Abstract

The effect of high pressure on the conductivity in the basal plane of HTSC single crystals of Y0.77Pr0.23Ba2Cu3O7−δ is investigated. It has been established that the excess conductivity, Δσ(T), of these single crystals in a wide temperature range Tf < T < T* can be described by an exponential temperature dependence. The description of the excess conductivity using the relation Δσ ~ (1 − T/T*)exp(Δ*ab/T) can be interpreted in terms of the mean-field theory, where T* is represented as the temperature pseudogap opening, and the temperature dependence of the pseudogap (PG) is satisfactorily described in the framework of the BCS-BEC crossover theory. An increase in the applied pressure leads to the effect of narrowing the temperature interval for the realization of the PG-regime, thereby expanding the region of the linear dependence ρ(T) in the ab-plane.

Highlights

  • The study of the pseudogap anomaly continues to be one of the main directions of high-temperature superconductivity (HTSC) physics [1,2,3]

  • Among the theoretical works supporting the first point of view is the crossover theory from the Bardeen–Cooper–Schrieffer (BCS) mechanism to the Bose–Einstein condensation (BEC) mechanism [11], in which the temperature dependencies of the pseudogap were obtained for the case of weak and strong pairing

  • In the present study we investigate the effect of high hydrostatic pressure up to 11 kbar on the temperature dependence of the pseudogap in Y­ 1−xPrxBa2Cu3O7−δ single crystals with an average (x≈0.23) concentration of praseodymium at temperatures far from the critical temperature (T > > Tc)

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Summary

Introduction

The study of the pseudogap anomaly (decrease in the density of states) continues to be one of the main directions of high-temperature superconductivity (HTSC) physics [1,2,3]. Among the theoretical works supporting the first point of view is the crossover theory from the Bardeen–Cooper–Schrieffer (BCS) mechanism to the Bose–Einstein condensation (BEC) mechanism [11], in which the temperature dependencies of the pseudogap were obtained for the case of weak and strong pairing. These dependencies are described by equation: Δ(T ) = Δ(0) − T Δ(0) exp Δ(0) T × ⎡ ⎢ ⎢⎢1 ⎢⎣ +

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