2016
DOI: 10.1007/jhep02(2016)181
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Exact conformal blocks for the W-algebras, twist fields and isomonodromic deformations

Abstract: Abstract:We consider the conformal blocks in the theories with extended conformal W-symmetry for the integer Virasoro central charges. We show that these blocks for the generalized twist fields on sphere can be computed exactly in terms of the free field theory on the covering Riemann surface, even for a non-abelian monodromy group. The generalized twist fields are identified with particular primary fields of the W-algebra, and we propose a straightforward way to compute their W-charges. We demonstrate how the… Show more

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Cited by 12 publications
(20 citation statements)
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“…However, in order to apply bosonization one has to restrict the elements g ∈ N G (h) ⊂ G to the Cartan normalizer, and this will be the key object in our definition of the twist fields. In particular, bosonization means that one considers the space H˙g as a sum of twisted representations of the Heisenberg algebra h. These representations depend not only on the elements g ∈ N G (h), but also on additional data: eigenvalues of the zero modes of the ginvariant part of h. This extra data, below to be called r-charges following [16], has discrete freedom, since only the exponents of such eigenvalues are specified by g. We also denote below the most refined data asg = (g, r).…”
Section: Twisted Representations and Twist-fieldsmentioning
confidence: 99%
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“…However, in order to apply bosonization one has to restrict the elements g ∈ N G (h) ⊂ G to the Cartan normalizer, and this will be the key object in our definition of the twist fields. In particular, bosonization means that one considers the space H˙g as a sum of twisted representations of the Heisenberg algebra h. These representations depend not only on the elements g ∈ N G (h), but also on additional data: eigenvalues of the zero modes of the ginvariant part of h. This extra data, below to be called r-charges following [16], has discrete freedom, since only the exponents of such eigenvalues are specified by g. We also denote below the most refined data asg = (g, r).…”
Section: Twisted Representations and Twist-fieldsmentioning
confidence: 99%
“…These "averaged over a cycle" parameters have been called as r-charges in [16]. Hence, all elements of g ∈ N GL(N ) (h) can be conjugated to the products over the cycles…”
Section: Cartan Normalizersmentioning
confidence: 99%
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