Chiral symmetry on the edge of two-dimensional symmetry protected topological phases

Symmetry protected topological (SPT) states are short-range entangled states with symmetry. The boundary of a SPT phases has either gapless excitations or degenerate ground states, around a gapped bulk. Recently, we proposed a systematic construction of SPT phases in interacting bosonic systems, how...

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Bibliographic Details
Main Authors: Chen, Xie (Contributor), Wen, Xiao-Gang (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2014-08-18T14:59:48Z.
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Online Access:Get fulltext
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100 1 0 |a Chen, Xie  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Chen, Xie  |e contributor 
100 1 0 |a Wen, Xiao-Gang  |e contributor 
700 1 0 |a Wen, Xiao-Gang  |e author 
245 0 0 |a Chiral symmetry on the edge of two-dimensional symmetry protected topological phases 
260 |b American Physical Society,   |c 2014-08-18T14:59:48Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/88750 
520 |a Symmetry protected topological (SPT) states are short-range entangled states with symmetry. The boundary of a SPT phases has either gapless excitations or degenerate ground states, around a gapped bulk. Recently, we proposed a systematic construction of SPT phases in interacting bosonic systems, however it is not very clear what is the form of the low-energy excitations on the gapless edge. In this paper, we answer this question for two-dimensional (2D) bosonic SPT phases with Z[subscript N] and U(1) symmetry. We find that while the low-energy modes of the gapless edges are nonchiral, symmetry acts on them in a "chiral" way, i.e., acts on the right movers and the left movers differently. This special realization of symmetry protects the gaplessness of the otherwise unstable edge states by prohibiting a direct scattering between the left and right movers. Moreover, understanding of the low-energy effective theory leads to experimental predictions about the SPT phases. In particular, we find that all the 2D U(1) SPT phases have even integer quantized Hall conductance. 
520 |a National Science Foundation (U.S.) (Grant DMR-1005541) 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review B