2021/11/30 by Julian Boesl, Rohit Dilip, Frank Pollmann +1
Physics and Astronomy · #Boson #Condensed matter physics #Density matrix renormalization group #Fractional quantum Hall effect #Magnetic field #Mott insulator #Physics #Physics of Superconductivity and Magnetism #Quantum #Quantum Hall effect #Quantum and electron transport phenomena #Quantum entanglement #Quantum many-body systems #Quantum mechanics #Quantum spin Hall effect #Renormalization group #Topological insulator #Topological order #Topology (electrical circuits) #cond-mat.mes-hall #cond-mat.quant-gas #cond-mat.str-el #quant-ph
paper · pdf · doi:10.1103/physrevb.105.075135
published as Phys. Rev. B 105, 075135 (2022) · 8 pages, 6 figures, published version
openalex created_date 2021/12/06 · openalex publication_date 2022/02/18 · arxiv created 2022/02/21 · arxiv updated 2022/02/23 · openalex updated_date 2026/08/06
The Bose-Hubbard model subjected to an effective magnetic field hosts a plethora of phases with different topological orders when tuning the chemical potential. Using the density matrix renormalization group method, we identify several gapped phases near the first Mott lobe at strong interactions. They are connected by a particle-hole symmetry to a variety of quantum Hall states stabilized at low fillings. We characterize phases of both particle and hole type and identify signatures compatible with Laughlin, Moore-Read, and bosonic integer quantum Hall states by calculating the quantized Hall conductance and by extracting the topological entanglement entropy. Furthermore, we analyze the entanglement spectrum of Laughlin states of bosonic particles and holes for a range of interaction strengths, as well as the entanglement spectrum of a Moore-Read state. These results further corroborate the existence of topological states at high fillings, close to the first Mott lobe, as hole analogs of the respective low-filling states.