Self-dual Quantum Electrodynamics as Boundary State of the three dimensional Bosonic Topological Insulator
arXiv:1510.06032 · doi:10.1103/PhysRevB.92.220416
Abstract
Inspired by the recent developments of constructing novel Dirac liquid boundary states of the topological insulator, we propose one possible boundary state of the bosonic symmetry protected topological state with symmetry. This boundary theory is described by a quantum electrodynamics (QED) with two flavors of Dirac fermions () coupled with a noncompact U(1) gauge field: , where is the internal noncompact U(1) gauge field, and are two external gauge fields that couple to and global symmetries respectively. We demonstrate that this theory has a "self-dual" structure, which is a fermionic analogue of the self-duality of the noncompact CP theory with easy plane anisotropy. Under the self-duality, the boundary action takes exactly the same form except for an exchange between and . The self-duality may still hold after we break one of the U(1) symmetries (which makes the system a bosonic topological insulator), with some subtleties that will be discussed.
5 pages
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