magnetic ordering, magnetic anisotropy and the mean-field
TRANSCRIPT
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Magnetic ordering, magnetic anisotropyand the mean-field theory
Alexandra Kalashnikova
FerromagnetsMean-field approximation
Curie temperature and critical exponents
Temperature dependence of magnetization and Bloch law
Magnetic susceptibility
Magnetic anisotropy
Magnetic-dipole contribution
Magneto-crystalline anisotropy and its temperature dependence
Ferro- and antiferromagnets in an external field
Temperature dependence of magnetization and Bloch law
Antiferromagnets
Neel temperature
Susceptibility
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Magnetic ordering, magnetic anisotropyand the mean-field theory
FerromagnetsMean-field approximation
Curie temperature and critical exponents
Temperature dependence of magnetization and Bloch law
Magnetic susceptibility
Temperature dependence of magnetization and Bloch law
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Mean-field approximation: Weiss molecular field
wMHm
H
JWeiss molecular field - field created by neighbor magnetic momentsμ
Alignment of a magnetic moment μin the total field H+wM ?
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A brief reminder: independent magnetic moments in external field
cosHU
kTUT Thermal energy:
At room temperature:
H
J21101.4
Potential energy of a magnetic moment
μ
cosHUH Potential energy of a magnetic moment in the field H:
J23102.1 In a field of 1MA/m:
003.0~/ TH UU
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H
Induced magnetization
cosexpexp
kT
H
U
U
T
H
Probability for a magnetic moment to orient at the angle θ:
1
cothNM
Full magnetization along the field:
kT
H
Paramagnetism: independent magnetic moments in external field
kT
Langevine function L
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H
Full magnetization along the field:
kT
MH
At RT in the field of 1МА/м:
003.0
1
cothNM
Paramagnetism: independent magnetic moments in external field
003.0
Paramagnetic susceptibility:
HkT
NNLNM
3....)3/()(
2
kT
N
H
Mpara
3
2
Curie law
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H
Quantization of the magnetic moment
zBz Jg
Resulting magnetization along the field:
kT
HgJ B JJJJz ....1,
Fe3+
Gd3+
Paramagnetism: independent magnetic moments in external field
JBBNgJM
Brillouin function
[Henry, PR 88, 559 (1952)]
Cr3+
Fe3+
kT
JJNg Bpara
3
)1( 22
...
3
1
J
JNgJM BAt small :
Curie law
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Ferromagnets: Weiss molecular field
H
JS
)(Sz SBS kT
HHSg mB )(
zSNJH
Weiss field due to exchange interactions J
)( SBz SBg
Averaged projected magnetic moment:
B
zm
g
SNJH
Weiss field due to exchange interactions Jwith N nearest neighbors:
kT
g
SNJHSg
SBSB
zB
Sz
Self-consistent solution
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< S
z>(
)
H
JS
Back to ferromagnets: Weiss molecular field
H=0
< S
HNJ
g
NJS
kTS B
z
)(Sz SBS
kT
HHSg mB )(
2 non-zero solutions: zS
=02 opposite orientations of the order parameter
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BS(
)
H
JS
Ferromagnets (S=1/2): Curie temperature
T1
TC>T1
H=0
T2>TC
Variations of these curves with T:
H
NJ
g
NJS
kTS B
z
)(Sz SBS
=0Ordering temperature:
k
JNTC
2nd order phase transition
At T>TC 0zS
10
Variations of these curves with T:
zS changes continuously with T
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H
JS
Ferromagnets (S=1/2): Magnetization in a vicinity of TC
BS(
)
T1
TC>T1
H=0
T2>TC
HNJ
g
NJS
kTS B
z
)(Sz SBS
=0
At T→TC
0
0
zS 2/1
14
3
T
TS C
z
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H
JS
Ferromagnets (S=1/2): Curie temperature
Ordering temperature:k
JNTC
2nd order phase transition
Mean-field approximation Reality:
1D case:
2D case:
3D case:
Mean-field approximation predicts:
02 k
JTC
k
JTC 4
k
JTC 6
No magnetic ordering
Reality:
k
JTC 269.2
k
JTC 511.4
Agreement gets better for the 3D case
Reason:fluctuations were neglected
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H
JS
Ferromagnets (S=1/2): at low temperatures
BS(
)
T1
TC>T1
H=0
T2>TC
)(Sz SBS
At T→0
SSz
kT
HHSg mB )(
TTz
CeS /2212
1
2/30 )/(1)( CTTMTM
Prediction:
Reality:
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< S
z>(
)
H
JS
Ferromagnets (S=1/2) in applied field
TC0H
< S
)(Sz SBS
Non-zero magnetization above TC
Susceptibility
Above TC
in small fields )( C
Bz
TTk
HS
kT
HHSg mB )(
)(
1
C
TTTTkC
Curie-Weiss law
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Weiss molecular field theory:
1)0( TS
S
M
M
1
0HM
Ferromagnets
0TCT
k
JNTC
2/1
1
T
TS C
z Critical exponentβ=1/2
)(
1
C
TTTTkC
Curie-Weiss lawTemperature CurieCritical exponentγ=-1
Landau theory of phase transitions givesthe same values of critical exponents
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Weiss molecular field theory:
1)0( TS
S
M
M
1
Ferromagnets
0TCT
0.5 1 0.5
TTM CS
)( TTC
)( TTC Landau theory and MF
Spin-spin correlations 16
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Mean-field approximation: Bethe mean-field theory
JS0
From uncorrelated spins to uncorrelated clusters of spins
S0 interaction with its 4 neighbors is treated exactly(cluster)
Sj are subject to effective (Weiss) fieldSj
))2/(ln(
2
NNk
JTC
))2/(ln( NNkC
1D case:
2D case:
3D case:
k
JTC 885.2
k
JTC 993.4
No magnetic ordering
k
JTC 269.2
k
JTC 511.4
Agreement is improved
0CT
Approximation predicts: Reality:
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Temperature dependence of magnetization
At T>0
At T=0
Thermal fluctuations
M(r)=M0
M(r)
Minimum of the exchange energySSz
18
Superposition of harmonic waves – thermal spin waves (introduced by Bloch)
Nonparallel Si Increase of the exchange energy
M(r)
The magnitude of the gradient of M is important!
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Magnetization at T>0
Characteristic period of magnetization variation λλ
λλ>> a (inter-atomic distance)
… … ……
Plane waves in a continuous medium
M(r)=M0+ΔM(r)
|ΔM(r)|<<M0
Small deviation of M from M0
(M(r))2 =M02=const
Length of M is conserved
H
19
λλ<< L (sample size)Plane waves in a continuous medium(some analogy with sound waves)
Energy of a ferromagnet as a function of the spatial distribution of magnetization?
-(M(r)-M0)HIncrease of the Zeeman energy:
Increase of the exchange energy:
Exchange constant
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Magnetization at T>0
… … ……
Energy of a ferromagnet as a function of the spatial distribution of magnetization:
H
20
-(M(r)-M0)HIncrease of the Zeeman energy
Increase of the exchange energy
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Magnetization at T>0
… … ……
H
M , M << M
z
21
Mx, My<< M0Small deviations of M:
M0
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Magnetization at T>0
… … ……H z
22
Introduce complex combinations:
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Magnetization at T>0: Exchange waves
… … ……
H z
23
A sum of the energies of plane waves –spin waves
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Energy of a ferromagnet:
number of quasiparticles - magnonsin the state with an energy:
Magnetization at T>0: magnons
24
Quasi-momentum of magnon
Effective mass of a magnon
Bose-Einstein distribution of thermal magnons
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Each magnon reduces the total magnetic moment of the sample by μ
Quadratic dispersionBose-Einstein distribution
Magnetization at T>0: magnons
25
Bloch (3/2-) law: correct temperature dependence of magnetization at low T
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Magnetic ordering, magnetic anisotropyand the mean-field theory
Antiferromagnets
Neel temperature
Susceptibility
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Antiferromagnets
Magnetic sublattices:
μ1i μ2i
M1=Σμ1i/V M2=Σμ2i/V
M=M1+M2Magnetization(ferromagnetic vector)
Number of magnetic sublattices is equivalent to the number of magnetic ions in the magnetic unit cell
Equivalent magnetic sublattices – same type of magnetic ions in the same crystallographic positions
L=M1-M2 Antiferromagnetic vector)
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Antiferromagnets: Neél temperature
Molecular (Weiss) fieldsfor the case of two sublattices:
HA=wAAMA+wABMB
HB=wBBMB+wBAMA
wAA=wBB=w1Equivalent sublattices:
wAB=wBA=w2
MA=-MB
H=0
Magnetization of a sublattice
A B
T1H=0
BS(
)
Neél temperature:
Magnetization of a sublattice in the presence of the molecular fields:
T1
TN>T1
H=0
T2>TC
For each sublattice:
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Antiferromagnets: susceptibility
Hparafm
1
wAA=wBB=w1>0Equivalent sublattices:
wAB=wBA=w2<0MA=-MB
Asymptotic Curie temperature:
HA=wAAMA+wABMB+H
HB=wBBMB+wBAMA+H
kTpara
1
)(
1
A
afmTTk
1
TCTAT TN
Asymptotic Curie temperature:
Susceptibility above TN: )(
1
C
ferroTTk
kT)( ATTk
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Antiferromagnets: susceptibility
TN
Hparafm
Susceptibility in the Neél point:
Equivalent sublattices: MA=-MB
wAA=wBB=w1>0
wAB=wBA=w2<0
TN
Susceptibility at T=0: χ=0
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Antiferromagnets: some examples
TN
31
[P. W. Anderson, Phys. Rev. 79, 705 (1950)]
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Magnetic ordering, magnetic anisotropyand the mean-field theory
32
Magnetic anisotropy
Magnetic-dipole contribution
Magneto-crystalline anisotropy and its temperature dependence
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Magnetic anisotropy
Magnetic anisotropy energy – energy required to rotate magnetizationfrom an “easy” to a “hard” direction
Magnetization – axial vector
Without anisotropy net magnetization of 3D solids would be weak;in 2D systems it would be absent
[Mermin and Wagner, PRL 17, 1133 (1966)]
M
Sources of anisotropy:•Deformation•Intrinsic electrical fields•Shape etc….
- polar impacts
Magnetization – axial vector
Magnetic anisotropy sets an axis, not a direction33
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Magnetic anisotropy: phenomenological consideration
Uniaxial anisotropy...sinsin 4
22
1 uua KKE
01 uK
01 uK [001] – easy axis
(001) – easy plane
2 KE
Effective anisotropy field
M
Cubic anisotropy
...23
22
212
23
21
23
22
22
211 KKwa
01 K
01 K
easy axes- {100}
easy axes- {111}
...cos2 1
nM
H M
KE uaa
3
34
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Magnetic anisotropy
Compound erg cm-3 erg cm-3
Origins of magnetic anisotropy
Interactions between pairsof magnetic ions
•Magnetic-dipolar interactions
•Anisotropic exchange
•Single-ion anisotropy
Spin-orbit interaction
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Magnetic-dipolar contribution to the anisotropy
cos ϕ=α1 ...35
3
7
6
3
1
)(
21
41
21
q
l
wE ex
x
Dipolar interaction
Cubic crystal
M
For a pair of neighboring ions:
...357
11
qxQuadrupolar interaction
const2 23
21
23
22
22
21 NqEa
N – number of atoms per volume unit
NqK 21 – cubic anisotropy constant
fcc: vcc:NqK 9/161 NqK 1 36
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Hexagonal crystal
θ...sinsin 4
22
1 uua KKE
Cubic crystal
...35
3
7
6
3
1)( 2
141
21
qlE
...23
21
23
22
22
211 KEa
cos ϕ=α
Magnetic-dipolar contribution to the anisotropy
θ21 uua
qlKu ~1
Contributes to the shape anisotropy
This films demonstrate in-plane anisotropy37
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Single-ion anisotropy (crystal-field theory)
Splitting of the 3d shellIn the ligand field:
[001]
[100]
[111]
Spinel CoFe2O4
Co2+ in the octahedral coordination+ trigonal distortion along [111]
O2-
In the ligand field:[100]
x2-y2 ; z2
xy; xz; yz
3d7
Co2+
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Splitting of the 3d shell
[001]
[100]
[111]Co2+ in the octahedral coordination
+ trigonal distortion along [111]
Single-ion anisotropy (crystal-field theory)
Splitting of the 3d shellIn the ligand field + trigonal distortion
Maxima of electronic density– along the axis [111]
Maxima of electronic density– in the plane (111)
x2-y2 ; z2
xy; xz; yz
3d7
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[001]
[100]
[111]
x2-y2 ; z2
Co2+ in the octahedral coordination+ trigonal distortion along [111]
Splitting of the 3d shellIn the ligand field + trigonal distortion
Single-ion anisotropy (crystal-field theory)
xy; xz; yz
3d7Orbital moment L||[111]
Spin-orbit interaction cosLSwSO SL -angle between S и [111]
0Co2+ (3d7)3rd Hunds rule:40
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[001]
[100]
[111]
cosLSwSO SL -angle between S и [111]
Co2+ (3d7) 0
Co2+ in the octahedral coordination+ trigonal distortion along [111]
Single-ion anisotropy (crystal-field theory)
)( 222222xzzyyxa LSNw
Averaging over 4 types of Co2+ positionswith distortions along different {111} axes:
[Slonczewski, JAP 32, S253 (1961) ]
0
01 K41
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Temperature dependence of magneto-crystalline anisotropy
Classical theory gives:
2
)1(
)0(
)(
)0(
)(
nn
S
S
n
n
M
TM
K
TKnna KE
Cubic anisotropy10
)()(
Sn TMTK[Zener, Phys. Rev. 96, 1335 (1954)]
42
Uniaxial anisotropy
)0(
)(
)0(
)(
S
S
n
n
M
TM
K
TK
3
)0(
)(
)0(
)(
S
S
n
n
M
TM
K
TKFe
Exp:Theory:
Competition between different anisotropies gives rise to spin-reorinetation transitions
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Magnetic ordering, magnetic anisotropyand the mean-field theory
Ferro- and antiferromagnets in an external field 43
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Ferromagnets in applied magnetic field: domain walls displacement
[100]
Cubic anisotropy (K1>0)
H
[100]
44
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Technical magnetization processes:magnetization rotation
Reversible rotation towards the field Irreversible rotation towards the field
H H
MMe.a. e.a.
Ferromagnets in applied magnetic field: rotation of magnetization
45
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Magnetization process in a multisublattice medium:spin-flop and spin-flip transitions in an antiferromagnet
H
H
Χmax=-1/w2
H
H
M
H
H
HS=-w2MS 46
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H
If the anisotropy is weak:
Magnetization process in a multisublattice medium:spin-flop and spin-flip transitions in an antiferromagnet
H
M
H
H
H
HC
HSCondition for the spin-flop (spin-reorienetation transition)
47
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Magnetization process in a multisublattice medium:spin-flop and spin-flip transitions in an antiferromagnet
H
If the anisotropy is weak: If the anisotropy is strong:
H
M
If the anisotropy is weak:
H
H
H
If the anisotropy is strong:
H
M
H
H
Spin-flip
HC
HS HC
48