2020
DOI: 10.1103/physrevb.102.115154
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Generalized string-net model for unitary fusion categories without tetrahedral symmetry

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Cited by 22 publications
(15 citation statements)
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“…[33] (see Refs. [31,32,[41][42][43] for such generalizations). In both of these classes of models, it is well understood how to find the ground-state degeneracy [13,44] and the properties of the excitations, such as braiding statistics [13,32,33] (as we will elaborate on shortly).…”
mentioning
confidence: 99%
“…[33] (see Refs. [31,32,[41][42][43] for such generalizations). In both of these classes of models, it is well understood how to find the ground-state degeneracy [13,44] and the properties of the excitations, such as braiding statistics [13,32,33] (as we will elaborate on shortly).…”
mentioning
confidence: 99%
“…The matrix elements of this operator are worked out in detail in [1,6]. Every operator B a p is a 18-body operator in the sense that its action explicitly depends on the six string types living on the edges of the plaquette p, the six multiplicities and the six edges adjacent to the plaquette, but acts diagonally on the latter.…”
Section: A Levin and Wen's String-netsmentioning
confidence: 99%
“…Ever since their conception, the string-net models as originally proposed by Levin and Wen [1] and their subsequent generalizations [2][3][4][5][6][7] have provided a rich playground for studying microscopic realisations of non-chiral topologically ordered phases of matter in 2+1 dimensions. Taking a unitary fusion category (UFC) D [8] as input, these exactly solvable models allow for the explicit realization of several key features of topologically ordered systems, such as ground state degeneracies that depend on the topology of the space and anyonic quasi-particle excitations that satisfy non-trivial braiding statistics.…”
Section: Introductionmentioning
confidence: 99%
“…Since we drop the unitary condition, things are sightly different: the Hamiltonian is symmetric (it is easy to see that the matrix element is invariant under the exchange of abc and a b c ) but not Hermitian. However, the spectrum of the Hamiltonian is still entirely real for it is a projector (the possible eigenvalue for a projector is either 1 or 0), which means that B 2 p = B p at each plaquette p. In order to prove it as an projector, we need another relation, called completeness relation in [9]:…”
Section: A String-net Modelmentioning
confidence: 99%