Abstract:In 2+1-dimensions (2+1D), a gapped quantum phase with no symmetry (i.e. a topological order) can have a thermal Hall conductance κxy = c π 2 k 2 B 3h T , where the dimensionless c is called chiral central charge. If there is a U1 symmetry, a gapped quantum phase can also have a Hall conductance σxy = ν e 2 h , where the dimensionless ν is called filling fraction. In this paper, we derive some quantization conditions of c and ν, via a cobordism approach to define Chern-Simons topological invariants which are as… Show more
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