2017
DOI: 10.48550/arxiv.1711.07982
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Symmetry-enriched topological order in tensor networks: Defects, gauging and anyon condensation

Abstract: We study symmetry-enriched topological order in two-dimensional tensor network states by using graded matrix product operator algebras to represent symmetry induced domain walls. A close connection to the theory of graded unitary fusion categories is established. Tensor network representations of the topological defect superselection sectors are constructed for all domain walls. The emergent symmetry-enriched topological order is extracted from these representations, including the symmetry action on the underl… Show more

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Cited by 42 publications
(80 citation statements)
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“…Mathematically, this is guaranteed by the fact that the fusion categories D and C are Morita equivalent; the sectors are given by the monoidal centers of these fusion categories, which are equivalent for Morita equivalent fusion categories [22]. At the level of the MPO symmetries, the monoidal center can be constructed from the tube algebra [14,66], the central idempotents of which correspond to the different sectors in the model. The dimension of these central idempotents is in general different for the two models, which is reflected in the difference in Hilbert space dimension.…”
Section: Iid Bond Algebras and Dualitymentioning
confidence: 99%
“…Mathematically, this is guaranteed by the fact that the fusion categories D and C are Morita equivalent; the sectors are given by the monoidal centers of these fusion categories, which are equivalent for Morita equivalent fusion categories [22]. At the level of the MPO symmetries, the monoidal center can be constructed from the tube algebra [14,66], the central idempotents of which correspond to the different sectors in the model. The dimension of these central idempotents is in general different for the two models, which is reflected in the difference in Hilbert space dimension.…”
Section: Iid Bond Algebras and Dualitymentioning
confidence: 99%
“…where |P i is anyon basis. Explicit wave-functions for unitary models based on a tensor network have been constructed explicitly [18][19][20][21][22][23][24]. We would like to adapt these methods to construct left/right anyon basis in the non-Hermitian model.…”
Section: Modular S T Matrix For Non-hermitian Galois Conjugate String...mentioning
confidence: 99%
“…The multiplication of the basis elements e i := A abcd defines some algebra, from which we find both central and simple idempotents as desrcibed in Appendix B. The algebra of A abcd can be used to calculate the action of the Dehn twist on a state with a symmetry Z a along the torus 73 :…”
Section: S and T Matrices From F Symbolsmentioning
confidence: 99%
“…The T was is given in eq.59 and the basis change B is given by the combination of F-symbols, as shown in 73 : For non-Abelian anyon models, the inversion P −1 for 2 or more dimensional idempotents actually means the sum of inverted simple idempotents. Unlike the matrix of central idempotent, the matrix of simple idempotents P simple in most cases is square and invertible.…”
Section: S and T Matrices From F Symbolsmentioning
confidence: 99%
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