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Volumn 63, Issue 18, 1989, Pages 1996-1999

Phenomenology of the normal state of Cu-O high-temperature superconductors

Author keywords

[No Author keywords available]

Indexed keywords

EID: 33847533065 PISSN: 00319007 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevLett.63.1996 Document Type: Article

Times cited : (2011)

References (16)

1
- 4143113923
- (1987) Phys. Rev. Lett. , vol.59 , pp. 1337
- Gurvitch, M.¹ Fiory, A.T.²

2
- 84926554441
- edited by, J. Müller, J. L. Olsen, North Holland, Amsterdam
- (1988) Materials and Mechanisms of Superconductivity
- Steglich, F.¹

3
- 84927407690
- (a) For a recent review, see T. Timusk and D. B. Tanner, in The Physical Properties of High Temperature Superconductors, edited by D. M. Ginsberg (World Scientific, Singapore, 1987);

5
- 0542376680
- For a review, see, edited by, H. Kamimura, A. Oshiyama, Springer-Verlag, Heidelberg
- (1989) Mechanisms of High Temperature Superconductivity
- Sugai, S.¹

6
- 0001519788
- For a review, see, in Ref. 4. For more recent work, see, for example
- (1989) Phys. Rev. Lett. , vol.63 , pp. 1008
- Lee, M.¹ Kapitulnik, A.² Beasley, M.R.³ Gurvitch, M.⁴

7
- 84927407689
- See, for example, articles by R. E. Walstedt and W. Warren, in Ref. 4; Y. Kitaoka et al., in Ref. 4; and H. Yasuoka, in Ref. 4.

11
- 84927407678
- In contrast to T1-1 for Cu, T1-1 for O is consistent with a Korringa rate or at best with a b term which, appropriately normalized, is only case 1 over 6 of that for Cu. [M. Takigawa (private communication); R. Walstedt (private communication)]. This behavior can only be obtained from a appropriate q vec dependence of P̃. As mentioned earlier, if a smooth function of q vec multiplies Eq. (1), none of the results discussed here are altered. Discussion of the differences between T1-1 for O and Cu requires a detailed microscopic theory for P̃ for Cu-O metals.

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