2007
DOI: 10.1007/s10485-007-9102-7
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The Fusion Algebra of Bimodule Categories

Abstract: We establish an algebra-isomorphism between the complexified Grothendieck ring F of certain bimodule categories over a modular tensor category and the endomorphism algebra of appropriate morphism spaces of those bimodule categories. This provides a purely categorical proof of a conjecture by Ostrik concerning the structure of F. As a by-product we obtain a concrete expression for the structure constants of the Grothendieck ring of the bimodule category in terms of endomorphisms of the tensor unit of the underl… Show more

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Cited by 25 publications
(32 citation statements)
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References 32 publications
(99 reference statements)
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“…In view of recent development using category theory (cf. [12]), both conjectures can in fact be stated in categorical terms, and we do not know any counter examples in the categorical setting. In Proposition 5.17 we prove that a weaker version of Conjecture 5.12 implies Conjecture 5.1, and from this we are able to prove Conjecture 5.1 for modular tensor category from SU(n) at level k (cf.…”
Section: Introductionmentioning
confidence: 89%
“…In view of recent development using category theory (cf. [12]), both conjectures can in fact be stated in categorical terms, and we do not know any counter examples in the categorical setting. In Proposition 5.17 we prove that a weaker version of Conjecture 5.12 implies Conjecture 5.1, and from this we are able to prove Conjecture 5.1 for modular tensor category from SU(n) at level k (cf.…”
Section: Introductionmentioning
confidence: 89%
“…There is a straightforward generalization when the non-diagonal theory is defined through an automorphism of the fusion rules for the bulk local operators [7]. For blockdiagonal modular invariant theories, the fusion relations of TDLs can be noncommutative (see, for example, [15] for related discussions).…”
Section: Verlinde Lines In Diagonal Rcftsmentioning
confidence: 99%
“…An invariant way to characterize a global symmetry and its 't Hooft anomaly is by the associated (invertible) topological defect lines L [11][12][13][14][15][16][17][18][19][20][21][22][23]. See [24,25] for modern applications of topological defect lines to renormalization group flows and gauging.…”
Section: Topological Defect Lines and Anomaliesmentioning
confidence: 99%
“…To the left of R = √ 2, the bounds become flat, because a gap of (∆ gap ) L = 1 4 can also be interpreted as a gap of any smaller value. 21 To the right of R = 2, the bounds become flat and unsaturated.…”
Section: Some Comments On the Numerical Bounds Shown Inmentioning
confidence: 99%