Abstract

The method of synthetic gauge potentials opens up a new avenue for our understanding and discovering novel quantum states of matter. We investigate the topological quantum phase transition of Fermi gases trapped in a honeycomb lattice in the presence of a synthetic non-Abelian gauge potential. We develop a systematic fermionic effective field theory to describe a topological quantum phase transition tuned by the non-Abelian gauge potential and explore its various important experimental consequences. Numerical calculations on lattice scales are performed to compare with the results achieved by the fermionic effective field theory. Several possible experimental detection methods of topological quantum phase transition are proposed. In contrast to condensed matter experiments where only gauge invariant quantities can be measured, both gauge invariant and non-gauge invariant quantities can be measured by experimentally generating various non-Abelian gauges corresponding to the same set of Wilson loops.

Highlights

  • The method of synthetic gauge potentials opens up a new avenue for our understanding and discovering novel quantum states of matter

  • In this work, we investigate the topological quantum phase transition (TQPT) of fermions hopping on a honeycomb lattice in the presence of a synthetic non-Abelian gauge potential

  • In the TQPT in an anisotropic honeycomb lattice studied in[20,23], there is no synthetic gauge potential, the collision is between two time-reversal related Dirac points, so the merging points can only be located at half of a reciprocal lattice

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Summary

Introduction

The method of synthetic gauge potentials opens up a new avenue for our understanding and discovering novel quantum states of matter. We develop a systematic fermionic effective field theory to describe a topological quantum phase transition tuned by the non-Abelian gauge potential and explore its various important experimental consequences. Bermudez et al.[24] studied Fermi gases trapped in a honeycomb optical lattice in the presence of a synthetic SU(2) gauge potential They discovered that as one tunes the parameters of the non-Abelian gauge potential, the system undergoes a topological quantum phase transition (TQPT) from the ND 5 8 massless Dirac zero modes phase to a ND 5 4 phase. Despite this qualitative picture, there remain many important open problems.

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