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Bibliographic Details
Main Authors: Huang, Zongyao, Wang, Zhengjie, Hua, Xiangyu, Wang, Huiyu, Li, Zhaohang, Liu, Shihao, Wang, Zhiwei, Quan, Feixiong, Wang, Zhen, Tao, Jing, He, James Jun, Xiang, Ziji, Chen, Xianhui
Format: Preprint
Published: 2026
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Online Access:https://arxiv.org/abs/2604.00608
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Table of Contents:
  • In two dimensions, a phase-coherent superconducting state is established via a Berezinskii-Kosterlitz-Thouless (BKT) transition, whose critical temperature $T_{\rm BKT}$ is determined by the global superfluid stiffness in uniform superconducting systems. We report that at the interface between (111)-oriented KTaO$_3$ and ferromagnetic EuO, the two-dimensional superconducting state exhibits a BKT transition relying on the direction of in-plane bias current. The highest $T_{\rm BKT}$ occurs when current is applied along one of the [11$\bar{2}$] axes of KTaO$_3$, underscoring a spontaneous breaking of the threefold lattice rotational symmetry. Such directional dependence of $T_{\rm BKT}$ is consistently reflected in the nonreciprocal signals stemming from superconducting fluctuations above the transition. We attribute this phenomenon to an interfacial phase segregation; the phase with higher $T_{\rm BKT}$ self-organizes into quasi-one-dimensional textures that stretch along one of the [11$\bar{2}$] directions. Our results point toward the emergence of exotic phases of matter beyond the description of conventional BKT physics at a superconducting interface that is subjected to ferromagnetic proximity.