Wave functions of bosonic symmetry protected topological phases

We study the structure of the ground-state wave functions of bosonic symmetry protected topological (SPT) insulators in three space dimensions. We demonstrate that the differences with conventional insulators are captured simply in a dual vortex description. As an example, we show that a previously...

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Bibliographic Details
Main Authors: Xu, Cenke (Author), Todadri, Senthil (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2014-09-03T19:24:21Z.
Subjects:
Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Xu, Cenke  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Todadri, Senthil  |e contributor 
700 1 0 |a Todadri, Senthil  |e author 
245 0 0 |a Wave functions of bosonic symmetry protected topological phases 
260 |b American Physical Society,   |c 2014-09-03T19:24:21Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/89161 
520 |a We study the structure of the ground-state wave functions of bosonic symmetry protected topological (SPT) insulators in three space dimensions. We demonstrate that the differences with conventional insulators are captured simply in a dual vortex description. As an example, we show that a previously studied bosonic topological insulator with both global U(1) and time-reversal symmetry can be described by a rather simple wave function written in terms of dual "vortex ribbons." The wave function is a superposition of all the vortex-ribbon configurations of the boson, and a factor (−1) is associated with each self-linking of the vortex ribbons. This wave function can be conveniently derived using an effective field theory of the SPT phase in the strong-coupling limit, and it naturally explains all the phenomena of this SPT phase discussed previously. The ground-state structure for other three-dimensional (3D) bosonic SPT phases are also discussed similarly in terms of vortex loop gas wave functions. We show that our methods reproduce known results on the ground-state structure of some 2D SPT phases. 
520 |a Alfred P. Sloan Foundation 
520 |a David & Lucile Packard Foundation 
520 |a Hellman Family Foundation 
520 |a National Science Foundation (U.S.) (NSF Grant No. DMR-1151208) 
520 |a National Science Foundation (U.S.) (NSF Grant No. DMR-1005434) 
520 |a Simons Foundation (Award No. 229736) 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review B