Vortex phase diagram and temperature-dependent second-peak effect in overdoped Bi$_{2}$Sr$_{2}$CuO$_{6 + \delta}$ crystals

TL;DR

This study maps the vortex phase diagram of overdoped Bi2201 superconductors, revealing a temperature-dependent second-peak effect linked to increased anisotropy and interlayer coupling, with doping influencing vortex stability.

Contribution

It provides the first detailed vortex phase diagram of overdoped Bi2201, highlighting the doping-dependent shift of vortex phases and the role of anisotropy in the second-peak effect.

Findings

Second-peak effect strongly depends on temperature and doping.

Increased doping enhances vortex phase stability and interlayer coupling.

Critical temperature follows a parabolic relation with hole concentration.

Abstract

We study the vortex phase diagram of the single-layer Bi2Sr2CuO6+d (Bi2201) superconductor by means of bulk magnetization measurements on high-quality oxygen-overdoped crystals. In striking contrast with the results found in the moderately-doped two and three-layer Bi-based cuprates, Bi2201 exhibits a strong temperature-dependent second-peak effect. By means of measurements of the in and out-of-plane first-penetration field we provide direct evidence that this phenomenon is mainly associated to an increase of the electromagnetic anisotropy on warming. The effect of oxygen-doping d on the vortex phase diagram results in both the irreversibility and second-peak lines shifting to higher temperatures and fields. This enhanced stability of the Bragg glass phase suggests that the interlayer coupling between Cu-O layers increases with d. In addition, we found that the critical temperature follows the parabolic relation with the number of holes per Cu-O plane that holds for most single and two-layer cuprates.