-
1
-
-
85037897295
-
-
For a comprehensive description of the physics of the cuprates from this point of view, see P.W. Anderson, The Theory of Superconductivity in the High-(Formula presented) Cuprates (Princeton University Press, Princeton, NJ, 1997).
-
For a comprehensive description of the physics of the cuprates from this point of view, see P.W. Anderson, The Theory of Superconductivity in the High-(Formula presented) Cuprates (Princeton University Press, Princeton, NJ, 1997).
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-
-
-
4
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-
85037915750
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-
C. Buhler and A. Moreo, cond-mat/9807034 (unpublished), and references therein.
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-
-
Buhler, C.1
Moreo, A.2
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12
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-
0001121021
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-
For a recent discussion of the pairing symmetry in (Formula presented) see D.F. Agterberg, Phys. Rev. Lett. 80, 5184 (1998).
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(1998)
Phys. Rev. Lett.
, vol.80
, pp. 5184
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-
Agterberg, D.F.1
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14
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0000301053
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T. Imai, A. W. Hunt, K. R. Thurber, and F. C. Chou, Phys. Rev. Lett. 81, 3006 (1998).
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(1998)
Phys. Rev. Lett.
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, pp. 3006
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Imai, T.1
Hunt, A.W.2
Thurber, K.R.3
Chou, F.C.4
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17
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-
0000670622
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P. Pieri, S. Daul, D. Baeriswyl, M. Dzierzawa, and P. Fazekous, Phys. Rev. B 54, 9250 (1996).
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(1996)
Phys. Rev. B
, vol.54
, pp. 9250
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-
Pieri, P.1
Daul, S.2
Baeriswyl, D.3
Dzierzawa, M.4
Fazekous, P.5
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22
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-
85037879620
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-
For a review, see J. Annett, N. Goldenfeld, and A.J. Leggett, in Physical Properties of High Temperature Superconductors V, edited by D.M. Ginsberg (World Scientific, Singapore, 1996).
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For a review, see J. Annett, N. Goldenfeld, and A.J. Leggett, in Physical Properties of High Temperature Superconductors V, edited by D.M. Ginsberg (World Scientific, Singapore, 1996).
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-
-
-
24
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-
85037905865
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-
We do not consider odd-frequency pairing, where even (odd) parity implies triplet (singlet) pairing (Ref. 21
-
We do not consider odd-frequency pairing, where even (odd) parity implies triplet (singlet) pairing (Ref. 21).
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-
-
-
25
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-
85037873427
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-
At a given T, the thermodynamic limit of Eq. (7) is achieved only for a lattice size (Formula presented) In Fig. 66 we have used (Formula presented) The phase diagram calculated for (Formula presented) is essentially identical. Thus we expect (Formula presented)
-
At a given T, the thermodynamic limit of Eq. (7) is achieved only for a lattice size (Formula presented) In Fig. 66 we have used (Formula presented) The phase diagram calculated for (Formula presented) is essentially identical. Thus we expect (Formula presented)
-
-
-
-
26
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-
85037898684
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-
Estimates for ρ=0.25.
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Estimates for ρ=0.25.
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-
-
-
31
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-
0009299938
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-
D. Vollhardt, N. Blümer, K. Held, M. Kollar, J. Schlipf, and M. Ulmke, Z. Phys. B 103, 283 (1997).
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Z. Phys. B
, vol.103
, pp. 283
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Vollhardt, D.1
Blümer, N.2
Held, K.3
Kollar, M.4
Schlipf, J.5
Ulmke, M.6
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34
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-
0030142210
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-
A.P. Mackenzie, S. R. Julian, A. J. Diver, G. J. McMullan, M. P. Ray, G. G. Lonzarich, Y. Maeno, S. Nishizaki, and T. Fujita, Phys. Rev. Lett. 76, 3786 (1996).
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(1996)
Phys. Rev. Lett.
, vol.76
, pp. 3786
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Mackenzie, A.P.1
Julian, S.R.2
Diver, A.J.3
McMullan, G.J.4
Ray, M.P.5
Lonzarich, G.G.6
Maeno, Y.7
Nishizaki, S.8
Fujita, T.9
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