Abstract

Consideration is given to thermodynamical properties of a three-dimensional Bose-condensate of translation-invariant bipolarons (TI-bipolarons) in magnetic field. The critical temperature of transition, critical magnetic fields, energy, heat capacity and the transition heat of TI-bipolaron gas are calculated. Such values as maximum magnetic field, London penetration depth and their temperature dependencies are calculated. The results obtained are used to explain experiments on high-temperature superconductors.

Highlights

  • Before the discovery of high-temperature superconductivity (HTSC) Bardeen-Cooper-Schrieffer theory [1] (BCS) played the role of fundamental microscopic theory of superconductivity with, no alternative

  • Review of various HTSC theories is presented in numerous papers

  • All the approaches, are based on the same proposition the phenomenon of bosonization of Fermi-particles, or Cooper effect. This proposition straightforwardly leads to the conclusion that the phenomenon of superconductivity is related to the phenomenon of Bose-Einstein condensation (BEC)

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Summary

Introduction

Before the discovery of high-temperature superconductivity (HTSC) Bardeen-Cooper-Schrieffer theory [1] (BCS) played the role of fundamental microscopic theory of superconductivity with, no alternative. Calculation of the ground state energy Ebp for the case of Froehlich Hamiltonian was performed in [38,42] by minimization of (16) in fk and in Ψ in the absence of a magnetic field. This resolves the problem of the low temperature of condensation which arises both in the small radius polaron theory and in the large radius polaron theory in which expression (26) involves the bipolaron mass [50,51,52,53,54,55,56,57] Another important result is that the critical temperature Tc for the parameter values considerably exceeds the gap energy ω0.

Current States of a TI-Bipolaron Gas
Thermodynamic Properties of a TI-Bipolaron Gas in a Magnetic Field
Comparison with the Experiment
Scaling Relations
Summary
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