2015
DOI: 10.48550/arxiv.1509.00038
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The classification of subfactors with index at most $5 \frac{1}{4}$

Abstract: Subfactor standard invariants encode quantum symmetries. The small index subfactor classication program has been a rich source of interesting quantum symmetries. We give the complete classi cation of subfactor standard invariants to index 5 1 4 , which includes 3+ √ 5, the rst interesting composite index.Theorem. There are exactly 15 subfactor standard invariants with index in (5, 5 1 4 ], besides the Temperley-Lieb-Jones A ∞ and the reducible A(1)∞ standard invariants at every index. (See Theorem A below.)

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Cited by 11 publications
(22 citation statements)
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“…The standard invariant has been axiomatized in many equivalent ways; in finite depth, we have Ocneanu's paragroups [Ocn88] and Popa's canonical commuting squares [Pop90]. Popa's λ-lattices [Pop95a] give an axiomatization of the standard invariant in the general case, and Jones' equivalent planar algebras [Jon99] provide a powerful graphical calculus for the construction [BMPS12] and classification [JMS14,AMP15] of standard invariants. Using Longo's Q-systems [Lon89], the article [Müg03] re-interprets the standard invariant as a unitary Frobenius algebra object in a rigid C*-tensor category [LR97,Yam04].…”
Section: Introductionmentioning
confidence: 99%
“…The standard invariant has been axiomatized in many equivalent ways; in finite depth, we have Ocneanu's paragroups [Ocn88] and Popa's canonical commuting squares [Pop90]. Popa's λ-lattices [Pop95a] give an axiomatization of the standard invariant in the general case, and Jones' equivalent planar algebras [Jon99] provide a powerful graphical calculus for the construction [BMPS12] and classification [JMS14,AMP15] of standard invariants. Using Longo's Q-systems [Lon89], the article [Müg03] re-interprets the standard invariant as a unitary Frobenius algebra object in a rigid C*-tensor category [LR97,Yam04].…”
Section: Introductionmentioning
confidence: 99%
“…The Haagerup subfactor is the first subfactor that is not directly related to either an ordinary group or a quantum group, and whether its Drinfeld center is related to a quantum group (conformal field theory) or not is an interesting open problem. At the time of writing, the classification of finite depth subfactors is completed up to index 5+1/4 (see [32], [29], [1], and references therein), and it turns out that three subfactors actually exist among Haagerup's list, namely the Haagerup subfactor, Asaeda-Haagerup subfactors constructed in [2], and the extended Haagerup subfactor constructed in [3]. The original construction of the Haagerup subfactor in [2] used computation of connections, a special type of 6j-symbols.…”
Section: Introductionmentioning
confidence: 99%
“…He established a notion of index for subfactors, which is an invariant (hence opened the way to classification questions) and surprisingly quantized for values between 1 and 4 (Jones' rigidity theorem). Since then, the major efforts have been devoted to the study of finite index (finite depth) subfactors and a complete classification has been achieved for subfactors with index at most 5 + 1 4 [JMS14], [AMP15], using techniques of [Pop95a] and [Jon99]. At the same time, the analyses of QFT extensions [LR95] and of theories with defects and boundaries [BKLR16] cover the finite index case only, both being based on the notion of Q-system (which is tightly connected to the existence of conjugate morphisms ῑ of the inclusion morphism ι : N ֒→ M for a subfactor N ⊂ M, hence to the finiteness of the dimension of ι in the sense of [LR97]).…”
Section: Introductionmentioning
confidence: 99%