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For a recent review see M. Randeria, Proceedings of the International School of Physics, “Enrico Fermi,” Varenna, 1997 (North Holland, New York, in press)
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For a recent review see M. Randeria, Proceedings of the International School of Physics, “Enrico Fermi,” Varenna, 1997 (North Holland, New York, in press).
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0030169494
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M.R. Norman, H. Ding, M. Randeria, J.C. Campuzano, T. Yokoya, T. Takeuchi, T. Takahashi, T. Mochiku, K. Kadowaki, P. Guptasarma, and D.G. Hinks, Nature (London) 392, 157 (1998).
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85038304059
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Although strictly speaking this expression is valid only in the weak coupling limit, it can actually be extended up to intermediate coupling by replacing the bare interaction with a renormalized one. See for example Ref. 9
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Although strictly speaking this expression is valid only in the weak coupling limit, it can actually be extended up to intermediate coupling by replacing the bare interaction with a renormalized one. See for example Ref. 9.
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18
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11944271433
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J.C. Campuzano, G. Jennings, M. Faiz, L. Beaulaigue, B.W. Veal, J.Z. Liu, A.P. Paulikas, K. VanderVoort, H. Claus, R.S. List, A.J. Arko, and R.J. Bartlett, Phys. Rev. Lett. 64, 2308 (1990);
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19
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0000187919
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C.G. Olson, R. Liu, D.W. Lynch, R.S. List, A.J. Arko, B.W. Veal, Y.C. Chang, P.Z. Jiang, and A.P. Paulikas, Phys. Rev. B 42, 381 (1990).
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21
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85038316742
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The factor (Formula presented) determines the symmetry of the order parameter. For an s-wave superconductor (Formula presented) while for a d-wave superconductor (Formula presented)
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The factor (Formula presented) determines the symmetry of the order parameter. For an s-wave superconductor (Formula presented) while for a d-wave superconductor (Formula presented)
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22
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0000697590
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J.M. Singer, M.H. Pedersen, T. Schneider, H. Beck, and H.-G. Matultis, Phys. Rev. B 54, 1286 (1996).
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0031199315
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J. Phys. Chem. Solids (to be published)
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M. Oda, K. Hoya, R. Kubota, C. Manabe, N. Monomo, T. Nakano, and M. Ido, Physica C 281, 135 (1997);H. Ding, J.C. Campuzano, M.R. Norman, M. Randeria, T. Yokoya, T. Takahashi, T. Takeuchi, T. Mochiku, K. Kadowaki, P. Guptasarma, and D.G. Hinks, J. Phys. Chem. Solids (to be published).
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Takeuchi, T.14
Mochiku, T.15
Kadowaki, K.16
Guptasarma, P.17
Hinks, D.G.18
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24
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85038290845
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In obtaining this equation we have used a “soft” cutoff procedure, which ensures that (Formula presented) approaches (Formula presented) continuously at (Formula presented) in order to avoid the spurious singularities that a sharp cutoff would give rise to in the self-energy. For this particular calculation, we have replaced (Formula presented) with (Formula presented)with (Formula presented)
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In obtaining this equation we have used a “soft” cutoff procedure, which ensures that (Formula presented) approaches (Formula presented) continuously at (Formula presented) in order to avoid the spurious singularities that a sharp cutoff would give rise to in the self-energy. For this particular calculation, we have replaced (Formula presented) with (Formula presented)with (Formula presented)
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25
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85038339521
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In this and other plots of the spectral function, a broadening factor (Formula presented) has been added to the imaginary part of the self-energy, in order to make the sharp peaks visible
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In this and other plots of the spectral function, a broadening factor (Formula presented) has been added to the imaginary part of the self-energy, in order to make the sharp peaks visible.
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