1999
DOI: 10.1016/s0370-2693(99)01260-5
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The Hadamard function and the Feynman propagator in the AdS/CFT correspondence

Abstract: We construct the retarded Green function and the Hadamard function in the Lorentzian (d+1)-dimensional anti-de Sitter spacetime for the Poincaré coordinate by performing the mode integration directly. We explore the structure of singularities for the position-space Feynman propagator derived from them. The boundary scaling limits of the bulk Feynman propagator yield the bulk-boundary propagator and the boundary conformal correlation function with an extra factor.

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Cited by 6 publications
(4 citation statements)
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“…Previous discussion of the Lorentzian signature AdS/CFT appears also in refs. [6,7,8,9]. One boundary condition at the horizon stands out from the physical point of view.…”
Section: Minkowski Ads/cft Prescription 31 Difficulties With Minkowsmentioning
confidence: 99%
“…Previous discussion of the Lorentzian signature AdS/CFT appears also in refs. [6,7,8,9]. One boundary condition at the horizon stands out from the physical point of view.…”
Section: Minkowski Ads/cft Prescription 31 Difficulties With Minkowsmentioning
confidence: 99%
“…Research issues important for various applications of Feynman propagators were discussed in [46]. Note that this paper is among one of the first on that subject.…”
Section: Further Development Of the Approachmentioning
confidence: 99%
“…In this section we take a first look at the computation of the bulk Feynman, retarded and advanced propagators (see also [25] [26]). We concentrate on quantizing the modes Φ ∝ J ν proportional to the Bessel function with positive index ν ≥ 1.…”
Section: Bulk Propagatormentioning
confidence: 99%