-
3
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-
21844496437
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-
In their paper, the theory of the AHE on the ferromagnetic metals proposed by ref. 4 is corrected and its reality is proved rigorously, by taking account of the correlation between electrons in a consistent way, which makes the lifetime of the quasiparticle finite
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H. Kontani and K. Yamada: J. Phys. Soc. Jpn. 63 (1994) 2627. In their paper, the theory of the AHE on the ferromagnetic metals proposed by ref. 4 is corrected and its reality is proved rigorously, by taking account of the correlation between electrons in a consistent way, which makes the lifetime of the quasiparticle finite.
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J. Phys. Soc. Jpn.
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Kontani, H.1
Yamada, K.2
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4
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36149024918
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The reality of the mechanism of the AHE proposed in their paper has been controversial for years: see ref. 5
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R. Karplus and J. M. Luttinger: Phys. Lev. 95 (1954) 1154. The reality of the mechanism of the AHE proposed in their paper has been controversial for years: see ref. 5.
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Phys. Lev.
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Karplus, R.1
Luttinger, J.M.2
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5
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0012234520
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J. Smit: Physica 21 (1955) 877; ibid. 24 (1958) 39.
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Smit, J.1
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0012234520
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J. Smit: Physica 21 (1955) 877; ibid. 24 (1958) 39.
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Physica
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7
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23544475490
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F. C. Zhang and T. K. Lee: Phys. Rev. Lett. 58 (1987) 2728; G. Aeppli and C. M. Varma: Phys. Rev. Lett. 58 (1987) 2729; D. L. Cox: Phys. Rev. Lett. 58 (1987) 2730.
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Phys. Rev. Lett.
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Zhang, F.C.1
Lee, T.K.2
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8
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24544458490
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F. C. Zhang and T. K. Lee: Phys. Rev. Lett. 58 (1987) 2728; G. Aeppli and C. M. Varma: Phys. Rev. Lett. 58 (1987) 2729; D. L. Cox: Phys. Rev. Lett. 58 (1987) 2730.
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Phys. Rev. Lett.
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Aeppli, G.1
Varma, C.M.2
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9
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11644320353
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F. C. Zhang and T. K. Lee: Phys. Rev. Lett. 58 (1987) 2728; G. Aeppli and C. M. Varma: Phys. Rev. Lett. 58 (1987) 2729; D. L. Cox: Phys. Rev. Lett. 58 (1987) 2730.
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Phys. Rev. Lett.
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Cox, D.L.1
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12
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77952965559
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3 is frequently believed to shows the oddparity superconducting state because of the constant Knight shift below the transition temperature; see Y. Kohori, T. Ko hara, H. Shibai, Y. Oda, Y. Kitaoka and K. Asayama: J. Phys. Soc. Jpn. 57 (1987) 395.
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J. Phys. Soc. Jpn.
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Kohori, Y.1
Ko Hara, T.2
Shibai, H.3
Oda, Y.4
Kitaoka, Y.5
Asayama, K.6
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15
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0039708060
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nqp defined in his paper are equal to χP and χV introduced in our paper, respectively.
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Phys. Rev. B
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Nakano, M.1
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19
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85033745283
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RPA = 1.84.
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RPA = 1.84.
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-
-
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20
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35949011563
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W. Metzner and D. Vollhardt: Phys. Rev. Lett. 62 (1989) 324; U. Brandt and C. Mielsch: Z. Phys. B 75 (1989) 365; V. Janis: Z. Phys. B 83 (1991) 227; F. J. Ohkawa: Phys. Rev. B 44 (1991) 6812; A. Georgs and G. Kotliar: Phys. Rev. B 45 (1992) 6479.
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Phys. Rev. Lett.
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Metzner, W.1
Vollhardt, D.2
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21
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34249965994
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W. Metzner and D. Vollhardt: Phys. Rev. Lett. 62 (1989) 324; U. Brandt and C. Mielsch: Z. Phys. B 75 (1989) 365; V. Janis: Z. Phys. B 83 (1991) 227; F. J. Ohkawa: Phys. Rev. B 44 (1991) 6812; A. Georgs and G. Kotliar: Phys. Rev. B 45 (1992) 6479.
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Z. Phys. B
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Mielsch, C.2
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0000774237
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W. Metzner and D. Vollhardt: Phys. Rev. Lett. 62 (1989) 324; U. Brandt and C. Mielsch: Z. Phys. B 75 (1989) 365; V. Janis: Z. Phys. B 83 (1991) 227; F. J. Ohkawa: Phys. Rev. B 44 (1991) 6812; A. Georgs and G. Kotliar: Phys. Rev. B 45 (1992) 6479.
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Z. Phys. B
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Janis, V.1
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23
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0000517724
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W. Metzner and D. Vollhardt: Phys. Rev. Lett. 62 (1989) 324; U. Brandt and C. Mielsch: Z. Phys. B 75 (1989) 365; V. Janis: Z. Phys. B 83 (1991) 227; F. J. Ohkawa: Phys. Rev. B 44 (1991) 6812; A. Georgs and G. Kotliar: Phys. Rev. B 45 (1992) 6479.
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Phys. Rev. B
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Ohkawa, F.J.1
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24
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0000800335
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W. Metzner and D. Vollhardt: Phys. Rev. Lett. 62 (1989) 324; U. Brandt and C. Mielsch: Z. Phys. B 75 (1989) 365; V. Janis: Z. Phys. B 83 (1991) 227; F. J. Ohkawa: Phys. Rev. B 44 (1991) 6812; A. Georgs and G. Kotliar: Phys. Rev. B 45 (1992) 6479.
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Phys. Rev. B
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, pp. 6479
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Georgs, A.1
Kotliar, G.2
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30
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85033752791
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note
-
c(ω) is negligible in this paper.
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-
-
-
31
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85033742297
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The polarization factor, 1 - Γb,β(0,0) · Az(0)ρ(0), is given up to the 1st order of U as 1 + Uρ(0)/3 (>1)
-
The polarization factor, 1 - Γb,β(0,0) · Az(0)ρ(0), is given up to the 1st order of U as 1 + Uρ(0)/3 (>1).
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-
-
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32
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85033761265
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For J = 5/2 single-site Anderson model without ECF, whose Van Vleck susceptibility is rigorously zero, R = (2J + 1)/2J is proven rigorously in the same way as done in §6. This is also expected for SU(6)-PAM without ECF under the approximation (6.4)
-
For J = 5/2 single-site Anderson model without ECF, whose Van Vleck susceptibility is rigorously zero, R = (2J + 1)/2J is proven rigorously in the same way as done in §6. This is also expected for SU(6)-PAM without ECF under the approximation (6.4).
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-
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33
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33750739025
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For instance, see A. J. Mills and P. A. Lee: Phys. Rev. B 35 (1987) 3394; B. Jin and Y. Kuroda: J. Phys. Soc. Jpn. 57 (1988) 1687.
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Phys. Rev. B
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Mills, A.J.1
Lee, P.A.2
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34
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0642334166
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For instance, see A. J. Mills and P. A. Lee: Phys. Rev. B 35 (1987) 3394; B. Jin and Y. Kuroda: J. Phys. Soc. Jpn. 57 (1988) 1687.
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(1988)
J. Phys. Soc. Jpn.
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Jin, B.1
Kuroda, Y.2
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35
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0002213232
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Such a property of the Pauli's principle has already been pointed out for orbital degenerate Anderson model: see A. Yoshimori: Prog. Theor. Phys. 55 (1976) 67.
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(1976)
Prog. Theor. Phys.
, vol.55
, pp. 67
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Yoshimori, A.1
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37
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0001344825
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H. Schweitzer and G. Czycholl: Z. Phys. B 79 (1990) 377; H. Schweitzer and G. Czycholl: Z. Phys. B 67 (1991) 3724.
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(1990)
Z. Phys. B
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, pp. 377
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Schweitzer, H.1
Czycholl, G.2
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38
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4243354216
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H. Schweitzer and G. Czycholl: Z. Phys. B 79 (1990) 377; H. Schweitzer and G. Czycholl: Z. Phys. B 67 (1991) 3724.
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Z. Phys. B
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Schweitzer, H.1
Czycholl, G.2
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