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Topological semimetal in a fermionic optical lattice

2010/11/30 by Kai Sun, W. Vincent Liu, Andreas Hemmerich +1 · 13 citations
Materials Science · Physics and Astronomy · #Band gap #Cold Atom Physics and Bose-Einstein Condensates #Condensed matter physics #Gapless playback #Graphene research and applications #Optical lattice #Parity (physics) #Phase transition #Physics #Quantum #Quantum mechanics #Quantum phase transition #Quantum phases #Semimetal #State of matter #Symmetry protected topological order #Topological Materials and Phenomena #Topological degeneracy #Topological insulator #Topological order #Topology (electrical circuits) #cond-mat.quant-gas

paper · pdf · doi:10.1038/nphys2134

published as Nature Physics 8, 67-70 (2012) · 6 pages, 3 figures and Supplementary Information

openalex publication_date 2011/11/20 · arxiv created 2012/08/15 · arxiv updated 2012/08/16 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/06

Abstract

Optical lattices play a versatile role in advancing our understanding of correlated quantum matter. The recent implementation of orbital degrees of freedom in chequerboard and hexagonal optical lattices opens up a new thrust towards discovering novel quantum states of matter, which have no prior analogs in solid state electronic materials. Here, we demonstrate that an exotic topological semimetal emerges as a parity-protected gapless state in the orbital bands of a two-dimensional fermionic optical lattice. The new quantum state is characterized by a parabolic band-degeneracy point with Berry flux 2π, in sharp contrast to the π flux of Dirac points as in graphene. We prove that the appearance of this topological liquid is universal for all lattices with D4 point group symmetry as long as orbitals with opposite parities hybridize strongly with each other and the band degeneracy is protected by odd parity. Turning on inter-particle repulsive interactions, the system undergoes a phase transition to a topological insulator whose experimental signature includes chiral gapless domain-wall modes, reminiscent of quantum Hall edge states.

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