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Multipolar Fermi-surface deformation in a Rydberg-dressed Fermi gas with long-range anisotropic interactions

Yijia Zhou1,2, Rejish Nath3, Haibin Wu4,5, Igor Lesanovsky1,6, and Weibin Li1

  • 1School of Physics and Astronomy and Centre for the Mathematics and Theoretical Physics of Quantum Non-equilibrium Systems, University of Nottingham, Nottingham NG7 2RD, United Kingdom
  • 2Graduate School of China Academy of Engineering Physics, Beijing 100193, China
  • 3Department of Physics, Indian Institute of Science Education and Research, Dr. Homi Bhabha Road, Pune 411008, Maharashtra, India
  • 4State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
  • 5Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
  • 6Institut für Theoretische Physik, University of Tübingen, 72076 Tübingen, Germany

Phys. Rev. A 104, L061302 – Published 20 December, 2021

DOI: https://doi.org/10.1103/PhysRevA.104.L061302

Abstract

We study theoretically the deformation of the Fermi surface (FS) of a three-dimensional gas of Rydberg-dressed Li6 atoms. The laser dressing to high-lying Rydberg D states results in angle-dependent soft-core-shaped interactions whose anisotropy is described by multiple spherical harmonics. We show that this can drastically modify the shape of the FS and that its deformation depends on the interplay between the Fermi momentum kF and the reciprocal momentum k¯ corresponding to the characteristic soft-core radius of the dressing-induced potential. When kF<k¯, the dressed interaction stretches a spherical FS into an ellipsoid. When kF≳k¯, complex deformations are encountered which exhibit multipolar characteristics. We analyze the formation of Cooper pairs around the deformed FS and show that they occupy large orbital angular momentum states (p, f, and h wave) coherently. Our study demonstrates that Rydberg dressing to high angular momentum states may pave a route toward the investigation of unconventional Fermi gases and multiwave superconductivity.

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