M. Oinonen et al. E Pougheon G.L. Poli Y.H. Pu et al. H. Sakurai et al. K. Schmidt et al. M. Shibata et al. G.A. Souliotis et al. K. Stimmerer et al. S.L. Tabor et al. J. Wawryszczuk et al. J. Wauters et al. X.J. Xu et al. W.E Yang et al. K. Zaerpoor et al.

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