2003
DOI: 10.1103/physrevd.68.125012
|View full text |Cite
|
Sign up to set email alerts
|

Systematics of coupling flows in AdS backgrounds

Abstract: We give an effective field theory derivation, based on the running of Planck brane gauge correlators, of the large logarithms that arise in the predictions for low energy gauge couplings in compactified AdS 5 backgrounds, including the one-loop effects of bulk scalars, fermions, and gauge bosons. In contrast to the case of charged scalars coupled to Abelian gauge fields that has been considered previously in the literature, the one-loop corrections are not dominated by a single 4D Kaluza-Klein mode. Neverthele… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
120
0

Year Published

2003
2003
2018
2018

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 59 publications
(122 citation statements)
references
References 38 publications
2
120
0
Order By: Relevance
“…However, if the object has a non-vanishing quadrupole moment Q ij then there is a logarithmic divergence that requires a counterterm operator of the form dτQ ij R µiνj v µ v ν , leading to classical renormalization group logarithms in physical observables [7]. For instance, the composite object obtained by integrating out the orbital scale r in the black hole binary has a Q ij = 0, and so one expects, by the power counting of the EFT, terms of the form v 6 log v relative to the leading order quadrupole power loss which are calculable by renormalization group methods [8]. A typical Feynman diagram that contributes to the renormalization group equations at order v 6 is given in Fig.…”
Section: Einstein-hilbert Term the Functional Integration Is Performmentioning
confidence: 99%
“…However, if the object has a non-vanishing quadrupole moment Q ij then there is a logarithmic divergence that requires a counterterm operator of the form dτQ ij R µiνj v µ v ν , leading to classical renormalization group logarithms in physical observables [7]. For instance, the composite object obtained by integrating out the orbital scale r in the black hole binary has a Q ij = 0, and so one expects, by the power counting of the EFT, terms of the form v 6 log v relative to the leading order quadrupole power loss which are calculable by renormalization group methods [8]. A typical Feynman diagram that contributes to the renormalization group equations at order v 6 is given in Fig.…”
Section: Einstein-hilbert Term the Functional Integration Is Performmentioning
confidence: 99%
“…In the absence of localized kinetic terms, the matter-independent term in the effective Kähler potential is known from refs. [53,54] (see also [55,56,57] )and has the form ∆Ω eff ≃ c w /(4π 2 ) z 2 0 z −4 1 , where c w ≃ 1.165. Applying the shift, we find…”
Section: Strongly Warped Casementioning
confidence: 99%
“…An effective field theory approach to gauge coupling evolution in AdS, based on gauge theory correlators whose external points are on the Planck brane, was obtained in Ref. [12]. Different methods of computing radiative corrections to the low-energy zero-mode gauge couplings were adopted in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…The issue of gauge coupling evolution in the AdS background has also been discussed recently in Refs. [15,16,17], and analyzed using deconstruction in [18]. However, a fully realistic theory of grand unification in AdS has not been constructed.…”
Section: Introductionmentioning
confidence: 99%