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On a Canonical Quantization of 3D Anti de Sitter Pure Gravity

We perform a canonical quantization of pure gravity on AdS3 using as a technical tool its equivalence at the classical level with a Chern-Simons theory with gauge group SL(2,R)xSL(2,R). We first quantize the theory canonically on an asymptotically AdS space --which is topologically the real line tim...

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Detalles Bibliográficos
Autores principales: Kim, Jihun, Porrati, Massimo
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP10(2015)096
http://cds.cern.ch/record/2045167
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author Kim, Jihun
Porrati, Massimo
author_facet Kim, Jihun
Porrati, Massimo
author_sort Kim, Jihun
collection CERN
description We perform a canonical quantization of pure gravity on AdS3 using as a technical tool its equivalence at the classical level with a Chern-Simons theory with gauge group SL(2,R)xSL(2,R). We first quantize the theory canonically on an asymptotically AdS space --which is topologically the real line times a Riemann surface with one connected boundary. Using the "constrain first" approach we reduce canonical quantization to quantization of orbits of the Virasoro group and Kaehler quantization of Teichmuller space. After explicitly computing the Kaehler form for the torus with one boundary component and after extending that result to higher genus, we recover known results, such as that wave functions of SL(2,R) Chern-Simons theory are conformal blocks. We find new restrictions on the Hilbert space of pure gravity by imposing invariance under large diffeomorphisms and normalizability of the wave function. The Hilbert space of pure gravity is shown to be the target space of Conformal Field Theories with continuous spectrum and a lower bound on operator dimensions. A projection defined by topology changing amplitudes in Euclidean gravity is proposed. It defines an invariant subspace that allows for a dual interpretation in terms of a Liouville CFT. Problems and features of the CFT dual are assessed and a new definition of the Hilbert space, exempt from those problems, is proposed in the case of highly-curved AdS3.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-20451672023-10-04T07:45:56Zdoi:10.1007/JHEP10(2015)096http://cds.cern.ch/record/2045167engKim, JihunPorrati, MassimoOn a Canonical Quantization of 3D Anti de Sitter Pure GravityParticle Physics - TheoryWe perform a canonical quantization of pure gravity on AdS3 using as a technical tool its equivalence at the classical level with a Chern-Simons theory with gauge group SL(2,R)xSL(2,R). We first quantize the theory canonically on an asymptotically AdS space --which is topologically the real line times a Riemann surface with one connected boundary. Using the "constrain first" approach we reduce canonical quantization to quantization of orbits of the Virasoro group and Kaehler quantization of Teichmuller space. After explicitly computing the Kaehler form for the torus with one boundary component and after extending that result to higher genus, we recover known results, such as that wave functions of SL(2,R) Chern-Simons theory are conformal blocks. We find new restrictions on the Hilbert space of pure gravity by imposing invariance under large diffeomorphisms and normalizability of the wave function. The Hilbert space of pure gravity is shown to be the target space of Conformal Field Theories with continuous spectrum and a lower bound on operator dimensions. A projection defined by topology changing amplitudes in Euclidean gravity is proposed. It defines an invariant subspace that allows for a dual interpretation in terms of a Liouville CFT. Problems and features of the CFT dual are assessed and a new definition of the Hilbert space, exempt from those problems, is proposed in the case of highly-curved AdS3.We perform a canonical quantization of pure gravity on AdS$_{3}$ using as a technical tool its equivalence at the classical level with a Chern-Simons theory with gauge group $ \mathrm{S}\mathrm{L}\left(2,\mathbb{R}\right)\times \mathrm{S}\mathrm{L}\left(2,\mathbb{R}\right) $ . We first quantize the theory canonically on an asymptotically AdS space -which is topologically the real line times a Riemann surface with one connected boundary. Using the “constrain first” approach we reduce canonical quantization to quantization of orbits of the Virasoro group and Kähler quantization of Teichmüller space. After explicitly computing the Kähler form for the torus with one boundary component and after extending that result to higher genus, we recover known results, such as that wave functions of $ \mathrm{S}\mathrm{L}\left(2,\mathbb{R}\right) $ Chern-Simons theory are conformal blocks. We find new restrictions on the Hilbert space of pure gravity by imposing invariance under large diffeomorphisms and normalizability of the wave function. The Hilbert space of pure gravity is shown to be the target space of Conformal Field Theories with continuous spectrum and a lower bound on operator dimensions. A projection defined by topology changing amplitudes in Euclidean gravity is proposed. It defines an invariant subspace that allows for a dual interpretation in terms of a Liouville CFT. Problems and features of the CFT dual are assessed and a new definition of the Hilbert space, exempt from those problems, is proposed in the case of highly-curved AdS$_{3}$.We perform a canonical quantization of pure gravity on AdS3 using as a technical tool its equivalence at the classical level with a Chern-Simons theory with gauge group SL(2,R)xSL(2,R). We first quantize the theory canonically on an asymptotically AdS space --which is topologically the real line times a Riemann surface with one connected boundary. Using the "constrain first" approach we reduce canonical quantization to quantization of orbits of the Virasoro group and Kaehler quantization of Teichmuller space. After explicitly computing the Kaehler form for the torus with one boundary component and after extending that result to higher genus, we recover known results, such as that wave functions of SL(2,R) Chern-Simons theory are conformal blocks. We find new restrictions on the Hilbert space of pure gravity by imposing invariance under large diffeomorphisms and normalizability of the wave function. The Hilbert space of pure gravity is shown to be the target space of Conformal Field Theories with continuous spectrum and a lower bound on operator dimensions. A projection defined by topology changing amplitudes in Euclidean gravity is proposed. It defines an invariant subspace that allows for a dual interpretation in terms of a Liouville CFT. Problems and features of the CFT dual are assessed and a new definition of the Hilbert space, exempt from those problems, is proposed in the case of highly-curved AdS3.arXiv:1508.03638CERN-PH-TH-2015-188CERN-PH-TH-2015-188oai:cds.cern.ch:20451672015-08-14
spellingShingle Particle Physics - Theory
Kim, Jihun
Porrati, Massimo
On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title_full On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title_fullStr On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title_full_unstemmed On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title_short On a Canonical Quantization of 3D Anti de Sitter Pure Gravity
title_sort on a canonical quantization of 3d anti de sitter pure gravity
topic Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP10(2015)096
http://cds.cern.ch/record/2045167
work_keys_str_mv AT kimjihun onacanonicalquantizationof3dantidesitterpuregravity
AT porratimassimo onacanonicalquantizationof3dantidesitterpuregravity