English

Hydrostatic pressure effect on the pseudogap in Y0.77Pr0.23Ba2Cu3O7-δsingle crystals

Superconductivity 2026-06-27 v1

Abstract

We studied the changes of resistivity ρ(T)\rho(T), superconducting transition temperature TcT_c, fluctuation conductivity σ(T)\sigma'(T), and pseudogap Δ(T)\Delta^*(T) of Y1xPrxBa2Cu3O7δY_{1-x}Pr_xBa_2Cu_3O_{7-\delta} (YPrBCO) (x=0.23x = 0.23) single crystal under hydrostatic pressure (HP) up to 1.1\sim 1.1 GPa. Defects created by magnetic inclusions of PrBa2Cu3O7δPrBa_2Cu_3O_{7-\delta} (PrBCO) were found to play a significant role in the behavior of the sample. The largest decrease in ρ(T)\rho(T) was found depending on HP at a rate of dlnρ(100 K)/dP=(29±0.2)%GPa1d\ln\rho(100~K)/dP = -(29 \pm 0.2) \% \cdot GPa^{-1}. This indicates that the mechanisms of the influence of HP on the ρ(T)\rho(T) and TcT_c of YPrBCO and YBa2Cu3O7δYBa_2Cu_3O_{7-\delta} single crystals are different. From the analysis of the pseudogap, it was revealed that the mechanism of the interaction of charge carriers with magnetic PrBCO impurities changes three times with increasing HP. Relatively low HP, up to 0.5\sim 0.5 GPa, promotes the formation of defects caused by PrBCO magnetic inclusions. Starting from 0.6 GPa, the HP neutralizes the influence of magnetic impurities, and the magnetic maximum on Δ(T)\Delta^*(T) disappears. Above 1.0\sim 1.0 GPa, HP aligns the magnetic moments of PrBCO, and the magnetic maximum reappears on Δ(T)\Delta^*(T), more pronounced than at P=0P = 0.

Cite

@article{arxiv.2606.28794,
  title  = {Hydrostatic pressure effect on the pseudogap in Y0.77Pr0.23Ba2Cu3O7-δsingle crystals},
  author = {A. L. Solovjov and L. V. Bludova and A. S. Kolesnik and E. V. Petrenko and M. V. Shytov and A. Sedda and E. Lähderanta and D. Sergeyev and R. V. Vovk},
  journal= {arXiv preprint arXiv:2606.28794},
  year   = {2026}
}

Comments

13 pages, 8 figures

R2 v1 2026-07-22T20:15:15.515Z