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  • Letter

Bosonic Pfaffian state in the Hofstadter-Bose-Hubbard model

F. A. Palm1,2,*, M. Buser1,2, J. Léonard3, M. Aidelsburger2,4, U. Schollwöck1,2, and F. Grusdt1,2

  • 1Department of Physics and Arnold Sommerfeld Center for Theoretical Physics (ASC), Ludwig-Maximilians-Universität München, Theresienstrasse 37, D-80333 München, Germany
  • 2Munich Center for Quantum Science and Technology (MCQST), Schellingstrasse 4, D-80799 München, Germany
  • 3Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA
  • 4Department of Physics, Ludwig-Maximilians-Universität München, Schellingstrasse 4, D-80799 München, Germany

  • *f.palm@physik.uni-muenchen.de

Phys. Rev. B 103, L161101 – Published 5 April, 2021

DOI: https://doi.org/10.1103/PhysRevB.103.L161101

Abstract

Topological states of matter, such as fractional quantum Hall states, are an active field of research due to their exotic excitations. In particular, ultracold atoms in optical lattices provide a highly controllable and adaptable platform to study such new types of quantum matter. However, finding a clear route to realize non-Abelian quantum Hall states in these systems remains challenging. Here we use the density-matrix renormalization-group (DMRG) method to study the Hofstadter-Bose-Hubbard model at filling factor ν=1 and find strong indications that at α=1/6 magnetic flux quanta per plaquette the ground state is a lattice analog of the continuum non-Abelian Pfaffian. We study the on-site correlations of the ground state, which indicate its paired nature at ν=1, and find an incompressible state characterized by a charge gap in the bulk. We argue that the emergence of a charge density wave on thin cylinders and the behavior of the two- and three-particle correlation functions at short distances provide evidence for the state being closely related to the continuum Pfaffian. The signatures discussed in this letter are accessible in current cold atom experiments and we show that the Pfaffian-like state is readily realizable in few-body systems using adiabatic preparation schemes.

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