Magnetic Neutron Scattering and Spin-Polarized Neutrons
Magnetic Neutron Scattering and Spin-Polarized Neutrons
Magnetic Neutron Scattering and Spin-Polarized Neutrons
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<strong>Magnetic</strong> <strong>Neutron</strong> <strong>Scattering</strong><br />
<strong>and</strong><br />
<strong>Spin</strong>-<strong>Polarized</strong> <strong>Neutron</strong>s<br />
C. Ulrich<br />
Department Prof. B. Keimer<br />
Max-Planck-Institute for solid state research, Stuttgart, Germany
Nuclear <strong>Neutron</strong> <strong>Scattering</strong>:<br />
- Elastic <strong>Neutron</strong> <strong>Scattering</strong><br />
Diffraction – Crystal Structure<br />
- Inelastic <strong>Neutron</strong> <strong>Scattering</strong><br />
Excitations - Phonons<br />
<strong>Magnetic</strong> <strong>Neutron</strong> <strong>Scattering</strong>:<br />
- Elastic <strong>Neutron</strong> <strong>Scattering</strong><br />
Diffraction – <strong>Spin</strong> Structure<br />
- Inelastic <strong>Neutron</strong> <strong>Scattering</strong><br />
Excitations - Magnons<br />
ferro / antiferromagnetic<br />
magnetic moment<br />
direction of the spins
(1/2, 1/2, 1/2) - Bragg Reflection<br />
T < 77 K<br />
G -ty p e<br />
Integrated Intensity (cnts/10 sec)<br />
10000<br />
1000<br />
0 50 100 150 200 250<br />
Temperature (K)<br />
µ 0 = 1.72 µ B / V 3+ -ion
TYPE:<br />
Ferromagnet<br />
Antiferromagnet<br />
G-type A-type C-type
(1/2, 1/2, 0) - Bragg Reflection<br />
7 7 K < T < 116 K<br />
C -typ e<br />
Integrated Intensity (cnts/10 sec)<br />
10000<br />
1000<br />
0 50 100 150 200 250<br />
Temperature (K)<br />
µ 0 = 1.05 µ B / V 3+ -ion
QHXWURQ<br />
VSLQ<br />
PDJQHWLF<br />
ILHOG
Q=k f -k i
e -
M(r)<br />
f(Q)<br />
f(Q)<br />
Fourier<br />
Transform<br />
distribution of the e - -spins<br />
around the atom<br />
magnetic form factor<br />
Q
mag. Formfactor of the free Fe 4+ - ion<br />
Intensity (arb. units - [ 1/2 g f mag<br />
])<br />
3000<br />
2500<br />
2000<br />
1500<br />
1000<br />
500<br />
SrFeO 3<br />
mag F. Fe 4+<br />
mag F. Fe 3+<br />
S2<br />
0<br />
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7<br />
sin(Θ)/λ (Å -1 )
Crystal Structure of LaTiO 3
How to distinguish between<br />
magnetic <strong>and</strong> nuclear <strong>Neutron</strong> <strong>Scattering</strong><br />
- temperature dependence<br />
magnetic Bragg peaks vansih above the<br />
magnetic ordering temperature<br />
- magnetic form factor decreases with Q<br />
- polarized neutrons
2000<br />
1800<br />
1600<br />
magnetic<br />
Sr 3<br />
Fe 2<br />
O 7<br />
1800<br />
1600<br />
Int1<br />
Int3<br />
Intensity (cnts/12 sec)<br />
1400<br />
1200<br />
1000<br />
800<br />
600<br />
400<br />
200<br />
AM am 39<br />
AL<br />
38 al<br />
1 234 56 78 91011 1213 14 151617 18 1920 2122324 26<br />
AB 25 2728293031323 34 353637 C DEF GH I JKLMNOPQ RSTUV WX Y AK<br />
a b cd e f gh i j k l mn op q ak<br />
r s t u vw x y ZAABACADAEAFAGAHAIAJ<br />
z a abacadaeafag ah aiaj<br />
magnetic<br />
nuclear<br />
AO<br />
40 4142 aoap AP<br />
AQ<br />
AN an 43 aq<br />
AR ar<br />
44<br />
AS 45 as ATAUAVAWAXAYAZBABBCBD<br />
4647 atauavawax 484950 515253545565758 ay az bab bcbdbebfbg BEBFBG 59 BHBI 6061626364656 bhbibjbkblbmbnbobpbqbrbsbtbubvbw BJBKBLBMBNBOBPBQBRBSBTBUBVBWBXBY 67 68 6970717273 74<br />
75 767 bxby BZCACBCC 78798081 bzcacb cc<br />
0<br />
0.6 0.8 1.0 1.2 1.4<br />
Intensity (cnts / 12 sec)<br />
1400<br />
1200<br />
1000<br />
800<br />
600<br />
400<br />
200<br />
0<br />
0 20 40 60 80 100 120 140 160 180 200<br />
(Q H<br />
, 0, 0 )<br />
Temperature (K)
Lecture Notes<br />
X-Ray <strong>and</strong> <strong>Neutron</strong> <strong>Scattering</strong><br />
B. Keimer <strong>and</strong> C. Ulrich
Inelastic <strong>Neutron</strong> <strong>Scattering</strong><br />
magnon dispersion<br />
Heisenberg Hamiltonian:<br />
H = Σ i j J S i • S j<br />
J = exchange interaction<br />
IUHTXHQF\HQHUJ\<br />
PRPHQWXP<br />
b<strong>and</strong> width ∝ J
Magnon Dispersion Relation in LaMnO 3<br />
inelastic neutron scattering<br />
Q (A -1 )<br />
[1,1,0] [0,0,1]<br />
K. Hirota et al., Physica B 237, 36 (1997)
75,636SHFWURPHWHUDW)50<br />
,,
20<br />
Magnon Dispersion YTiO 3<br />
18<br />
16<br />
14<br />
Energy (meV)<br />
12<br />
10<br />
8<br />
6<br />
4<br />
2<br />
0<br />
(0 0 2)<br />
(0 0 1)<br />
(0 -1 1)<br />
(0 K L) (r.l.u.)<br />
(0 -1 2)<br />
(0 0 2)<br />
Intensity (cnts/70 sec)<br />
400<br />
300<br />
200<br />
100<br />
T = 5 K<br />
T = 50 K<br />
0<br />
0 5 10 15 20 25<br />
Energy (meV)
Y 1-x<br />
Ca x<br />
VO 3<br />
(1 %)<br />
35<br />
Data2 Data3 Data1<br />
Data4<br />
30<br />
YVO 3<br />
1 %<br />
5 %<br />
Energy (meV)<br />
25<br />
20<br />
15<br />
10<br />
5<br />
Y 1-x<br />
Ca x<br />
VO 3<br />
QL<br />
(0.5, 0.5, 1)<br />
QHKL<br />
(0.25, 0.25, 1.5)<br />
0<br />
0.50 0.55 0.60 0.65 0.70 0.75 1.0 1.1 1.2 1.3 1.4 1.5 1.4 1.3 1.2 1.1 0.50 1.0 0.45 0.40 0.35 0.30 0.25<br />
(0.5, 0.5, 0)<br />
(0.5, 0.5, 1)<br />
Qhk<br />
(0.75, 0.75, 0)<br />
(0.25, 0.25, 1)<br />
QHKL<br />
(0.5, 0.5, 1.5)