55
UCRL-JC-126741 PREPRINT Nuclear Modeling Applied to Radioisotope Productim Ma’Cil 19,1997
UCRL-JC-126741
PREPRINT
Nuclear Modeling Applied to Radioisotope Productim
Ma’Cil 19,1997
.
DISCLAIMER
This documentwas prepared= an accountof work spaasoredby ao agaIcy of theUnitedStatesCovemment. NeithertbaUnitedSmt= Govermtentnor theUaiverntyof Caiifotnianoraty of theirasnpkyee%makesanyW8m=tty, esprcssor impli~ or-umes ayl+Wtyor~Uyf*-~, *dexordti=of any Monnatio* apparatq prod* orproeaesdiael~orrep-eats thatits usewoutdnotinf~eprivately ownedsights.Rd~ bereiotoaoyapecifkeommercialDroducts.~ orservieebYtradeISSMGtrademark ~, W *e-k
by the UnitedSt&s Gwesnment ‘ti tba Universityof CaIifoti* ‘Ibe views andopinions of authomeqmssed herein do not ~y state or retlect those of theUnitedStatesGovernmentor theUniversityof Cdiforni+ and shall not & used foradvetiisingor productendorsementporposes.
Nuclear Modeling Applied to Radioisotope Production
M. G. Mustafa
Lawrence Livermore National Laboratory, Livermore, CA, U.S.A. 94550
and
M. Blann, San Diego, CA, U. S. A.
Abstract
Calculated excitation fimctions are provided for all proton induced reactions listed for the
Coordinated Research Program (CRP) on Development of a Reference Charged Particle
Cross Section Data Base for Medical Radioisotope Production under the International
Atomic Energy Agency (IAEA). The excitation functions are compared with experimental
data sets as provided to the CRP. We discuss the merit of calculated results with respect to
the experimental data.
1) Introduction
In this report we present tabular results of calculated excitation functions for
production of isotopes usefi.das beam monitors or for medical use. This is done as part of
an IAEA-CRP. The reactions considered are summarized on p2, followed by the tabular
information. We present figures, some with experimental results as presented to the CRP,
some with only calculated yields. These are presented following the tables.
The question to be addressed is to what degree nuclear model codes may aid in data
evaluation and production. We will fust give very brief comments on the comparisons
between calculated excitation functions and experimental yields. We will conclude with a
few subjective opinions on the question of the role of theory in evaluation. All calculated
results to be presented in this work were from the HMS Alice codel ), using the Monte
Carlo precompound formulation, with either a Fermi gas level density, or using the shell
dependent model of Kataria and Ramamurthyz). The optical model was used for inverse
reaction cross sections, with an energy mesh size of 0.1 MeV to 0.5 MeV in order to get
smooth behavior with change of incident energy.
1
2) Presentation of Results
In the following we present some discussion of most of the results.
Fig. la, b:
Fig. 2a:
Fig. 3:
Fig.4a
Fig. 4b:
Fig. 6:
1So(p, n) 18F - The ALICE code does not use nuclear structure information
as input, nor does it contain many body break-up physics. Its use for
elements as light as 180 is questionable, yet it has given reasonable results
in the past for targets as light as Be. We have run only the Kataria-
Ramamurthy (hereafter referred to as K-R) level density option due to the
double closed shell structure of 160.
zTAl(p, x) zzNa - The calculated result gives a good reproduction of the
experimental result so far as shape goes. The peak yield is = 50% higher
than (i.e 1.5 times) the experimental meanq). The error at peak is= 25 mb in
a reaction cross section of= 600 mb, or around 4%. Expressed in this
mode, the error is not unreasonable. This point is made to emphasize that
nuclear modeling codes may be expected to be best for prediction of major
channels - those representing a major part of the reaction cross section, and
be more speculative the smaller the fraction of the reaction cross reaction
represented by the product.
na~i ( p,x ) ~V - The calculated result is in quite reasonable agreement with
experiment, being of order 25% high at the maximum.
n~i ( p,x ) ~’Ni - The level density model of Kataria-Rarnamurthy gives a
very good reproduction of the excitation function up to the peak and down
to the precompound tail. The latter is somewhat undeqmxiicted. It has long
been known that shell corrected level densities are required in the Ni-Co
region.
Here we show the overestimation of 5TNiwhich results if Fermi gas level
densities are used. We also show the calculated excitation fbnction for the
direct production of STCU,which would decay into sTNi in activation
measurements. Calculated 5TNiexcitation functions should probably add in
the STCUpredicted yields, since experimental results probably represent
cumulative rather than independent yields.
XWU (p,x)s6Co - The calculations give a good energy dependence for the
excitation function., The Fermi gas result is nearly a factor of 2 high, the
K-R result a factor of two low. The peak cross section is around 14 mb, so
2
the calculations are in error by 7 to 15 mb out of a reaction cross section of
around 900 mb, or of order 1-2910.This again illustrates the difficulty of
calculating small cross sections accurately.
Fig. 9: 11lCd (p,n)l 1lIn - The peak yield of around 800 mb is a major part of the.
reaction cross section. The calculated excitation function is in quite good
agreement with the experimental results. There is some discrepancy in the
threshold region, however some is likely due to error in setting the
experimental energy scale since there appears to be yield below the
minimum threshold Q value.
Fig. 10: 1@i(p,2n)l 1lIn- Calculated and experimental yields are in excellent
agreement; the peak cross section is the major fraction of the reaction cross
section.
Fig. 11: naWd(p,x)11lIn - The calculated yields are in excellent agreement with
experimental results over the entire energy range. The data of Zaitseva
appear to be based on faulty range-energy curves.
Fig. 13a lz71(p,x)lzgXe, 1231-The calculated peak is around 3570 higher than the
experimental peak of around 350 mb. The calculated result also seems to
‘peak’ around 4 MeV below the experimental result. We show the calculated
independent yields for both lzgXe and 1231production.
Fig. 14 a,b,c: 20sTl(p, 3n)zOlPb - Calculations are shown using Fermi gas and K-R level
densities. Both results are in agreement with experimental results to within
= 1090,which is also the order of experimental uncertainties and spread
between different data sets. Again, the peak cross sect.ionl area major part
of the reaction cross section, so we expect the modeled result to do well.
The calculated shapes are not in good agreement with experimental results
on the low energy side (see 14c). The experimental results seem to be
somewhere in between the shapes given by the Fermi-gas and K-R level
density models. The experimental results also vary significantly, and this
may reflect propagation of range-energy errors in stacked foil experiments.
3. Discussions of Results/Conclusions
Nuclear model calculations are certainly useful for providing excitation functions
where measurements have not, or cannot be made. They maybe useful where decay
scheme data necessary for activation measurements are uncertain. They should do best
where the cross sections to be calculated represent a significant fraction of the total reaction
cross section, and more poorly as the yields become increasingly low.
3
The calculations presented he~ for the HMS ALICE code generalIy gave
satisfactory agreement with the experimental trends, but it is and always has been clear that
good experimental data are the fmt choice for evaluated results. Several of the calculations
presented herein agree poorly in the energy range just above threshold. It would be
interesting to see if a Hauser-Feshbach calculation with nuclear structure information gave
an improvement in this regime. Certainly use of the Kataria-Ramamurthy level density
compensated, and indeed overcompensated for this effect for the 203Tl(p, 3n)zOlPb
reaction, indicating that more careful attention to details of the level density may hold a part
of the answer to this question. A consideration of the accuracy of experimental cross
sections is also necessary in the region; range-energy errors propagate and increase in
stacked foil experiments, and may lead to large errors on a result which depends
exponentially on energy.
Work performed under the auspices of the U.S. Department of Energy by the Lawrence
Livermore National Laboratory under contract number W-7405-ENG-48.
References
1) M. Blann, Phys. Rev. C (Sept 1996)
2) S.K Kataria and V.S. Ramamurthy Nut. Phys. A349, 10 (1980)
3) Experimental data present in this work was provided by Dr. F. Tarkanyi, private
communication Nov. 1996.
i
List of Tables
Table 1:
Table 2:
Table 3:
Table 4Z
Table 4b
Table 5:
Table 6:
Table 7:
Table 8:
180(p,n)18Fcalculated excitation functions using Kataria-Rarnamurthy level
density tables
27Al(pX)22Naexcitation fimction calculations
‘~i(p,x)4sV excitation function calculations
@Ni(p,x)S7Ni excitation fimction calculation using K-R level density model
‘~i(p,x)57Ni excitation function calculation using Fermi gas level density
model
“WU(PJ)6243S 65zn excitation function calculations
‘aWu(p,x)56Coexcitation Iinction calculations
6%Zn(p,x)bTGaexcitation function calculations
“Wn(p,x)6TGa excitation function calculations
4
Table 9: 11lCd(p,n) 11lIn excitation function calculations
Table 10 112cd@,2n)l 11~ excitation finction calctdations
Table 11: naWd(p,x)l 1lIn”excitation fi.mctioncalculations
Table 12: lzATe(p,2n)lz31excitation function calculations
Table 13: lzTI(p,x)lzsXe excitation fimction calculations
Table 14: 1271(P,X)1Z31excitation function calculations
Table 15: zOsTl(p,3n)zOlPbexcitation function calculations
5
List of Figures
Fig. la)
Fig. lb)
Fig. 2a)
Fig. 2b)
Fig. 3)
Fig. 4a)
Fig. 4b)
Fig. 4c)
Fig. 5a)
Fig. 5b)
Fig. 6)
Fig. 7a)
Fig. 7b)
Fig. 8a)
Fig. 8b
Fig. 9)
Fig. 10)
Fig. 1la)
Fig. llb
Fig. 12a)
Fig. 12b)
Fig. 13a)
Fig. 13b)
Fig. 14a)
Fig. 14b)
Fig. 14c)
lsO(p,n)lBF excitation function calculated with K-R level densities
lsO(p,n)lsF excitation function calculated with K-R level densities
zTAl(p#zNa calculated and experimental excitation functions
Calculated 2TAl(p,x)22Naexcitation function
-i(p,x)~V calculated and experimental excitation fimctions
naWi(p,x)57Ni calculated and experimental excitation fimctions
@-Ni(p,x)sTNi , 57cU c~culated (Fermi g= leveldensities) and
experimental excitation functionsnatNi(P,x)5TNi,STCUc~c~ated excitation functions
nacu(p,x) 62,63,65Zn c~c~ated excit~on finctions
naWu(p,x)62@, 65Zn calculated excitation functions
na~u(pA)5~o c~culated ~d experimen~ excitation function Fermi g~
results x 1, dashed line; K-Rx 1, solid line.
@%Zn(p,x)GTGacalculated excitation fhnction using Fermi gas level densities
~Zn(p,x)6TGa calculated excitation function using Fermi gas level densities
nWn(p,x)6TGa calculated excitation function using Fermi gas level densities
r%Zn(p,x)67Ga calculated excitation function using Fermi gas level densities11l~(pm)l 11~ c~c~~d ~d expel-imen~ excitation fictions
112Cd(p,n)l1lIn calculated and experimental excitation fi.mctions
n~d(p,x)l 111.ncalculated and experimental excitation functions
n~d(p,x) 11lIn excitation function calculated result
lz4Te(p,2n)lzgI calculated result
12ATe(p,2n)1231calculated result
1271(p,x)lz3Xe, 1231c~c~ated ~d experimen~ excitation fUnct.iOns.
Only primary yields shown for calculated results.
12vI(p,x)lz3Xe, 1231calculated only
z03Tl(p,3n)201Pbcalculated and experimental excitation functions.
2@H(p,3n)zOlPb calculated and experimental excitation functions.
z03Tl(p,3n)201Pbcalculated and experimental excitation functions.
6
Table l.180(p,n)18F excitation function calculatedwith level densities due to Kataria-Ramamurthy model
Elab Reaction Cross 18F(MeV) Section (rob) (rob)
2.62.72.82.93.0
::;4.55.05.56.06.57.07.58.09.0
10.011.012.013.014.016.018.020.025.030.035.040.050.0
448.0466.3488.2505.3521.3585.4628.5651.9665.8677.1690.5708.5726.1742.8751.3743.2713.0679.3654.8635.9624.0615.4618.6615.2557.6505.2477.1
“451.5407.2
0.040.8
::;6.3
23.252.390.0
118.7150.3173.0197.0214.2238.6249.5261.0236.4195.8163.6135.6113.381.161.448.429.019.715.412.08.8
Tab1e2: 27Al(p,x)22Na calculated excitation functions in mb
Elab
(MeV)
12.013.014.015.016.017.018.019.020.021.023.025.027.029.031,033.035.037.039.041.043.045.050.055.060.065.070.080.090.0
ReactionCrossSection
(rob)
799.7816.8821.2811.4788.0761.4737.9719.9707.9703.7702.2703.5697.3681.2659.9639.9624.3612.3601.7591.5581.1571.9547.0526.8508.3491.6476.6450.8428.1
11
25
0.010.050.220.390.590.991.281.521.902.001.781.641.521.461.41
11
24
0.010.080.322.274.917.748.638.447.266.35
11 11
23 22
0.153.5
23.643.641.658.174.090.5
103.6105.1102.888.275.560.751.744.133.025.821.216.414.519.924.732.238.635.8
0.042.27.8
14.124.836.053.563.466.359.450.139.131.626.425.028.2
11
21
0.020.241.354.907.758.026.695.314.31
11
20
0.010.040.09
Elab(MeV)
0.450E+010.460E+010.470E+OI0.480E+010.490E+010.500E+010.5 10E+O10.520E+OI0.530E+010.540E+010.550E+010.560E+010.570E+010.580E+OI0.590E+010.600E+OI0.700E+OI0.800E+010.900E+01O.100E+O2O.110E+O2O.120E+02O.130E+02O.140E+02O.150E+02O.160E+02O.170E+02O.180E+02O.190E+020.200E+020.250E+020.300E+020.350E+020.400E+020.450E+020.500E+020.550E+020.600E+020.650E+020.700E+020.750E+020.800E+020.850E+020.900E+020.950E+02
Table 3: natTi(p,x)AsV calculated excitation functions in mb
::
0. 186E+02O.196E+020.208E+020.2 18E+020.228E+020.237E+020.247E+020.256E+020.265E+020.273E+020.283E+020.291 E+020.298E+020.305E+020.3 11E+020.3 17E+020.359E+020.380E+020.393E+020.404E+020.41 8E+020.430E+020.423E+020.352E+020.258E+020.182E+020.129E+020.938E+010.729E+010.606E+010.360E+010.238E+01O.184E+01O.152E+010.131E+010.128E+OI0.964E+O00.867E+O00.785E+O00.696E+O00.705E+O00.58 lE+OO0.536E+O00.497E+O00.469E+O0
2349
0.185E+02O.195E+020.207E+020.217E+020.227E+020.237E+020.246E+020.256E+020.265E+020.274E+020.282E+020.291E+020.299E+020.307E+020.314E+020.320E+~20.366E+020.388E+020.399E+020.408E+020.359E+020.272E+020.220E+020.240E+020.288E+020.328E+020.347E+020.358E+020.357E+020.354E+020.309E+020.134E+020.739E+OI0.547E+010.443E+010.388E+010.338E+010.301E+OI0.261E+010.236E+010.219E+OI0.203E+010.190E+01O.170E+010.156E+01
2348
0.527E+02O.112E+03O.160E+03O.197E+030.227E+030.251E+030.271E+030.290E+030.306E+030.319E+030.333E+030.412E+030.442E+030.450E+030.465E+030.528E+030.485E+030.496E+030.485E+030.398E+03O.31OE+O30.226E+03O.173E+03O.132E+03O.100E+O30.637E+020.458E+020.395E+020.336E+020.256E+02O.21OE+O2O.175E+02O.151E+02O.132E+020.118E+02O.I08E+02O.106E+O20.919E+010.844E+010.75lE+O1
2347
0.163E+02O.170E+02O.185E+020.200E+020.214E+020.226E+020.239E+020.251E+020.263E+020.274E+020.285E+020,295E+020.304E+020.315E+020.324E+020.332E+020.391E+020.427E+020.437E+020.433E+020.375E+OI0.368E+020.275E+020.183E+020.125E+020.118E+020.554E+02O.112E+030.159E+030.271E+030.254E+03O.136E+030.681E+020.467E+020.378E+020.328E+020.288E+020.243E+020.213E+020.191E+02O.179E+02O.162E+02O.146E+020.136E+02O.127E+02
2346
0.597E+01O.117E+02O.152E+020.181E+020.202E+020.221E+020.236E+020.223E+02O.184E+02O.133E+02o.107E+O2O.103E+O2O.119E+020.976E+01O.163E+020.298E+020.267E+020.199E+02O.154E+02O.113E+020.953E+OI0.829E+010.768E+010.728E+010.639E+010.576E+010.549E+01
2345
0.306E+O00.727E+O00.429E+O00.464E+O00.342E+O00.327E+O00.608E+O00.806E+O00.689E+O00.476E+O00.446E+O00.370E+O00.368E+O00.3 10E+OO0.261E+O0
Table 4a: n@Ni(p,x)s7Ni excitation functions in mb.Kataria-Ramamurthy level density model is used.
E1ab(h4eV)
0.142E+020.144E+020.146E+020.148E+02O.150E+02O.152E+020.154E+02O.156E+02O.158E+02O.160E+02O.162E+02O.164E+02O.166E+02O.168E+02O.170E+02O.172E+02O.174E+02O.176E+02O.178E+02O.180E+020.1 82E+02O.184E+02o.186E+02O.188E+020.190E+020.192E+02O.194E+02O.196E+02O.198E+020.200E+020.250E+020.300E+020.350E+020.400E+020.450E+020.500E+020.550E+020.600E+020.650E+020.700E+020.750E+020.800E+020.850E+020.900E+020.950E+02O.100E+O3
2864
0.739E+O00.729E+O00.727E+O00.714E+O00.702E+O00.692E+O00.682E+O00.669E+O00.664E+O00.660E+O00.639E+O00.637E+O00.630E+O00.631E+O00.614E+O00.628E+O00.609E+O00.613E+O00.606E+O00.594E+O00.576E+O00.574E+O00.580E+O00.581E+O00.560E+O00.575E+O00.577E+O00.566E+O00.544E+O00.581E+O00.443E+O00.368E+O00.301E+O00.263E+O00.223E+O00.197E+O00.169E+O0O.162E+O0O.137E+O00.134E+O00.122E+O0O.1O7E+OO0.969E-010.909E-010.927E-010.802E-01
28 28 28 28 28 2863 62 61 60 59 58
0.370E+O00.408E+O00.459E+O00.5 17E+O00.571E+O00.615E+O00.672E+O00.735E+O00.780E+O00,843E+O00.892E+O00.942E+O0O.IOOE+O1O.1O5E+O10.113E+010.121E+01O.127E+OIO.135E+OIO.140E+010.145E+010.151E+010.158E+010.162E+010.169E+010.175E+01O.174E+01O.184E+010.187E+01O.195E+01o. J98E+010.261E+010.203E+OIO.156E+010, 134E+010.130E+010.124E+010.1 15E+01O.106E+O10.980E+O00.933E+O00.926E+O00.877E+O00.857E+O00.840E+O00.798E+O00.755E+O0
0.792E+010.770E+010.741E+010.712E+010.684E+010.660E+010.626E+010.605E+010.594E+010.565E+010.545E+010.5 17E+010.496E+010.481E+010.463E+010.452E+010.437E+OI0.422E+010.402E+010.394E+010.380E+010.366E+010.357E+010.349E+010.330E+010.323E+010.319E+010.312E+010.303E+010.331E+010.351E+010.448E+010.497E+010.443E+010.362E+010.31 lE+O10.277E+010.252E+010.226E+010.218E+010.209E+01O.197E+01O.189E+010.178E+010.168E+010.161E+01
O.172E+02O.184E+02O.195E+020.204E+020.212E+020.21 8E+020.224E+020.228E+020.230E+020.238E+020.240E+020.243E+020.245E+020.245E+020.247E+020.239E+020.241E+020.240E+020.241E+020.242E+020.242E+020.243E+020.242E+020.242E+020.242E+020.243E+020.243E+020.244E+020.244E+020.240E+020.222E+02O.144E+020.959E+010.952E+010.950E+010.935E+OI0.815E+010.732E+010.657E+010.615E+010.585E+010.551E+010.534E+010.492E+010.472E+010.457E+01
O.146E+03O.140E+030.135E+03O.130E+030.123E+03O.120E+03O.115E+03O.108E+O3O.1O3E+O30.970E+020.92 1E+020.868E+020.822E+020.777E+020.737E+020.700E+020.691E+020.659E+020.628E+020.601E+020.572E+020.520E+020.502E+020.483E+020.468E+020.455E+020.438E+020.429E+020.420E+020.406E+020.298EI-020.308E+020.309E+020.271E+020.203E+02O.169E+02O.160E+02O.147E+020.133E+020.124E+020.1 15E+02O.107E+O2O.1O2E+O20.938E+010.878E+010.865E+01
O.154E+020.208E+020.265E+020.324E+020.386E+020.439E+020.501E+020.569E+020.628E+020.636E+020.693E+020.742E+020.801E+020.859E+020.913E+020.965E+02O.106Ei03O.111E+03O.116E+03O.120E+03O.125E+03o.132E+03O.136E+03O.140E+030.144E+03o.147E+03O.150E+03O.153E+030.156E+03O.158E+03O.175E+030,102E+O30.644E+020.508E+020.457E+020.408E+020.372E+020.234E+020.323E+020.305E+020.288E+020.257E+020.247E+020.243E+020.238E+020.227E+02
0.357E+O00,333E+030.31 1E+030.300E+030.278E+030.259E+030.240E+030.224E+030.207E+03O.192E+03O.179E+030.167E+030.156E+03O.146E+030.136E+03O.128E+030.120E+030.1 13E+03O.1O1E+O30.948E+020.908E+020.874E+020.825E+020.801E+020.785E+020.742E+020.729E+020.699E+020.668E+020.685E+020.376E+020.305E+020.481E+020.567E+020.458E+020.365E+020.297E+020.238E+020.231E+020.219E+020.206E+020.202E+020.181E+020.163E+02O.155E+02O.152E+02
2857
0.158E-010.787E+O00.227E+OI0.413E+010.652E+010.870E+01O.115E+02O.146E+02O.173E+020.204E+020.240E+020.267E+020.301E+020.332Ei020.360E+020.390E+020.443E+020.480E+020.509E+020.540E+020.58 1E+020.609E+020.659E+020.704E+020.741E+020.789E+020.824E+020.821E+02O.177E+030.131E+030.742E+020.596E+020.529E+020.521E+020.547E+020.505E+020.445E+020.406E+020.388E+020.379E+020.390E+020.369E+020.334E+020.317E+02
Table 4b: natNi(p,x)S7Ni using Fermi gas level densities.Calculated excitation functions are in mb.
Elab(MeV)
0.142E+020.144E+02O.146E+02O.148E+02O.150E+020.152E+02O.154E+02O.156E+020.158E+02O.160E+02O.162E+02O.164E+02O.166E+02O.168E+02O.170E+02O.172E+02O.174E+02O.176E+02O.178E+02O.180E+02O.182E+02O.184E+02O.186E+02O.188E+02O.190E+02O.192E+02O.194E+02O.196E+020.198E+020.200E+020.250E+020.300E+020.350E+020.400E+020.450E+020.500E+020.550E+020.600E+020.650E+020.700E+020.750E+020.800E+020.850E+020.900E+020.950E+02
2864
0.760E+O00.775E+O00.802E+O00.812E+O00.804E+O00.815E+O00.816E+O00.817E+O00.819E+O00.837E+O00.823E+O00.820E+O00.829E+O00.848E+O00.842E+O00.832E+O00.813E+O00.836E+O00.827E+O00.825E+O0O.81OE+OO0.802E+O00.828E+O00.812E+O00.8 15E+O00.792E+O00.8 13E+O00.792E+O00.769E+O00.816E+O00.593E+O00.475E+O00.396E+O00.342E+O00.296E+O00.250E+O00.226E+O00.197E+O0O.184E+O00.161E+O0O.150E+O0O.137E+O00.133E+O00.121E+O0O.1O7E+OO
2863
0.576E+10.777E+010.945E-4)1O.123E+O0O.145E+O0O.177E+O00.204E+O00.244E+O00.271E+O00.305E+O00.337E+O00.380E+O00.432E+O00.475E+O00.51 3E+O00.564E+O00.615E+O00.672E+O00.714E+O00.781E+O00.816E+O00.882E+O00.943E+O00.986E+O0O.105E+OIO.1O9E+O1O.114E+01O.122E+01O.129E+010.132E+010.194E+J10.164E+010.131E+01O.122E+010.1 12E+010.1 10E+O10.957E+O00.906E+O00.865E+O00.806E+O00.809E+O00.800E+O00.795E+O00.712E+O00.701E+O0
2862
0.451 E+O14.555E+010.464E+010.465E+010.468E+010.466E+010.473E+010.473E+010.473E+010.475E+OI0.466E+OI0.470E+OI0.465E+010.463E+010.457E+010.451E+010.455E+010.444E+OI0.439E+010.432E+010.431E+010.425E+010.420E+010.425E+010.407E+010.406E+010.407E+010.406E+010.398E+010.408E+010.443E+010.504E+010.538E+010.489E+010.428E+010.371E+010.331E+010.301E+010.280E+010.259E+010.249E+010.227E+010.217E+010.212E+010.200E+01
2861
0.418E+OI0.490E+010.559E+OI0.623E+OI0.665E+OI0.697E+OI0.705E+010.704E+010.690E+010.690E+OI0.709E+010.728E+010.744E+010.761E+010.792E+010.814E+010.837E+OI0.857E+OI0.925E+OI0.943E+010.963E+010.980E+01O.100E+O2O.102E+O2O.105E+O2O.103E+O2O.105E+O2O.107E+O2O.1O9E+O2O.114E+02O.139E+020.975E+010.728E+010.678E+OI0.731E+010.722E+010.665E+010.577E+010.521E+010.485E+010.468E+OI0.444E+010.440E+010.415E+010.387E+01
2860
0.730E+020.733E+020.732E+020.739E+020.741E+020.744E+020.748E+020.741E+020.744E+020.742E+020.741E+020.734E+020.725E+020.7 18E+020.71 1E+020.697E+020.684E+020.672E+020.660E+020.652E+020.639E+020.612E+020.606E+020.594E+020.580E+020.578E+020.568E+020.562E+020.548E+020.572E+020.409E+020.414E+020.362E+020.303E+020.255E+020.219E+020.197E+020.188E+020.168E+020.150E+020.140E+020.130E+020.127E+02O.120E+020.111E+02
2859
0.868E+O00.270E+010.592E+010.817E+01O.134E+02O.196E+020.268E+020.347E+020.430E+020.513E+020.600E+020.683E+020.766E+020.846E+020.926E+020.999E+02O.108E+O30.115E+03O.125E+03O.131E+03O.136E+030.143E+03o.147E+030.152E+030.155E+030.156E+030.159E+030.161E+030.164E+030.165E+030.163E+030.120E+030.769E+020.562E+020.525E+020.483E+020.443E+020.403E+020.375E+020.338E+020.323E+020.305E+020.303E+020.288E+020.274E+02
2858
0.375E+030.371E+030.366E+030.362E+030.359E+030.356E+030.353E+030.349E+030.346E+030.34 1E+030.336E+030.332E+030.326E+030.32 1E+030.316E+030.309E+030.303E+030.296E+030.282E+030.276E+030.267E+030.261E+030.253E+030.245E+030.239E+030.232E+030.226E+030.220E+030.213E+030.217E+03O.115E+03O.119E+03O.154E+03O.132E+03O.101E+O30.784E+020.680E+020.616E+020.571E+020.534E+020.499E+020.460E+020.420E+020.405E+020.390E+02
2857
0. 109E+2O.122E+010.806E+010.158E+020.257E+020.376E+020.508E+020.65 IE+020.802E+020.870E+02O.102E+O3O.117E+030.133E+03O.147E+03O.162E+03O.178E+03O.186E+030.199E+030.212E+030.225E+030.237E+030.248E+030.259E+030.271E+030.280E+030.290E+030.3 12E+030.386E+030.205E+030.121E+030.964E+020.960E+020.925E+020.871E+020.774E+020.717E+020.691E+020.648E+020.607E+020.576E+020.554E+020.537E+02
Table 5: natCu(p,x)62@~65Zn calculated with Fermi gas leveldensities. Excitation functions are in mb.
Elab(MeV)
0.220E+010.230E+010.240E+010.250E+010.260E+010.270E+010.280E+010.290E+010.300E+01O.31OE+O10.320E+010.330E+010.340E+010.350E+010.360E+010.370E+010.380E+010.390E+010.400E+01O.41OE+O10.420E+010.430E+010.440E+010.450E+010.460E+010.470E+010.480E+010.490E+010.500E+01O.51OE+O10.520E+010.530E+010.540E+010.550E+010.560E+010.570E+010.580E+010.590E+010.600E+01O.61OE+O10.620E+010.630E+010.640E+010.650E+010.660E+010.680E+010.700E+010.720E+010.740E+010.760E+010.780E+010.800E+01
30 30 30 3065 64 63 62
0.474E+O00.677E+O00.938E+O00.126E+01o. 166E+010.325E+010.499E+010.628E+010.828E+OIO.1O1E+O2O.122E+02O.146E+02O.172E+020.200E+020.231E+020.263E+020.299E+020.335E+020.374E+020.413E+020.461E+020.505E+020.554E+020.600E+020.643E+020.690E+020.733E+020.780E+020.825E+020.867E+020.914E+020.955E+020.999E+02O.105E+O3O.110E+O30.1 13E+030.1 17E+03O.121E+03O.125E+030.129E+030.132E+030.136E+030.139E+03O.142E+030.148E+03O.154E+03O.160E+03O.165E+030.171E+03O.175E+03O.180E+03
0.170E+020.349E+02O.51OE+O20.651E+020.781E+020.896E+02O.102E+O30.113E+03O.123E+03O.133E+03O.143E+030.152E+030.161E+030.169E+03O.179E+030.187E+030.195E+030.202E+030.209E+030.216E+030.222E+030.228E+030.233E+030.238E+030.248E+030.257E+030.266E+030.275E+030.282E+030.289E+030.295E+03
Table 5 (contd.)
0.820E+OI0.840E+OI0.860E+010.880E+010.900E+010.920E+010.940E+010.960E+01O.I06E+02O.108E+O2O.110E+O2O.112E+02O.114E+02O.116E+02O.118E+02O.120E+02O.122E+02O.124E+02O.126E+02O.128E+02O.130E+02O.132E+020.1 34E+020.1 36E+020.138E+020.140E+020.142E+020.144E+020.146E+020.148E+020.150E+02O.152E+02O.154E+02O.156E+020.158E+02O.160E+02O.162E+02O.170E+02O.180E+020.190E+020.200E+020.250E+020.300E+020.350E+020.400E+020.450E+020.500E+020.525E+020.550E+020.575E+020.600E+020.625E+020.650E+020.675E+020.700E+020.725E+02
O.185E+03O.189E+03O.194E+03O.196E+030.200E+030.205E+030.208E+030.212E+030.223E+030.216E+030.207E+03O.189E+030.177E+03O.163E+03O.150E+03O.138E+03O.127E+03O.122E+030.1 12E+03O.102E+O30.935E+020.857E+020.787E+020.718E+020.661E+020.602E+020.558E+020.546E+020.4%E+020.465E+020.434E+020.403E+020.370E+020.346E+020.323E+020.308E+020.290E+020.269E+020.215E+020.185E+020.161E+020.950E+010.798E+OI0.673E+OI0.593E+OI0.516E+010.463E+010.415E+010.404E+010.334E+010.3 12E+010.303E+010.280E+010.268E+010.256E+010.254E+01
0.525E+01O.140E+020.250E+020.447E+020.589E+020.727E+020.867E+020.995E+020.1 11E+03O.117E+03O.128E+03O.138E+03O.146E+03O.154E+03O.161E+03O.168E+030.173E+030.178E+030.183E+03O.185E+030.189E+030.193E+030.196E+03O.199E+030.200E+030.202E+030.206E+030.208E+03O.21OE+O30.171E+030.174E+030.169E+030.167E+030.958E+020.406E+020.257E+020.192E+020.177E+02O.153E+02O.141E+02O.131E+02O.127E+02O.1O9E+O2O.114E+02O.108E+O2O.101E+O20.980E+010.897E+01
0.301E+030.309E+030.314E+030.309E+030.321E+030.326E+030.330E+030.336E+030.364E+030.367E+030.371E+030.374E+030.376E+030.379E+030.380E+030.382E+030.384E+030.385E+030.386E+030.386E+030.386E+030.387E+030.386E+030.378E+030.365E+030.348E+030.329E+030.310E+030.288E+030.268E+030.249E+030.223E+030.207E+03O.192E+03o.177E+03O.163E+030.144E+030.984E+020.733E+020.586E+020.483E+020.258E+020.495E+020.515E+020.396E+020.290E+020.214E+020.199E+02O.165E+02O.172E+02O.162E+02O.149E+02O.145E+02O.133E+020.125E+020.121E+02
0.345E-010.731E+01O.1%E+020.345E+020.515E+020.709E+020.903E+02O.1O9E+O30.125E+030.131E+030.147E+03O.162E+03O.176E+030.195E+030.320E+020.412E+02O.51OE+O20.599E+020.641E+020.277E+02O.197E+020.180E+020.160E+02O.139E+02O.132E+02O.116E+020.1 15E+02O.109E+O20.891E+010.963E+010.868E+010.836E+010.827E+01
Table 5 (contd.)
0.750E+02 0.259E+01 0.858E+01 0.1 19E+02 0.758E+010.800E+02 0.242E+OI 0.840E+01 0. I06E+02 0.661E+010.850E+02 0.214E+01 0.736E+01 0.985E+01 0.602E+010.900E+02 0.190E+01 O.71OE+OI 0.969E+OI 0.611E+010.950E+02 O.169E+01 0.645E+01 0.852E+01 0.505E+01O.1OOE+O3 O.154E+01 0.5%E+01 0.794E+01 0.534E+01
Table 6: IIatCu(p,x)saCo calculated with Fermi gas level densities.
Elab(MeV)
O.170E+02O.180E+020.190E+020.200E+020.250E+020.300E+020.350E+020.400E+020.450E+020.480E+020.500E+020.525E+020.550E+020.575E+020.600E+020.625E+020.650E+020.675E+020.700E+020.725E+020.750E+020.800E+020.850E+020.900E+020.950E+02O.100E+O3
0.480E+020.500E+020.525E+020.550E+020.575E+020.600E+020.625E+020.650E+020.675E+020.700E+020.725E+020.750E+020.800E+020.850E+020.900E+020.950E+02O.100E+O3
2760
0.205E~5O.174E+O00.193E+010.445E+010.506E+010.466E+010.457E+010.479E+010.469E+010.497E+OI0.454E+010.435E+010.409E+010.397E+010.376E+010.383E+010.387E+010.436E+010.459E+OI0.45 lE+O10.408E+010.416E+01
2760
0. 114E+020.132E+02O.157E+02O.183E+020.190E+020.177E+020.171E+020.158E+020.152E+020.144E+020.150E+020.161E+02O.167E+020.180E+02O.180E+020.164E+02O.156E+02
Excitation functions are in mb~
2759
0.198E+O00.620E+O0O.145E+010.296E+01O.I07E+02O.144E+02O.1OIE+O20.565E+010.623E+010.853E+010.970E+010.119E+020.128E+020.134E+020.138E+02O.138E+02O.147E+02O.150E+02O.149E+020.153E+020.147E+020.141E+020.136E+02O.131E+020.129E+020.130E+02
2758
0. 103E430.3 19E+010.233E+020.440E+020.453E+020.371E+020.300E+020.244E+020.204E+02O.199E+020.214E+020.226E+020.243E+020.255E+020.262E+020.270E+020.272E+020.305E+020.323E+020.321E+020.307E+020.288E+02
Kataria-Ramaurthy
2759
0. 103E+O20.133E+02O.167E+020.201E+020.224E+020.254E+020.283E+020.313E+020.325E+020.341E+020.333E+020.329E+020.3 12E+020.293E+020.282E+020.285E+020.282E+02
2758
O.31OE+O20.272E+020.229E+020.198E+020.185E+020.196E+020.200E+020.212E+020.230E+020.246E+020.259E+020.275E+020.321E+020.347E+020.352E+020.326E+020.320E+02
2757
0.407E-020.211E+010.251E+020.445E+020.513E+020.567E+020.544E+020.512E+020.452E+020.394E+020.349E+020.320E+020.306E+020.306E+020.295E+020.298E+020.325E+020.383E+020.395E+020.397E+02
level densities
2757
0.171E+020.230E+020.282E+020.309E+020.299E+020.278E+020.258E+020.227E+020.21 1E+020.194E+02O.187E+02O.175E+02O.168E+02O.173E+020.197E+020.216E+020.217E+02
2756
0.256E%30.225E-010.391E+O00.263E+010.865E+01O.149E+020.208E+020.268E+020.3 12E+020.322E+020.325E+020.31 1E+020.290E+020.226E+020.207E+02O.21OE+O20.219E+02
2756
0.458E-4150.956E4330.222E-010.239E+O00.765E+O0O.184E+010.303E+010.452E+010.542E+010.666E+010.73 lE+O10.739E+010.775E+010.634E+010.568E+010.532E+010.471E+01
2755
0.494E+50.871E-030.177E+10.756E4310.372E+O0O.1O2E+O10.195E+010.416E+01O.1O2E+O20.138E+020.144E+020.129E+020.1 10E+O2
0.214E-070.889EW50.1 19E-030.173E-020.153E-010.495E-01O.130E+O00.299E+O00.838E+O00.132E+01O.154E+010.141E+01O.132E+01
2755
Table 7: 68 Zn(p,x)67GaCalculated excitation function in mb
WV)
12.212.312.412.512.612.712.812.913.013.113.313.614.014.515.015.516.016.517.017.518.019.021.022.022.523.023.524.025.027.030.035.040.045.050.055.060.070.080.090.0
Reaction CrossSection (rob)
926.4929.1932.1934.6937.3939.6942.2944.4946.9949.0953.5959.8968.3981.3994.9
1008.41023.51039.51056.21073.41089.61119.01130.31119.11112.41107.11102.81099.11096.31109.91140.91110.31089.11067.01041.81018.7994.2951.9912.9878.9
67Ga
(rob)
0.000.026.2
16.429.744.961.980.6
100.4121.3166.0258.6345.5438.1514.1576.5627.2668.7703.4727.3750.5773.2773.8703.9653.4601.1548.3507.3422.9282.9173.2109.676.864.655.447.943.436.928.325.1
Table 8:natZn(p,x)67Ga calculated excitation functions in mb
Elab(A4eV)
0.250E+010.300E+010.350E+OI0.380E+010.390E+010.400E+010.420E+010.450E+010.500E+010.550E+010.600E+OIO.61OE+O10.620E+010.630E+OI0.650E+010.680E+010.700E+010.750E+010.800E+010.850E+010.900E+010.950E+01O.100E+O20.1 10E+O2O.120E+02O.130E+02O.140E+02O.150E+02O.160E+02O.170E+02O.180L+02O.190E+020.200E+020.220E+020.240E+020.250E+020.270E+020.300E+020.350E+020.400E+020.450E+020.500E+020.550E+020.600E+020.700E+020.800E+020.900E+02
3170
0. 163E-01O.107E+OO0.299E+O00.459E+O00.522E+O00.585E+O00.738E+O00.983E+O00.141E+010.1 85E+010.230E+010.239E+010.247E+010.255E+010.271E+010.293E+010.309E+010.346E+010.380E+010.413E+010.442E+010.458E+010.425E+010.311E+010.21 lE+O1O.142E+010.993E+O00.736E+O00.600E+O00.491E+O00.430E+O00.387E+O00.347E+O00.286E+O00.260E+O00.259E+O00.239E+O00.214E+O00.174E+O00.140E+O00.127E+O0O.1O6E+OO0.928EW10.815E-010.678E-010.562E410.497E-01
3169
0.954E-010.622E+O00.208E+010.324E+010.402E+010.454E+010.491E+010.515E+010.538E+010.554E+010.558E+O~0.533E+010.403E+010.275E+010.241E+010.166E+010.959E+O00.625E+O00.506E+O00.426E+O00.399E+O00.344E+O00.306E+O00.232E+O0O.197E+O00.174E+O0
3168
0.975E-03O.147E+02O.173E+020.218E+020.299E+020.432E+020.565E+020.703E+020.729E+020.752E+020.778E+020.823E+020.887E+020.932E+02O.104E+O3O.113E+03O.121E+03O.130E+03O.137E+03O.143E+030.151E+03O.155E+03O.138E+030.929E+020.624E+020.429E+020.307E+020.240E+02O.195E+02O.160E+020.1 19E+020.1 11E+02O.104E+O2O.106E+O20.1 10E+O20.887E+010.646E+010.5 18E+010.432E+010.366E+010.341E+010.279E+010.215E+01O.195E+01
3167
0.938Wll0.660E+O0O.189E+OI0.296E+010.338E+010.381E+010.477E+010.653E+010.944E+01O.124E+02O.154E+02O.159E+02O.164E+02O.170E+02O.180E+02O.194E+020.203E+020.225E+020.245E+020.263E+020.281E+020.297E+020.283E+020.215E+02O.149E+020.288E+020.718E+02O.101E+O3O.121E+03O.135E+03O.144E+03O.148E+03O.150E+03O.134E+030.964E+020.849E+020.561E+020.335E+020.223E+02O.172E+02O.144E+02O.123E+02O.105E+O20.896E+010.766E+010.609E+010.5 17E+01
3166
0. 103E+O20.226E+020.226E+020.445E+020.733E+020.849E+02O.1O6E+O30.121E+030.133E+030.143E+030.151E+03O.158E+030.165E+03O.170E+030.172E+030.170E+03O.131E+030.942E+020.675E+020.555E+020.485E+020.448E+020.367E+020.296E+020.298E+020.340E+020.536E+020.648E+020.472E+020.293E+02O.21OE+O2O.169E+020.151E+020.1 15E+020.991E+010.8 12E+01
Table 9: lllCd(p,n)lllIn calculated excitation functions in mb
Elab Reaction Cross 49 49 49 49 49(MeV) 111 110 109 108 107
4.24.44.64.85.05.25.45.65.86.06.26.46.66.87.07.27.47.67.88.08.28.48.68.89.09.29.49.610.011.012.013.014.016.018.020.025.030.035.040.045.050.055.060.070.080.090.0100.0
Section (rob)
2.34.46.49.2
16.322.332.243.556.170.887.8
107.0127.9150.8177.6205.3232.6259.8287.8315.8343.6371.1401.3428.5455.2481.3506.8531.2581.3694.9797.3889.7966.4
1073.91164.91245.71315.11411.11408.31429.71418.41410.81391.21376.91336.11298.41261.01226.5
2.34.46.4
1%:22.332.243.456.070.887.7
106.9127.9150.7177.3205.2232.0259.2287.4314.9342.7370.0399.3426.4452.7478.7503.6527.2576.0685.8679.7473.5305.2147.498.479.454.248.039.230.225.922.720.117.414.512.011.09.0
0.0105.6403.9787.8951.9
1036.0583,9207.9117.690.877.266.159.152.246.138.430.626.0
0.0483.5879.4626.0247.3155.2127.6114.499.082.571.259.046.7
0.082.2
486.2496.1313.9186.7131.392.278.265.156.0
0.0266.7
237.1294.4226.7108.967.855.148.4
Table 10: l12Cd(p,2n)lllIn calculated excitation functions in mb
Elab(MeV)
11.011.211.411.611.812.012.212.412.612.813.013.213.413.613.814.014.214.414.614.815.015.215.415.615.816.017.217.417.618.020.020.521.021.522.022.523.023.524.024.525.030.035.0
Reaction CrossSection (rob)
700.5721.6742.9763.8784.3804.3823.3842.3860.7878.5897.3913.9929.1945.6960.1973.8986.9998.9
1010.81022.11032.91043.41053.11062.91072.51081.81139.21148.31157.01175.01254.31269.71280.91289.31295.41299.81303.31306.51311.31317.11323.11421.01416.2
49112
692.1710.5710.5682.5642.1629.2583.0535.4490.3446.9406.4369.4332.8302.3273.6247.5226.0204.6186.7162.7149.1138.3127.6119.1111.5106.077.474.473.578.157.755.751.350.850.846.746,946.044.443.842.537.830.5
49111
0.00.04
20.568.527.8
160.5224.5288.8350.4410.6468.7520.4570.1616.6656.8694.9729.1759.0788.4820.5842.8862.4881.4896.8912.0924.6997.3
1006.01014.81023.01096.41103.81111.81100.01063.51003.4922.4853.4763.0673.7593.3202.5126.3
0.04
3?;:80.7
132.7211.2298.2383.5874.0729.2
Table 10 (contd.)
40.045.050.055.060.070.080.090.0100.0
1439.51428.51420.01400.51386.71345.51307.51270.01235.3
25.923.419.917.015.612.710.69.67.6
111.993.181.967.961.750.241.336.032.7
335.6188.3129.5106.394.577.068.258.853.0
Table 11: natCd(p,x)lllIn calculated excitation function in mb.
EM(MeV)
0.400E+010.420E+010.440E+010.460E+010.480E+OI0.500E+010.520E+010.540E+010.560E+010.580E+010.600E+OI0.620E+010.640E+010.660E+010.680E+010.700E+010.720E+010.740E+OI0.760E+010.780E+010.800E+010.820E+010.840E+010.860E+010.880E+010.900E+010.920E+010.940E+010.960E+01O.1OOE+O20.1 10E+O2O.120E+02O.130E+02O.140E+020.150E+020.160E+020.170E+02o. 180E+020.190E+020.200E+020.220E+020.240E+020.260E+020.280E+020.300E+020.320E+020.340E+020.360E+020.380E+020.400E+020.420E+02
lllIn
(rob)
0.000E+OO0.295E+O00.561E+O00.827E+O00.1 19E+01O.21OE+O10.287E+010.414E+010.559E+010.721E+010.91 lE+O10.113E+020.1 38E+020.164E+02O.194E+020.228E+020.264E+020.298E+020.333E+020.370E+020.405E+020.441E+020.476E+020.514E+020.548E+020.582E+020.616E+020.648E+020.678E+020.740E+020.883E+020.131E+030.176E+030.207E+030.222E+030.236E+030.248E+030.257E+030.270E+030.294E+030.325E+030.279E+030.218E+030.190E+030.190E+030.207E+030.242E+030.266E+030.279E+030.278E+030.264E+03
(Ee$
0.440E+020.460E+020.480E+020.500E+020.520E+020.540E+020.560E+020.600E+020.650E+020.700E+020.750E+020.800E+020.850E+020.900E+020.950E+02O.1OOE+O3
0.231E+03O.199E+03O.165E+030.138E+03O.118E+03O.110E+O3O.105E+O30.998E+020.885E+020.758E+020.655E+020.589E+020.536E+020.501E+020.469E+020.447E+02
Elab(MeV)
11.511.611.711.811.912.012.012.112.212.312.412.512.612.712.812.913.013.213.413.613.814.014.214.414.614.815.016.017.018.019.020.021.022.023.025.027.030.035.040.045.050.055.060.070.080.090.0
Table 12: 124Te(p,2n)1231Calculated excitation functions in mb.
Reaction CrossSection (rob)
714.8726.8738.7750.4761.3772.7772.7783.9794.9805.7816.3826.6836.8848.5858.3867.4876.8895.1914.0930.8947.0962.1977.0991.5
1005.51019.11031.91095.11153.21202.91242.71274.51296.41314.91334.41388.61443.01466.31495.81516.91516.01506.91495.91480.11443.61405.51368.7
53124
704.8716.4720.8716.6703.9687.3687.9668.1645.5624.2600.7575.7552.2529.1505.1481.0458.8413.9373.0335.2301.2289.4260.9234.1212.2193.1174.9116.785.970.862.957.450.150.045.745.142.538.531.228.022.420.018.416.613.210.89.4
53123
0.00.06.7
22.945.672.772.7
102.4134.3167.1200.4234.1268.0301.9335.3367.8399.8460.7518.7572.5619.3646.0687.4725.5761.1793.0820.0931.2
1008.61059.01096.21120.91134.61112.1998.1592.1346.4186.0121.8108.097.583.373.869.055.341.236.0
53122
1.963.0
481.7790.5966.3658.6315.8173.2134.3114.3103.788.266.658.3
Table 13: 1271(p,x)123Xe,1231Calculated excitation functions in mb.
EM(MeV)
35.036.037.038.039.040.041.042.043.044.045.046.047.048.049.050.051.053.055.057.060.063.065.070.075.080.085.090.095.0100.0
54123
0.0010.14
H32.668.1
115.3171.8248.8305.7359.5376.8415.4471.0472.7435.3376.6292.7215.1177.7124.9101.092.881.875.866.663.1
53123
0.0020.050.321.18
u12.219.229.039.151.566.592.9
111.1131.5152.0156.4153.9144.9135.8131.2126.0112.7112.1109.2
a’
Elab ReactionCress(MeV)
35.036.037.038.039.040.042.043.044.045.046.047.048.049.050.051.053.055.057.060.063.070.075.080.085.090.095.0100.0
Elab(lUeV)
35.036.037.038.039.040.041.042.043.044.045.046.047.048.049.050.0
Section(rob)
1517.61528.01534.71537.01535.81533.71531.81534.51536.01536.91536.61534.91532.11530.61527.91525.61522.51519.81514.81501.5149?).71468.61447.51429.31410.21392.41374.81356.8
Reaction CrossSection (rob)
1517.61528.01534.71537.01535.81533.71532.11531.81534.51536.01536.91536.61534.91532.11530.61527.9
54127
20.719.018.420.118.117.916.816.215.715.215.314.814.714.414.113.813.313.312.210.810.910.58.38.27.37.36.66.2
53127
37.837.634.935.734.132.732.332.831.231.530.230.230.429.827.728.4
. ...
Table 14: 1271(p,x)Xe,ICalculated excitation functions
54126
115.7112.3110.1104.7101.399.391.189.887.485.979.679.878.275.972.074.172.969.468.263.859.952.149.044.641.037.936.334.4
53126
97.0100.299.899.397.397.697.896.796.395.795.494.493.794.394.194.3
54125
474.6386.6320.9269.8230.7205.7163.6150.1146.4138.1128.9126.6118.6121.6117.9109.0104.499.695.287.981.580.471.066.061.558.453.950.4
53125
129.2141.8152.8157.6162.5165.3164.5162.7162.9162.1164.1163.7165.4165.7164.1163.6
in mb.
54124
622.3704.1763.3805.6835.2842.4829.1796.1741.1678.3602.0532.5466.0433.83827303.7245.9222.2196.4180.2152.9136.3122.5111.1106.094.788.081.7
53124
3.07.1
14.423.534.547.264.878.893.6
106.7117.9126.4130.3136.7141.7142.3
54123
0.0010.149.2
32.668.1
115.3171.8248.8305.7359.5376.8415.4471.0472.7435.3376.6292.7177.7124.9101.092.881.875.866.663.1
53123
0.0020.050.31.23.26.7
12.219.229.039.151.5
53122
Elab Reaction Cross(MeV) Section (rob)
51.0 1525.653.0 1522.555.0 1519.857.0 1514.860.0 1501.563.0 1490.765.0 1484.470.0 1468.675.0 1447.580.0 1429.385.0 1410.290.0 1392.4100.0 1356.8
53127
29.628.826.324.823.923.122.920.919.917.916.216.814.0
Table 14 (contd.)
53 53126 125
97.495.294.892.092.890.786.185.882.583.482.078.575.6
160.5157.3158.0155.9153.3159.1155.6150.0148.1144.5143.0136.8133.2
53124
141.0139.1144.9143.7140.8139.2138.2134.0132.5132.0127.6117.0115.5
53123
66.592.9
111.1131.5152.0156.4153.9144.9135.8131.2126.0112.1109.2
53122
0.020.340.9 ~4.2
17.732.954.296.3
112.0111.9100.788.685.2
Table 15: 203Tl(p,3n)201Pb
Elab(mev)
17.817.918.018.118.218.318.418.518.618.718.818.919.119.319.519.719.920.120.320.520.720.921.022.023.024.025.026027.028.029.030.031.032.033.034.035.040.045.050.055.060.065.070.075.580.085.090.095.0
Calculated excitation ‘Functions “ “
Reaction CrossSection (rob)
1078.91088.11097.71106.71117.11126.01134.81143.51152.11161.91170.41179.31195.81211.91227.61242.91258.31272.71286.81300.41313.61326.81333.01394.01445.91494.31543.41587.21624.81654.81681.91704.61727.61753.91789.11807.91828.91883.01937.91%4.01974.71985.61979.81975.61965.41952.51940.41924.71909.6
82203
33.533.733.534.333.133.733.533.733.434.733.733.733.933.233.933.432.432.832.533.431.933.532.630.829.628.728.728.027.527.425.924.122.823.021.821.520.320.318.413.913.411.810.810.48.77.98.27.06.5
82202
1031.81037.41045.51047.61054.21053.21053.61047.81042.31033.31025.11011.9981.5944.7928.4885.8839.4792.0743.4694.0648.2601.4582.8402.72903226.5182.6159.5145.7134.5-125.2120.5114.3108.7104.7102.3100.092.079.168.062.355.651.646.443.040.139.836.033.6
m mm
82201
0.51.63.66.8
11.718.427.037.950.965.883.2
102.1145.8196.0224.0280.7341.3401.3462.5522.9581.6638.9665.1905.6
1070.51181.01269.81319.71287.31150.5975.7744.3570.7437.0344.5282.2248.7170.8139.7118.6104.193.487.679.273.969.164.558.857.7
-—.
I@
10-’0
I I I I10 20
Proton energy (MeV)
40
Figure la.
,+--
300
250
I I I I
‘*O(p,n)’8F
10 20 30 40Proton energy (MeV)
70656055
~ 50g 45
g 40j 350 30
~ 25
6 2015105
0
I I I I I 1 I I 1 I I 1 I I I 1 1 I 1 4
A Stoyrr 90
■ Cllm 90
V Heydoggm 76
9 Hormand 66 -3A (Mt’t’i 95 .
■ Peek 79 AMidroi 85 ❑
■ Marquu 51 *
o Midwi 79 A
m Gfultor 62 m+ Gauvin 62 x
■ Qmrning 63 0
A pmmhkin 67 .
■ Wcigd 74 +
m OnfrichwA
Ax
Vukdov 8S
lagurra5-SOlar 88
Marques 52
B8kd 54
Hlnk 52
Fu~ 65
Tobdimr 71
WNAHO 72
A19kNn*w 66
Michd 66
Bo&m8mr 621
o 50 100 150 200Proton energy (MeV)
Figure 2a.
10’
k I I I I
‘Al(p,3p3n)=Na
1=
Proton energy (MeV)
Figure 2b.
500 ~ I I 1 I I [ I I 1 I I I I I I 14
450 –
400 “
350 –
= 300 —gco“~ 250 —oaa
; 200 –
150 –
10o–
50
L00
“%i(p,x)%
+
-1
+
+ –
Al I I I I I I I I I I I ! 110 20 30
Proton energy (Mev)
Figure 3.
I I I I I I I Io Atakamdfov at at. (166’)
400 : ■ Bawandonatat.(1675)A Kaut”m” (1660)
A Wchal at aL(1960)
350 ~ o Nkhal at aL(19ao)x BodanmmataL(laa6)
nTalkanyiot aL(laal)● 6onck at at. (1665)
~ 300 “ A6tay”atd. (1666)
r ■ Brtnknml (1679)_
~ 250 — K-R ‘a*Ni(p,x)57NiA PiotetaL(1662)■ FuNkawa d at. (1660)
.- 0 Lavkovaki (1661)5 ● Ewatt md Btann (1664)
8 200 , Btuck (1963)
@- Haa8bmak d ●l. (1676)
to % Zhwavh at at. (1666)
g 150 ■V cOhM at SL (1655)
+ Bfinkman at aL (lm+ Tanaka at ti (1’72)
100 –o
Li..+.?%x: ...~
50 –
I I 400 10+ 20 30 40 50 60 70 ~ 90
Proton energy (MeV)
Figure 4a.
450 I I I I I I I I
o Alakaandmv at al. (19S7)
400 ~ Ai Bamndonetd. (1975)
A KwtllwI (W&))
I l\ nat. E:~_ .A7w A Miahd ●t 81.(1980)
350
i
.
NI(P,XJ- IVI o Michai ●t al.(moo)x Bodarnann at al. (1995)
❑ Tarkanyl st aL (1~1)● Sonck ataL(19%)A .Swyn et al. (1S9S)
■ Srinknun (1979)
A Piai et al. (1S92)
■ Fumknwa otaL (1990)
o bvkovakl (1991)● twatl and Siam (1964)
9 Stuok (196$)
- Haa@mBkatal. (1~$)* Zhufavlw c181.(19M)
v Cohan at aL (19S5)
+ Srinknun .tsl. (1977)
\ + Tanaka at aL (1972)
L.0 0
100 :
50 y /6\ 57CU
I/ , ‘%+- A-4 --- ---
00~-A-+--..
104 20 30 40 50 60 70 8° ‘oproton energy (MeW
Figure 4b.
10-’0 20 40 60 80 100
Proton energy (MeV)
Figure 4c.
-4;●● I I I ~ I 1
20 40 60 80 100—.proton energy (MeW
Figure 5a.
o 20 40 w Uu IwlI
Proton energy (MeV)
Figure 5b.
!
221- [ I 1 b I I ! 1 I I 1 I 1 I I 1 1 i
18
4
2
0
~ A Gruttef82
o 50 100 150 200
Proton energy (Mev)
Figure 6.
10° I10-’L
oI I I I
20 40 60 80 100
Proton energy (MeV)
Figure 7a.
800
600
200
6*Zn(p,2n)G7Ga
1 I I I
20 40 60 80
proton energy (Mev)
Figure 7b.
‘mZn(p,x)G7Ga
lUo 20 40 60 80 100
Proton energy (MeV)
Figure 8a.
150
ao
‘tZn(p,x)@7Ga
I I
20 40 60 100
Proton energy (MeV)
Figure 8b.
900 t I 1 1 I I 1 I t I I 1 I 1 1 I I I 1 I I 1 1 I 1 [
lllCd(p,n)lllln+ Tarkanyi 94
■ Wing 62 1
,q-j~,l,,,,l
k
EH0 Otozai 66
: auu)1 Arm ● Skakun 75
A Skakun 79
t A Marten 85
I I 1 I 1 -. I I I I I 1 I t 1“o- 20 40 60 80 100
Proton energy (MeV)
Figure 9.
i
1200~,lll[llll]Jl111111 ‘1’ ’’’] ’’’’ 1’’’ ’1’’”1 ““-j
1000 ~ “2Cd(p,2n)’” In
zg 800 :
+ Tarkenyi 94
.j 600 :9 Skakun75
#A Otozai 66
❑ Nieckarz 69g 40006 200 :
0 I I ! I 111’ ’’’~’ ’’’l’’’’’”” “’”o 16 20 30 40 50 60 70 80 ‘0
protonenergy(Mev)
Figure 10.
I
350 -,, ,,, ,,, ,,, ,,, ,,, ,,,,, ,,, ,,, ,,, ,,, ,,, ,,, ,,,,, ,,,,
~ 300 5
s 250 7
g 200 r
: 150 Faz 100 r
6 50 F
o-’ 111,,1,,,111111111,,1,11 ,1,,,,1,1111111111111o 10 20 30 40 50 60 70 80 90 100
Proton energy(MeV)
Figure ha.
I I
Id y
z&
.Z 10’600amo6
10° ~
10-’ I I I Io 20 40 60 80 100
Proton energy (MeV)
I I I I I
I I I I
20 40 60 80
Proton energy (Mev)
Figure 12a.
1200
1000
200
0
12%e(p,2n)1=I
/
J I 1 I I-- .-
20 40 60 UuProton energy (Mev)
Figure 12b.
-$!i:’x)’”1I Uv x WilkW’M 75
50 A Pmns 76‘/
w~~--m
I I t I t I Io I I I 1 1 I ! I I I 1 I
20 40 60 80 100
Proton energy (Mev)
Figure 13a.
.
=1 $ .g#co=oalo00e 10’Q
1O-j. m40 50 60 70 80 90 100
Proton energy (MeV)
.
1800 L I I , I i 1 I , 1 I # , , , I I t , iI
I , , ,I
, , I II
1 , 1 ,I
, , 1 ,i
, 1 I 1
1
1600
1400I
%l(p,3n) and 2_l(p,5n)cross sections Lagunas-Solar(natural and enriched targets)
q
n 2%l(p,3n)M1Pb
A ‘%(p,5n)m1PbO 20%(p,5n)201Pb
enriched
AAilA
O AAAn*
.- .. —- —-- .J -!a I -I
OF’1 , 1 I I I I , t I , I I (3A I 1 t I 1 , , 1 I , t , , I a , t , I 1 t I
15 20 25 30 3: 40 46 50 55 60.- .-
proton energy (Mev)
Figure 14a.
.
1600r I I 1 I I I I 1 I I 1 1 i 1 i 1 1 I I I I 1
1600
1400I
g 1000“$ 800
: 600UJs 4000
200
Selected data fir %Y(p,3n)201Pb1
-15
Bonardi et al
/
-1-TkQaimLagunas-SolarHermanne _ xl
WLFD
b20
‘ x b’%9
AHo~F I t I I I I I I t I I I I t i
25Proton energy (MeV)
35
Figure 14b.
,.
‘“”””r===!1-
+/
I
I
I
I
I 1, II I I I I I I
17 f 19 21 23 25 27 29 31proton energy(CMev)
Figure 14c.
Technical Inform
ation Departm
ent • Lawrence Liverm
ore National Laboratory
University of C
alifornia • Livermore, C
alifornia 94551
