Boundary-to-bulk maps for AdS causal wedges and RG flow

Abstract We consider the problem of defining spacelike-supported boundary-to-bulk propagators in AdS d+1 down to the unitary bound ∆ = (d − 2)/2. That is to say, we construct the ‘smearing functions’ K of HKLL but with different boundary conditions where both dimensions ∆+ and ∆ − are taken into acc...

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Main Authors: Nicolás Del Grosso, Alan Garbarz, Gabriel Palau, Guillem Pérez-Nadal
Format: Article
Language:English
Published: SpringerOpen 2019-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP10(2019)135
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spelling doaj-27bb71a9f2f044edaaa8fedfa7e2ab062020-11-25T03:55:46ZengSpringerOpenJournal of High Energy Physics1029-84792019-10-0120191012910.1007/JHEP10(2019)135Boundary-to-bulk maps for AdS causal wedges and RG flowNicolás Del Grosso0Alan Garbarz1Gabriel Palau2Guillem Pérez-Nadal3Physics Department, University of Buenos AiresPhysics Department, University of Buenos AiresPhysics Department, University of Buenos AiresPhysics Department, University of Buenos AiresAbstract We consider the problem of defining spacelike-supported boundary-to-bulk propagators in AdS d+1 down to the unitary bound ∆ = (d − 2)/2. That is to say, we construct the ‘smearing functions’ K of HKLL but with different boundary conditions where both dimensions ∆+ and ∆ − are taken into account. More precisely, we impose Robin boundary conditions, which interpolate between Dirichlet and Neumann boundary conditions and we give explicit expressions for the distributional kernel K with spacelike support. This flow between boundary conditions is known to be captured in the boundary by adding a double-trace deformation to the CFT. Indeed, we explicitly show that using K there is a consistent and explicit map from a Wightman function of the boundary QFT to a Wightman function of the bulk theory. In order to accomplish this we have to study first the microlocal properties of the boundary two-point function of the perturbed CFT and prove its wavefront set satisfies the microlocal spectrum condition. This permits to assert that K and the boundary two-point function can be multiplied as distributions.http://link.springer.com/article/10.1007/JHEP10(2019)135AdS-CFT CorrespondenceRenormalization GroupConformal Field Theory
collection DOAJ
language English
format Article
sources DOAJ
author Nicolás Del Grosso
Alan Garbarz
Gabriel Palau
Guillem Pérez-Nadal
spellingShingle Nicolás Del Grosso
Alan Garbarz
Gabriel Palau
Guillem Pérez-Nadal
Boundary-to-bulk maps for AdS causal wedges and RG flow
Journal of High Energy Physics
AdS-CFT Correspondence
Renormalization Group
Conformal Field Theory
author_facet Nicolás Del Grosso
Alan Garbarz
Gabriel Palau
Guillem Pérez-Nadal
author_sort Nicolás Del Grosso
title Boundary-to-bulk maps for AdS causal wedges and RG flow
title_short Boundary-to-bulk maps for AdS causal wedges and RG flow
title_full Boundary-to-bulk maps for AdS causal wedges and RG flow
title_fullStr Boundary-to-bulk maps for AdS causal wedges and RG flow
title_full_unstemmed Boundary-to-bulk maps for AdS causal wedges and RG flow
title_sort boundary-to-bulk maps for ads causal wedges and rg flow
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-10-01
description Abstract We consider the problem of defining spacelike-supported boundary-to-bulk propagators in AdS d+1 down to the unitary bound ∆ = (d − 2)/2. That is to say, we construct the ‘smearing functions’ K of HKLL but with different boundary conditions where both dimensions ∆+ and ∆ − are taken into account. More precisely, we impose Robin boundary conditions, which interpolate between Dirichlet and Neumann boundary conditions and we give explicit expressions for the distributional kernel K with spacelike support. This flow between boundary conditions is known to be captured in the boundary by adding a double-trace deformation to the CFT. Indeed, we explicitly show that using K there is a consistent and explicit map from a Wightman function of the boundary QFT to a Wightman function of the bulk theory. In order to accomplish this we have to study first the microlocal properties of the boundary two-point function of the perturbed CFT and prove its wavefront set satisfies the microlocal spectrum condition. This permits to assert that K and the boundary two-point function can be multiplied as distributions.
topic AdS-CFT Correspondence
Renormalization Group
Conformal Field Theory
url http://link.springer.com/article/10.1007/JHEP10(2019)135
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AT alangarbarz boundarytobulkmapsforadscausalwedgesandrgflow
AT gabrielpalau boundarytobulkmapsforadscausalwedgesandrgflow
AT guillempereznadal boundarytobulkmapsforadscausalwedgesandrgflow
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