2012/01/20 by Maissam Barkeshli, John McGreevy · 2 citations
Physics and Astronomy · #Boson #Cold Atom Physics and Bose-Einstein Condensates #Composite fermion #Condensed matter physics #Electron #Fractional quantum Hall effect #Phase (matter) #Phase diagram #Phase transition #Physics #Quantum Hall effect #Quantum and electron transport phenomena #Quantum mechanics #Quantum phase transition #Quantum phases #Quantum spin Hall effect #Superfluidity #Symmetry breaking #Topological Materials and Phenomena #cond-mat.quant-gas #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.89.235116
published as Phys. Rev. B 89, 235116 (2014) · 5+2 pages, 2 figures
arxiv created 2012/01/20 · openalex publication_date 2014/06/13 · arxiv updated 2014/06/18 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We develop a theory of a direct, continuous quantum phase transition between a bosonic Laughlin fractional quantum Hall state and a superfluid, generalizing the Mott insulator to superfluid phase diagram of bosons to allow for the breaking of time-reversal symmetry. The direct transition can be protected by a spatial symmetry, and the critical theory is a pair of Dirac fermion fields coupled to an emergent Chern-Simons gauge field. The transition may be achieved in optical traps of ultracold atoms by starting with a \ensuremathν=1/2 bosonic Laughlin state and tuning an appropriate periodic potential to change the topology of the composite fermion band structure.