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Magnetic techniques for molecular and nanometric
materialsDante Gatteschi &
Roberta Sessoli
February 2008
Diapositive disponibili:
ftp://lamm21.chim.unifi.it/pub/Corso_Gatteschi_Sessoli
Per ogni problema scrivere a: [email protected]
Molecular Magnetic Materials
(nano)
EPR(Gatteschi)
Magnetic Techniques(Sessoli)
Molecular magnetic materials
• simple paramagnets: step 1
• Interacting paramagnets: step 2
• Size effects: step 3
Bulk 3D magnets
The first molecular ferromagnet
Miller, Epstein et al. MolCrystLiqCryst 1985
The first room temperature molecular
magnet
Miller, Epstein et al. Science, 1991
Nitroxides
Tc= 0.6 K
N
NO.
CH3
CH3
CH3CH3
O.
TC= 1.5 K
N
NNO2
O
O
Fullerene
TC= 16 K Alemand et al. Science 1991
p-NC-Cp-NC-C66FF44-CNSSN-CNSSN••: : a monomeric S-based a monomeric S-based radicalradical
Single molecule magnets, SMM
The first single molecule magnet:Mn12-acetate
S4||z
top view
T. Lis Acta Cryst. 1980, B36, 2042.
MS=-10
MS= 10Easy axis of magnetization
lateral view z
Mn(AcO)2•4H2O + KMnO4 in 60% v/v AcOH/H2O
[Mn12O12(OAc)16(H2O)4]·2AcOH·4H2O
Ground stateS = 8*2 - 4*3/2 = 10Msaturation = 2.S = 20B
Barrier 60 K
The library of molecular magnets: single chain magnets
More complex structures
Three different organizations
• 2: embedded in amorphous silica
• 3: LB film• 4: SAM
• Bogani et al. Adv Mater in press
magnetmagnet paramagnetparamagnetsuper super paramagnetparamagnet
Reducing the size
Classical physicsQuantum mechanics????????????
Paramagnet
Inorganic radicalsO2, NO..
Organic radicalsTyrosyl, nitroxides
TM coordination compounds
RE coordinationcompounds
Outline of the EPR section
EPR in a nutshell:• The principle of the experiment • Basic EPR: the spin HamiltonianHF experiments:• Radicals and Biological systems• Clusters
Outline of the EPR section 2
Spin interactions:• The spin hamiltonian of pairs • SH parameters of pairsThe Mn12 testing ground:• Epr• Nmr
EPR Spectroscopy in a Nutshell
• It is like NMR but is limited to paramagnetic systems
• Invented by Zavoiski in Kazan in 1944
• It needs a magnetic field and electromagnetic radiation
• Unlike NMR the field is scanned and the frequency is fixed
.
General design of an EPR General design of an EPR spectrometerspectrometer
SourceSourceklystron (conventional)FIR lasers ( > 240 GHz)Gunn diodes (95-400 GHz)Carcinotron (very High power)
DetectorDetectorcrystal diodesbolometersSchottky diodes
Transmission lineTransmission linerectangular waveguides up to 150 GHz)corrugated waveguides.via space with refocusing devicesoversized waveguides
MagnetMagnetelectromagnets (up to 1.5 Tesla)superconductive magnets (up to 17 Tesla)resistive magnets (30 Tesla)hybrid magnets (45 Tesla)pulsed magnets (hundreds of Tesla)
Sample environmentSample environmentresonating structuretemperature controlmultiple irradiation
.•Most of the efforts for the development of EPR at high frequeny are aimed at the extention at millimeter and sub-millimeter waves of the general design of the conventional microwave bridge.• The main problem along this path is the availability and/or the design and realization of devices (magic Tees, circulator, phase shifter etc.) able to carry on the function of the low-frequency analogoue.
The microvave techniques are used in conventional EPR. The propagation of the radiation is made by using mono- modal metallic rectangular waveguides, metallic cavities and the other devices present in a typical microwave bridge.
The microwave techniques can be successfully extended up to 150 GHz ca. Above this frequency waveguides become eccessively lossy (typical figure of merit 12 dB/m at 250 GHz) and the rectangular or cylindric cavities eccessively small.
EPR Spectroscopy in a Nutshell: Zeeman Term
In a system with S= 1/2, when the static magnetic field is parallel to z,
E(M)= MgμBH
a transition is observed when
gz BH= hν= ge BH0Similar expressions hold for x, and y.
The g values and their anisotropy depend on the chemical environment, therefore they provide structural information
Zeeman Splitting
-0.50
-0.25
0
0.25
0.50
0 2000 4000 6000 8000 10000
h=gBH
-1/2gBH
1/2 gBH
G
cm-1
Some Useful Relations1 GHz= 3.3561x10-2 cm-
1
Res. Freq. Band Res. Field (GHz) g=2.00
9 X 0.3234
35 Q 1.2578
95 W 3.1441
200 7.1876
300 10.7814
500 17.9690
Polycrystalline Powder EPR Spectra
The EPR spectra of polycrystalline powders or frozen solutions provide the gx, gy, and gz values directly provided that the linewidth is smaller than the anisotropy
Polycrystalline Powder Spectra
0.25 0.27 0.30 0.33 0.35
B (T)
g
g||
g
gz
gy
gx
isotropic
axial
rhombic
The Spin Hamiltonian
H = B B.g.S+S.D.S+ k Ik.Ak.S
Zeeman Fine Hyperfine
Interazione iperfine e Interazione iperfine e superiperfinesuperiperfineCu2+ S=1/2
63Cu I=3/2 69%
65Cu I=3/2 31%
1- Termine di contatto: Axx=Ayy=Azz=8/3(gegnBn)|n(0)|2
3- Pseudo- contatto :Interazione spin nucleare-momento orbitalico: è funzione dell’anisotropia di gTraccia non nulla, anisotropo
2- Termine dipolare:
anisotropo, traccia nulla (Axx+Ayy+Azz=0)
2nI+1 n=2, I=1
Informazioni sull’intorno di coordinazione
Il CuIl Cu2+ 2+ nei prioninei prioni
Determinazione dei diversi siti leganti e della stechiometria
Determinazione del numero di azoti leganti per uno dei siti coordinanti
Biochemistry 2003 42, 6794
1 eq.2 eq.3 eq. 4 eq.5 eq.6 eq.
Alta conc. Bassa conc.
5.3 eq. Cu2+
Cu2+ legato
pH=4.00
pH=7.40
Cu2+ libero
Affinità per il Cu2+ a pH>6
7 linee min. 3 N leganti
Q-band of 6
6 in solution. RT, X-band
The spin hamiltonian and the parameters
nucleii
NNCuCuCuCuBsp HH ii
2
10
65656363
1 IASIASIASSgB
g ACu/MHz
AN/MHz
QN/MHz
Euler angle/°
x 2.0405 95 36.3 1.28 = 35
y 2.0405 95 50.5 -0.70 = 14
z 2.1860 632 37.5 -0.58 = 0
High Frequency EPR: Why?
• increased resolution• simpler spectra• orientation effects• spectra from integer spin systems
with large zero field splitting• sign of the zero field splitting• different time scale
Enhanced Resolution
• The g tensor anisotropy of tyrosyl radicals present for instance in Photosystem II is completely resolved at high frequency. This provides important structural information, like their main orientation in the membranes.
Tyrosyl Radicals
• They are present in RNR and in Photosystem II
• RNR: ribonucleotide reductase catalyzes the reduction of ribonucleotide to deoxyribonucleotides
EPR of Tyrosyl rad. of S. typhymurium
250 GHz 9.45 GHz
O
H
HH
H
H H
COOHRHN
H
gx=2.0090
gy=2.0044
gz=2.0022
Tyrosyl Radical
The g values are sensitive to the environment
O
H
HH
H
H H
COOHRHN
H
x
y
gx is the most sensitive, because of the interaction of the non-bonding oxygen orbitalsUn et al. JACS 1999, 121, 5743
Resolution effect
P700+ radical cation of PSI
Tyrosyl Radical in Different Environments
N-ac-L-tyr L-tyr-HCl RNREC PSII YD PSII YZ
gx 2.0094 2.0067 2.00868 2.00740 2.00750
gy na 2.0045 2.00430 2.00425 2.00422
gz na 2.0023 2.00203 2.00205 2.00225
giso 2.0055 2.0045 2.00500 2.00466 2.00466
Brustolon et al. J Phys Chem A 1999, 103, 9636
Tyrosyl Radical in Different Species Tyrosyl radical
of RNR of different species
E.coli 2.0091
mouse 2.0076
herpes 2.0076
typhimurium 2.0089
JACS 120, 5080, 1998
Orientation Effects in membranes
Il tensore g nei metalli di transizione
L’anisotropia del fattore L’anisotropia del fattore gg
x2-y2 xy
xz yz
z2
662
22
8
2 2
zxy
Per un elettrone spaiato si ha:
gi=ge+
n
ng
ii
EE
gLnnLgΛ
g<ge dn n=1-4
g>ge dn n=6-9
g// = ge + 8 /(Edxy-Edx2-y
2)
g = ge + 2 /(Edyz- Edx2-y
2)
dx2-y
2
dz2
dxy
dxz,dyz
Es: Cu2+
elongato
dxy, dxz, dyz
dx2-y
2, dz2
d1, 2T2g
eg
t2g
Es: Ti3+
d2, 3T1g
Es: V3+
d3, 4A1g
Es: Cr3+
d5, 2T2g
Es: Fe3+
basso spin
d5, 6A1g
Es: Fe3+
alto spin
d6, 5T2g
Es: Fe2+
alto spin
Stati fondamentali in campo Stati fondamentali in campo ottaedrico -1ottaedrico -1
d9, 2Eg
Cu2+
Stati fondamentali Eg sono instabili rispetto alla distorsione Jahn-Teller e danno luogo a stati fondamentali orbitalmente non-degeneri
Stati fondamentali in campo Stati fondamentali in campo ottaedrico -2ottaedrico -2
d8, 3A2g
Es: Ni2+
Es: Co2+
d7, 4T2g
d4 , 5Eg
Mn3+
dx2-y
2
dz2
dxy
dxz,dyz
elong.
dz2
dx2-y
2
dxz,dyz
dxy
comp.
dz2
dx2-y
2
dxz,dy
z
dxy
comp.
dx2-y
2
dz2
dxy
dxz,dyz
elong.
Perturbative Approach
= ±/2S
n ng EE
gLnnLgΛ
g=
Valori di g per coordinazione pseudo-ottaedrica
Conf. elett. S Stato fond. gx gy gz
d1 1/2 2T2g ge-2/1 ge-2/2 ge-8/3
d2 1 3T1g ge-9/ ge-9/ ge
d3 3/2 4A2g ge-8/1 ge-8/2 ge-8/3
d4 2 5Eg comp. ge-6/1 ge-6/2 ge
elong. ge-2/1 ge-2/2 ge-8/3
d5 HS 5/2 6A1g ge ge ge
d6 2 5T2g ge+2/1 ge+2/2 ge+2/3
d7 3/2 4T2g Oh 2(5-)/3 2(5-)/3 2(5-)/3
elong. 0 0 2(3-)/3
comp. 4 4 2
d8 1 3A2g ge+8/1 ge+8/2 ge+8/3
d9 1/2 2Eg elong. ge+2/1 ge+2/2 ge+8/3
comp. ge+6/1 ge+6/2 ge
g values for some ions
Configurati
on
S GroundState
gxgy
gz
d1 1/2 T2ga -2/1 -2/2 -8/3
d3 3/2 A2gb -8/1 -8/2 -8/3
d4 2 Egc -2/1 -2/2 -8/3
d8 1 A2gd -8/1 -8/2 -8/3
d9 ½ Ege -2/1 -2/2 -8/3
Spin hamiltonian for an individual spin
H= B B.g1.S1+ S1.D1.S1+ j S1.A1j.Ij+..
Electronic Zeeman
Electron-electron interaction (zero field splitting)
Electron-nucleus interaction
Zero field splitting
H= D[S1z2-S1(S1+1)/3]+ E(S1x
2-S1y2)
0E/D1/3
diagonal
Couples states differing in M by ±2
-1.0
-0.5
0
0.5
1.0
1.5
-1.0 -0.5 0 0.5 1.0
axialaxial axial
Completely rhombic
Completely rhombic
Origin of the zero field splitting
For organic radicals: electron-electron dipolar interaction
For transition metal and rare earth ions: spin-orbit interaction
Ligand field approximation
= ±/2S
n ng EE
gLnnLgΛ
D1=2
A simpler treatmentD=(/2)[gz-(gx+gy)/2]; E=(/4)[gx-gy]
For tetragonally elongated Ni(II):
gx= gy= 2.25; gz= 2.24; =-315 cm-1
D= 1.57 cm-1
3A2
3A1
3E
Higher order termsHigher order terms, which have their origin in higher order perturbations, are most coveniently described by Stevens operator equivalents:
H=n k Bnk On
k operator
parameter
n=0,±2,±4,..±2S; k=0,1…n
Advantages of the Stevens Operators
• They fully exploit the symmetry: easy calculations
• The number of the terms to be included are defined by symmetry
• For a C4 quantization axis only the k= 0 and k= 4 terms must be included
• For C2, k=0,2,4
• The Onk operators couple states differing in
M by ±k
Some examples of operators
k=2 O20=3Sz
2-S(S+1)
O22=(S+
2+S-2)
k=4 O40 =35Sz
4-30S(S+1)Sz2+25Sz
2-6S(S+1)+3S2(S+1)2
O42={(7Sz
2-S(S+1)-5)(S+2+S-
2)}S/2
O43={Sz(S+
3+S-3)}S/2
O44=(S+
4+S-4)/2 {A,B}S=(AB+BA)/2
D=3B20;E=B2
2
Fine StructureWhen the Zeeman term is dominant each line is split into 2S equally spaced lines (fine structure)
For an axial anisotropy the resonance fields are given by:
H(M-M+1)=(g/ge)[H0+D’(M/2)(3cos2-1)]
D’= D/(geB)
Nel limite di gBH>>D e anisotropia uniassiale
H//
2S linee separate da H=2D/gB
H
2S linee separate daH=D/gB
H(MM+1)=(ge/g)[H0+(2M+1)/D’/2]
D’=(3cos2-1)D/(geB)
(M=-3)=9D-3gB H
(M=-2)=4D-2gB H
(M=-1)=1D-1gB H
etc
E(-3,-2)=5D-gB H
E(-2,-1)=3D-gB H
E(-1,-0)=1D-gB H
campi di risonanza:
HR(-3,-2)=(5D-h)/gB
HR(-2,-1)=(3D-h)/gB
HR(-1,-0)=(1D-h)/gB
H//
H
T
2D/gB
D/gB
Per T tutti i livelli sono equipopolati e l’intensità delle righe è proporzionale alla probabilità di transizione
Resonance fields for S states
H(MM+1)=(ge/g)[H0+(2M+1)/D’/2];
D’=(3cos2-1)D/(geB)
H//
H
2D/gB
D/gB
kBT<<gB
H
D < 0
HF-EPR Provides the Sign of DNegative D:±S lie
lowestEasy axis type anisotropy
At low T only the -S-S+1 transition is observed
Quantitative LF Approach
Bencini,A.; Ciofini,I.; Uytterhoeven, M.G. Inorg. Chim. Acta 1998, 274, 90
The energies of the LF levels are calculated using a full matrix diagonalization approach. The SH parameters, in principle to any order, are obtained by best fit of the calculated energies.
Both classic crystal field and Angular Overlap parametrization can be used
Ask him the program!
“EPR silent species”
• Ions with even numbers of unpaired electrons are EPR silent in a conventional X- or Q-band experiment due to large zero field splitting
• HF-EPR spectra of Mn(III), Fe(II), Ni(II), etc. become available
An example
-10
-5
0
5
10
15
0 0.5 1.0 1.5 2.0
H(T)
E (c
m-1)
Chromium(II) Manganese(III)
x2-y2
x2-y2z2
z2
Compressed Elongated
Jahn-Teller distortion
Chromium(II) Aquo Ion329 GHz
D=-2.20 cm-1; g= 1.98
Telser et al Inorg Chem 1998, 37, 5769
Manganese(III): SH Parameters
Compressed:
gz= 2.00; gx=1.97
D= 4.72 cm-1
B20= 3.854 cm-1
B40=-9.82 10-3 cm-1
B44=5.18 10-3 cm-1
Elongated:
gz= 1.96; gx=1.99
D= -4.83 cm-1
B20=-3.948 cm-1
B40=-6.70 10-5 cm-1
B44=1.86 10-3 cm-1
Dq=1600 cm-1
Vanadium(III) Alum
3T1g
3Ag
OhS6
Vanadium(III) EPR
D= 4.8581 cm-1;
gz=1.9500; gxy= 1.8656
Az= 0.0098, Axy= 0.0078 cm-
1
Tregenna-Piggott et al Inorg Chem 1999 38 5928
Gadolinium Contrast Agents
Contrast enhanced MRI is a very effective technique for detecting and characterizing lesions, for identifying patho-physiological abnormalities and for providing functional information.
Usually contrast agents are slowly relaxing paramagnets.
Gd3+ is widely used because of its large spin
Need for understanding the mechanism
Gadolinium Chelates
DOTAP
EOB-DTPA
Multifrequency Gd-DOTAP Spectra
9 GHz
94 GHz
249 GHz
Hpp= 400 G
Hpp= 25 G
Hpp= 9 G
The broadening effect is due to unresolved fine structure
At high frequency Zeeman energy is much larger than zfs and the lines sharpen
JACS 120, 1998m 5060
Gd-DOTAP in multilamellar aqueous dispersion
2
2
eff2
31gg
22zz
2yy
2xx
2 /DDD
R. S. Drago: Physical methods for chemists (Saunders, 1992)
J. S. Griffith: The theory of transition metal ions (Cambridge University Press, 1961)
J. R. Pilbrow: EPR of transition metal ions (Clarendon Press, 1990)
A. Abragam, B. Bleaney: EPR of transition ions (Dover, 1986)
J. A. Weil, J. E. Wertz, J. R. Bolton: Electron Paramagnetic Resonance (Wiley, 1994)
A. Bencini, D. Gatteschi: EPR of Exchange coupled systems (Springer Verlag, 1990)
A. Bencini, D. Gatteschi: Electron Paramagnetic Resonance Spectroscopy, in Inorganic Electronic Structure and Spectroscopy, E.I. Solomon, A.B.P.Lever, Vol. I Wiley 1999
Riferimenti bibliograficiRiferimenti bibliografici
Libri:
O. Kahn Molecular Magnetism VCH, Weinheim 1993.
Review:
A.-L. Barra, L.-C. Brunel, D. Gatteschi, L. Pardi, R. Sessoli, "High Frequency EPR Spectroscopy of Large Metal Ion Clusters. From Zero Field Splitting to Quantum Tunneling of the Magnetization" Acc. Chem. Res. 31, 460-466, 1998.
D. Gatteschi, R. Sessoli “Quantum tunneling of magnetization and related phenomena in molecular materials” Angew. Chem. Int. Ed. 42, 268-297, 2003.
D. Gatteschi, L. Pardi “High Frequency EPR Spectroscopy” in High Magnetic Fields, C. Berthier, L.P. Lévy, G. Martinez, Eds. Springer 2002.
J. van Slageren et al. “Frequency-domain magnetic resonance spectroscopy of moleuclar magnetic materials” Phys. Chem. Chem. Phys. 5, 3837-3843, 2003.
Riferimenti Riferimenti bibliograficibibliografici
Programmi di simulazioneProgrammi di simulazione
Alcuni esempi:
Sim (H. Weihe)http://sophus.kiku.dk/software/epr.html (Inorg. Chem 32, 1993, 1216)
Easyspin (S. Stoll) http://www.esr.ethz.ch
EPRNMR (J. A. Weil & M. J. Mombourquette) http://web.chem.queensu.ca/eprnmr/
3 - Convoluzione spettro (scelta di forme e larghezze di riga)
1 - Definizione del modello e dei parametri2 - Calcolo delle probabilità di transizione per diverse orientazioni e campi