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1 /,
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7 S=1/2 S=0 S=1/2
8
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11 S// m H m H = S G
12 e + +
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31 G Z (t) 1 0 t
32 G Z (t) 1 0 t
33 G Z (t) 1 0 t
34
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38 SR
39 G Z (t) = 1/3 + (2/3)(1-2 t 2 )exp(- 2 t 2 /2) G Z (t) 1-1/3 1/3 0 3/ 3/ t
40 G Z (t) = 1/3 + (2/3)(1-2 t 2 )exp(- 2 t 2 /2) G Z (t) - 1 G Z (t) 1 1/3 1/3 0 3/ 3/ t 1/3 1/3 0 t 1/3 x -1 1/3 y 1/3 z z 1/3 G Z (t) = 1 2/3 G Z (t) = 0 0 G Z (t) 1 t
41 SR G Z (t) 1 1/3 z 0 t
42 SR G Z (t) G Z (t) G Z (t) t 0 t 0 t -1
43 SR G Z (t) G Z (t) 1 1 1/3 1/3 0 t 0 t
44 SR G Z (t) 1 G Z (t) 1 0 t 0 t
45 SR G Z (t) G Z (t) 1 1 1/3 1/3 0 t 0 t
46 25 La 2-x Sr x Cu 1-y Fe y O 4 x = y = 0.01 Raw Asymmetry (%) Time (µsec) T = 20.5 K Normalized Asymmetry La 1.85 Sr 0.15 Cu 0.90 Ni 0.10 O 4 3 K 2 K 0.3 K 20 K 5 K Time (µsec)
47 N. Nishida et al., Jpn. J. Appl. Phys. 26 (1987) L1856
48 SR LF- SR) G Z (t) G Z (t) t 0 t
49
50 SR TF- SR) T > T c G Z (t) 1 0 t -1
51 TF- SR T < T c H c1 < H < H c2 H c1 < H < H c2 vortex vortex (m*/n s ) 1/2
52 TF- SR -2 n s /m*
53
54 SR TF- SR) = ( G Z (t) t
55
56
57 < 10-9 sec sec > 10-5 sec
58
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63 Bohr model E n 2 4 Z me = 2 2 8n ε h 2 4πεon h rn = 2 Zme mµ E 207 m E e o 2 µ e 2 r r e µ
64
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67 RAL PSI TRIUMF KEK-MSL J-PARC Pulse beam : long relaxation of muon spins DC beam : fast muon-spin precession and fast relaxation of muon spins
68 The END
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