2021
DOI: 10.1007/jhep05(2021)007
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Defect conformal blocks from Appell functions

Abstract: We develop a group theoretical formalism to study correlation functions in defect conformal field theory, with multiple insertions of bulk and defect fields. This formalism is applied to construct the defect conformal blocks for three-point functions of scalar fields. Starting from a configuration with one bulk and one defect field, for which the correlation function is determined by conformal symmetry, we explore two possibilities, adding either one additional defect or bulk field. In both cases it is possibl… Show more

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Cited by 11 publications
(18 citation statements)
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“…Finally, the study of higher-point functions is one of the long-term goals of the bootstrap. Progress in this direction was made in [54], where higher-point functions in the presence of defects were studied. Eventually, one should be able to obtain the corresponding Lorentzian inversion formulas, and implement the multi-point bootstrap in order to obtain even more restrictive constraints.…”
Section: Discussionmentioning
confidence: 99%
“…Finally, the study of higher-point functions is one of the long-term goals of the bootstrap. Progress in this direction was made in [54], where higher-point functions in the presence of defects were studied. Eventually, one should be able to obtain the corresponding Lorentzian inversion formulas, and implement the multi-point bootstrap in order to obtain even more restrictive constraints.…”
Section: Discussionmentioning
confidence: 99%
“…Finally, the study of higher-point functions is one of the long-term goals of the bootstrap. Progress in this direction was made in [56], where higher-point functions in the presence of defects were studied. Eventually, one should be able to obtain the corresponding Lorentzian inversion formulas, and implement the multi-point bootstrap in order to obtain even more restrictive constraints.…”
Section: Jhep05(2022)185mentioning
confidence: 99%
“…The prefactor Ξ is constructed in section 4.1.1 below, using ideas and constructions from [20] and [31], properly extended to spinning bulk fields. The final formula is stated in eq.…”
Section: Jhep03(2023)133mentioning
confidence: 99%
“…The invariant X that appears in the argument of the special function ψ is simply X = A z 2 A . Once again the prefactor Ξ is constructed explicitly, see section 4.2.1, using ideas and constructions from [20] and [31]. The final formula is stated in eq.…”
Section: Guide To Bulk Channel Blocksmentioning
confidence: 99%