Partial fillings of the bosonic quantum Hall state
arXiv:2212.14559 · doi:10.1103/PhysRevB.108.035136
Abstract
We study bosonic topological phases constructed from electrons. In addition to a bulk excitation energy gap, these bosonic phases also have a fermion energy gap, below which all local excitations in the bulk and on the edge are even combinations of electrons. We focus on chiral phases, in which all low-energy edge excitations move in the same direction, that arise from the short-range entangled quantum Hall state, the bosonic analog of the filled lowest Landau level of electrons. The edge-state theory features an Kac-Moody symmetry that can be decomposed into subalgebras, such as , , and . (Here, , , and denote orthogonal, unitary, and exceptional Lie algebras.) Using these symmetry decompositions, we construct exactly solvable coupled-wire model Hamiltonians for families of long-range entangled or bosonic fractional quantum Hall states that ``partially fill" the state and are pairwise related by a generalized particle-hole symmetry. These long-range entangled states feature either Abelian or non-Abelian topological order. Some support the emergence of non-local Dirac and Majorana fermions, Ising anyons, metaplectic anyons, Fibonacci anyons, as well as deconfined gauge fluxes and charges.
48 pages, 6 figures
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