Abstract
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 bosonic Laughlin state and tuning an appropriate periodic potential to change the topology of the composite fermion band structure.
- Received 24 January 2012
- Revised 29 May 2014
DOI:https://doi.org/10.1103/PhysRevB.89.235116
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