Time Reversal Symmetry Broken Electronic Phases in Thin Films of Bi$_2$Sr$_2$CaCu$_2$O$_{8+\delta}$

TL;DR

This study investigates how breaking time-reversal symmetry with magnetic fields affects electronic phases in Bi$_2$Sr$_2$CaCu$_2$O$_{8+\

Contribution

It reveals the distinct transport behaviors under TRS preservation and breaking, highlighting the role of topological transitions and disorder in high-Tc superconductor thin films.

Findings

Transport is governed by 2D BKT transition under TRS-preserving conditions.

External magnetic fields induce weak antilocalization before superconductivity is suppressed.

Highly disordered films show 3D weak localization with no superconductivity.

Abstract

High-temperature superconductors (high-Tc SCs) host a rich landscape of electronic phases encompassing the pseudogap, strange metal, superconducting, antiferromagnetic insulating, and Fermi-liquid regimes. The superconducting phase is notable for non-dissipative electronic functionality at relatively high temperatures. These phases are commonly probed in thermodynamic phase space by varying temperature or current through the sample. They can also be probed by breaking time-reversal symmetry (TRS) with an external magnetic field, which yields transition signatures distinct from those arising solely from temperature or current tuning. Here we show that electron transport in Bi$_2$Sr$_2$CaCu$_2$O$_{8+\delta}$ is primarily governed by two-dimensional superconductivity consistent with a Berezinskii-Kosterlitz-Thouless (BKT) topological phase transition, as supported by current-voltage characteristics measured under temperature variation; these measurements preserve TRS. In contrast, when an external magnetic field is applied, the superconducting state is consistently preceded by weak antilocalization (WAL), where bound vortex-antivortex pairs dissociate into a normal metallic state through an intermediate localized phase. We further establish that highly disordered films exhibit transport dominated by three-dimensional weak localization, with superconductivity entirely suppressed.