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Coexistence of the superconducting condensate and the quasi-stationary states of hole pairs

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Abstract

The formation of bound states in the case of a direct Coulomb repulsion between two holes whose reciprocal effective mass tensor has principal values of opposite signs is considered as a possible mechanism of high-T C superconductivity. The study of the specific features of the scattering amplitude shows that, under certain conditions, in addition to the quasi-stationary states, states with a negative attenuation are possible, which corresponds to the tendency toward the formation of a hole pair condensate. The coexistence of the quasi-stationary states and the condensate qualitatively agrees with the phase diagram of p-type doped high-T C superconducting cuprates.

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Translated from Pis’ma v Zhurnal Éksperimental’no\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) i Teoretichesko\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \) Fiziki, Vol. 72, No. 10, 2000, pp. 734–739.

Original Russian Text Copyright © 2000 by Belyavski\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l} \), Kopaev.

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Belyavskii, V.I., Kopaev, Y.V. Coexistence of the superconducting condensate and the quasi-stationary states of hole pairs. Jetp Lett. 72, 511–515 (2000). https://doi.org/10.1134/1.1343154

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  • DOI: https://doi.org/10.1134/1.1343154

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