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Bulletin of the American Physical Society

Bulk-boundary correspondence in (3+1)-dimensional topological phases

Apoorv Tiwari, Xiaohong Chen, Shinsei Ryu

Published Mar 18, 2016• 4 citations
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Bulk-boundary correspondence in (3+1)-dimensional topological phases

Xiao Chen, Apoorv Tiwari, Shinsei Ryu

We discuss (2+1)-dimensional gapless surface theories of bulk (3+1)-dimensional topological phases, such as the BF theory at level $\mathrm{K}$, and its generalization. In particular, we put these theories on a flat (2+1)-dimensional torus ${T}^{3}$ parameterized by its modular parameters, and compute the partition functions obeying various twisted boundary conditions. We show the partition functions are transformed into each other under $SL(3,\mathbb{Z})$ modular transformations, and furthermore establish the bulk-boundary correspondence in (3+1) dimensions by matching the modular $\mathcal{S}$ and $\mathcal{T}$ matrices computed from the boundary field theories with those computed in the bulk. We also propose the three-loop braiding statistics can be studied by constructing the modular $\mathcal{S}$ and $\mathcal{T}$ matrices from an appropriate boundary field theory.

arXiv:1509.04266•Physical review. B./Physical review. B•Jul 13, 2016•76 citations
We discuss (2+1)-dimensional gapless surface theories of bulk (3+1)-dimensional topological phases, such as the BF theory at level K\mathrm{K}K, and its generalization. In particular, we put these theories on a flat (2+1)-dimensional torus T3{T}^{3}T3 parameterized by its modular parameters, and compute the partition functions obeying various twisted boundary conditions. We show the partition functions are transformed into each other under SL(3,Z)SL(3,\mathbb{Z})SL(3,Z) modular transformations, and furthermore establish the bulk-boundary correspondence in (3+1) dimensions by matching the modular S\mathcal{S}S and T\mathcal{T}T matrices computed from the boundary field theories with those computed in the bulk. We also propose the three-loop braiding statistics can be studied by constructing the modular S\mathcal{S}S and T\mathcal{T}T matrices from an appropriate boundary field theory.