Anisotropic Superconductivity under an in-plane magnetic field using Corbino electrodes and its implication: From&nbsp;Fe (Te, Se)/Bi<sub>2</sub>Te<sub>3&nbsp;</sub>to&nbsp;Fe (Te, Se)/SrTiO<sub>3</sub>

ORAL

Abstract

Emergent physical phenomena like superconductivity are highly promising for advancements in quantum computing and sensing. Among these, topological superconductivity stands out as a revolutionary solution, as it addresses the long-standing challenge of achieving fault-tolerant quantum computing through the realization of robust and resilient qubits. Symmetry breaking in physics often signals remarkable phenomena. In superconductors, rotational symmetry breaking gives rise to nematic superconductivity, theoretically linked to unconventional Cooper pair pairing. Electrical transport experiments are commonly used to probe rotational symmetry breaking, with Corbino geometry being a widely used tool due to its symmetric device design, enabling azimuthally isotropic electron flow and eliminating geometric artifacts. In this work, using epitaxially grown Fe(Te, Se)/Bi2Te3 thin films, we observe mild six-fold oscillations superposed on dominant two-fold oscillations in the superconducting vortex state. We attribute the two-fold oscillations, surprisingly, to a failure of Corbino geometry in providing truly isotropic electron flow, as confirmed in a polycrystalline s-wave superconductor, MoRe, under similar conditions. By isolating the two-fold background, we uncover intrinsic six-fold oscillations, which we propose originate from interfacial superconductivity contributed by the underlying topological layer, Bi2Te3. These findings challenge conventional assumptions about Corbino geometry and highlight the interplay between topology and superconductivity. Ongoing experiments aim to unravel the precise origins of these intrinsic observations.

*This material is based upon work supported by the U.S. Department of Energy, Office of Science, National Quantum Information Science Research Centers, Quantum Science Center. The photolithography and metal deposition were performed at the Center for Nanophase Materials Sciences, which is a Department of Energy, Office of Science User Facility at Oak Ridge National Laboratory.

Presenters

  • Debarghya (Deb) Mallick

    • Oak Ridge National Laboratory
    • Oak Ridge National Lab

Authors

  • Debarghya (Deb) Mallick

    • Oak Ridge National Laboratory
    • Oak Ridge National Lab
  • Umesh Kumar

    • Oak Ridge National Laboratory
    • Rutgers University
  • Simon Kim

    • Oak Ridge National Laboratory
    • Oak Ridge National Lab
  • An-Hsi Chen

    • Materials Division, Oak Ridge National Laboratory
    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
  • Sujoy Ghosh

    • Oak Ridge National Laboratory
    • Los Alamos National Laboratory
  • Jacob Lowell Cook

    • Oak Ridge National Laboratory
    • University of Missouri
  • Johnson Lu

    • Oak Ridge National Lab
  • Gyula Eres

    • Oak Ridge National Laboratory
  • Steven Randolph

    • Oak Ridge National Lab
  • Satoshi Okamoto

    • Oak Ridge National Laboratory
    • Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • Matthew Brahlek

    • Oak Ridge National Laboratory
  • Robert G Moore

    • Oak Ridge National Laboratory