Specific temperature dependence of pseudogap in YBa$_2$Cu$_3$O$_{7-\delta}$ nanolayers

TL;DR

This study investigates the temperature dependence of the pseudogap in YBa2Cu3O7−δ nanolayers, revealing how magnetic layers influence superconducting fluctuations and the pseudogap behavior.

Contribution

First analysis of the pseudogap in YBCO-PrBCO superlattices using the local-pair model across the full temperature range, highlighting magnetic effects on superconductivity.

Findings

Pseudogap temperature dependence analyzed with the local-pair model.

Superconducting fluctuations extend up to 15 K above Tc.

Increasing PrBCO layers enhances the pseudogap maximum and magnetic influence.

Abstract

The pseudogap (PG) derived from the analysis of the excess conductivity $\sigma'(T)$ in superlattices and double-layer films of $YBa_2Cu_3O_{7-\delta}$-$PrBa_2Cu_3O_{7-\delta}$(YBCO-PrBCO), prepared by pulsed laser deposition, is studied for the first time. The $\sigma'(T)$ analysis has been performed within the local-pair (LP) model based on the assumption of the paired fermion (LPs) formation in the cuprate high-$T_c$ superconductors (cuprates) below the representative temperature $T^*\gg T_c$ resulting in the PG opening. Within the model, the temperature dependencies of the PG, $\Delta^*(T)$, for the samples with different number of the PrBCO layers ($N_{Pr}$) were analyzed in the whole temperature range from $T^*$ down to $T_c$. Near $T_c$, excess conductivity was found to be perfectly described by the Aslamasov-Larkin and Hikami-Larkin (Maki-Thompson term) fluctuation theories, suggesting the presence of superconducting fluctuations in a relatively large (up to 15 K) temperature range above $T_c$. All sample parameters were found to change with increase of $N_{Pr}$, finally resulting in the appearance of the pronounced maximum of $\Delta^*(T)$ at high temperatures. The result is most likely due to increasing influence of the intrinsic magnetism of PrBCO ($\mu_{Pr}\approx 4\,\mu_B$) and suggests the possibility to search in that way the change of interplay between the superconductivity and magnetism in cuprates.