Creating a bosonic fractional quantum Hall state by pairing fermions
arXiv:1612.09184 · doi:10.1103/PhysRevB.96.161111
Abstract
We numerically study the behavior of spin-- fermions on a two-dimensional square lattice subject to a uniform magnetic field, where opposite spins interact via an on-site attractive interaction. Starting from the non-interacting case where each spin population is prepared in a quantum Hall state with unity filling, we follow the evolution of the system as the interaction strength is increased. Above a critical value and for sufficiently low flux density, we observe the emergence of a twofold quasidegeneracy accompanied by the opening of an energy gap to the third level. Analysis of the entanglement spectra shows that the gapped ground state is the bosonic Laughlin state. Our work therefore provides compelling evidence of a topological phase transition from the fermionic quantum Hall state at unity filling to the bosonic Laughlin state at a critical attraction strength.
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- Measurable signatures of bosonic fractional Chern insulator states and their fractional excitations in a quantum-gas microscope
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