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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)

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