1985
DOI: 10.1016/0370-2693(85)91415-7
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Propagators and effective potentials in anti-de Sitter space

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Cited by 197 publications
(217 citation statements)
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“…Notice that for ρ * → 0 we obtain 48) while for ρ * → ∞ we have b p → 0 and we recover the formula for a pure CFT.…”
Section: Two-point Function In Ads Slicingsupporting
confidence: 79%
“…Notice that for ρ * → 0 we obtain 48) while for ρ * → ∞ we have b p → 0 and we recover the formula for a pure CFT.…”
Section: Two-point Function In Ads Slicingsupporting
confidence: 79%
“…Integrating this relation over m 2 then determines the effective Lagrangian density [8,9,19,21]. Exactly equivalent results are obtained from mode expansions or using zeta functions [9,14,20,22].…”
Section: Scalar Effective Action In Gravitational Backgroundsmentioning
confidence: 99%
“…Exactly equivalent results are obtained from mode expansions or using zeta functions [9,14,20,22]. The Feynman propagators for massive scalars in AdS d [14,19] and dS d [8] have the forms: Lagrangian density [8,9,19,21], and in higher dimensions this procedure can be taken as a definition of the corresponding effective Lagrangian density. It is clear already from (3.2) and (3.3) that odd and even dimensions are very different.…”
Section: Scalar Effective Action In Gravitational Backgroundsmentioning
confidence: 99%
“…This is indeed the case, as we now check. The bulk AdS Poincaré propagator has the form [74,75], (8.19) where…”
Section: Jhep09(2014)073mentioning
confidence: 99%