2016/05/11 by David F. Mross, Jason Alicea, Olexei I. Motrunich · 2 citations
Physics and Astronomy · #Boson #Composite fermion #Condensed matter physics #Dirac fermion #Fermi Gamma-ray Space Telescope #Fermion #Geometry #Magnetic field #Physics #Point reflection #Quantum Hall effect #Quantum and electron transport phenomena #Quantum many-body systems #Quantum mechanics #Quantum spin Hall effect #Symmetry (geometry) #Topological Materials and Phenomena #cond-mat.str-el
paper · pdf · doi:10.1103/physrevlett.117.136802
published as Phys. Rev. Lett. 117, 136802 (2016) · 8 pages, 5 figures
arxiv created 2016/05/11 · openalex publication_date 2016/09/22 · arxiv updated 2016/09/28 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/06
We introduce a particle-hole-symmetric metallic state of bosons in a magnetic field at odd-integer filling. This state hosts composite fermions whose energy dispersion features a quadratic band touching and corresponding 2π Berry flux protected by particle-hole and discrete rotation symmetries. We also construct an alternative particle-hole symmetric state-distinct in the presence of inversion symmetry-without Berry flux. As in the Dirac composite Fermi liquid introduced by Son [Phys. Rev. X 5, 031027 (2015)], breaking particle-hole symmetry recovers the familiar Chern-Simons theory. We discuss realizations of this phase both in 2D and on bosonic topological insulator surfaces, as well as signatures in experiments and simulations.