2018
DOI: 10.1007/s00220-018-3274-x
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Rigid Fuchsian Systems in 2-Dimensional Conformal Field Theories

Abstract: We investigate Fuchsian equations arising in the context of 2-dimensional conformal field theory (CFT) and we apply the Katz theory of Fucshian rigid systems to solve some of these equations. We show that the Katz theory provides a precise mathematical framework to answer the question whether the fusion rules of degenerate primary fields are enough for determining the differential equations satisfied by their correlation functions. We focus on the case of W 3 Toda CFT: we argue that the differential equations … Show more

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Cited by 8 publications
(6 citation statements)
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“…We will determine our block by solving a third-order BPZ differential equation. Rather than a direct derivation from the singular vector, we will use knowledge of the fusion rules for deriving this equation, in the spirit of [26]. The fusion rules determine the characteristic exponents of our Fuchsian differential equation at each one of the three singularities z = 0, 1, ∞.…”
Section: (42)mentioning
confidence: 99%
“…We will determine our block by solving a third-order BPZ differential equation. Rather than a direct derivation from the singular vector, we will use knowledge of the fusion rules for deriving this equation, in the spirit of [26]. The fusion rules determine the characteristic exponents of our Fuchsian differential equation at each one of the three singularities z = 0, 1, ∞.…”
Section: (42)mentioning
confidence: 99%
“…The properties of semi-degenerate W Nconformal blocks describing correlation functions of the Toda CFT and their gauge theory counterparts have been studied, for instance, in [33,16]. An interesting direction which is in a sense close to ours is the construction of integral representation of the 4-point conformal blocks of W 3 -algebra involving one semi-degenerate field of higher level (whose matrix elements cannot be reduced to primary ones only) and one fundamental degenerate field [4]. This construction is based on the middle convolution from the Katz theory of rigid systems.…”
Section: Introductionmentioning
confidence: 99%
“…We could not determine the constant α. Analogously to the determination of β, see (3.8), this requires to find the connection of a Fuchsian system. However, differently from the case N = 3, for N ≥ 4 this is a non-rigid rank 3 Fuchsian system and finding the connection of this system is a very hard problem, see the discussion in [29]. We let α undetermined and we use it as a fit parameter in the comparison with Monte-Carlo results.…”
Section: N (X) Gmentioning
confidence: 99%