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Modular discretization of the AdS2/CFT1 Holography
We propose a finite discretization for the black hole geometry and dynamics. We realize our proposal, in the case of extremal black holes, for which the radial and temporal near horizon geometry is known to be AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by replacing...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP02(2014)109 http://cds.cern.ch/record/1557710 |
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author | Axenides, Minos Floratos, E.G. Nicolis, S. |
author_facet | Axenides, Minos Floratos, E.G. Nicolis, S. |
author_sort | Axenides, Minos |
collection | CERN |
description | We propose a finite discretization for the black hole geometry and dynamics. We realize our proposal, in the case of extremal black holes, for which the radial and temporal near horizon geometry is known to be AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by replacing the set of real numbers $\mathbb{R}$ with the set of integers modulo $N$, with AdS$_2$ going over to the finite geometry AdS$_2[N]=SL(2,\mathbb{Z}_N)/SO(1,1,\mathbb{Z}_N)$. We model the dynamics of the microscopic degrees of freedom by generalized Arnol'd cat maps, ${\sf A}\in SL(2,\mathbb{Z}_N)$, which are isometries of the geometry at both the classical and quantum levels. These exhibit well studied properties of strong arithmetic chaos, dynamical entropy, nonlocality and factorization in the cutoff discretization $N$, which are crucial for fast quantum information processing. We construct, finally, a new kind of unitary and holographic correspondence, for AdS$_2[N]$/CFT$_1[N]$, via coherent states of both the bulk and boundary geometries. |
id | cern-1557710 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15577102022-08-10T20:39:55Zdoi:10.1007/JHEP02(2014)109http://cds.cern.ch/record/1557710engAxenides, MinosFloratos, E.G.Nicolis, S.Modular discretization of the AdS2/CFT1 HolographyParticle Physics - TheoryWe propose a finite discretization for the black hole geometry and dynamics. We realize our proposal, in the case of extremal black holes, for which the radial and temporal near horizon geometry is known to be AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by replacing the set of real numbers $\mathbb{R}$ with the set of integers modulo $N$, with AdS$_2$ going over to the finite geometry AdS$_2[N]=SL(2,\mathbb{Z}_N)/SO(1,1,\mathbb{Z}_N)$. We model the dynamics of the microscopic degrees of freedom by generalized Arnol'd cat maps, ${\sf A}\in SL(2,\mathbb{Z}_N)$, which are isometries of the geometry at both the classical and quantum levels. These exhibit well studied properties of strong arithmetic chaos, dynamical entropy, nonlocality and factorization in the cutoff discretization $N$, which are crucial for fast quantum information processing. We construct, finally, a new kind of unitary and holographic correspondence, for AdS$_2[N]$/CFT$_1[N]$, via coherent states of both the bulk and boundary geometries.We propose a finite discretization for the black hole geometry and dynamics. We realize our proposal, in the case of extremal black holes, for which the radial and temporal near horizon geometry is known to be AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by replacing the set of real numbers $\mathbb{R}$ with the set of integers modulo $N$, with AdS$_2$ going over to the finite geometry AdS$_2[N]=SL(2,\mathbb{Z}_N)/SO(1,1,\mathbb{Z}_N)$. We model the dynamics of the microscopic degrees of freedom by generalized Arnol'd cat maps, ${\sf A}\in SL(2,\mathbb{Z}_N)$, which are isometries of the geometry at both the classical and quantum levels. These exhibit well studied properties of strong arithmetic chaos, dynamical entropy, nonlocality and factorization in the cutoff discretization $N$, which are crucial for fast quantum information processing. We construct, finally, a new kind of unitary and holographic correspondence, for AdS$_2[N]$/CFT$_1[N]$, via coherent states of both the bulk and boundary geometries.arXiv:1306.5670CERN-PH-TH-2013-149CERN-PH-TH-2013-149oai:cds.cern.ch:15577102013-06-24 |
spellingShingle | Particle Physics - Theory Axenides, Minos Floratos, E.G. Nicolis, S. Modular discretization of the AdS2/CFT1 Holography |
title | Modular discretization of the AdS2/CFT1 Holography |
title_full | Modular discretization of the AdS2/CFT1 Holography |
title_fullStr | Modular discretization of the AdS2/CFT1 Holography |
title_full_unstemmed | Modular discretization of the AdS2/CFT1 Holography |
title_short | Modular discretization of the AdS2/CFT1 Holography |
title_sort | modular discretization of the ads2/cft1 holography |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1007/JHEP02(2014)109 http://cds.cern.ch/record/1557710 |
work_keys_str_mv | AT axenidesminos modulardiscretizationoftheads2cft1holography AT floratoseg modulardiscretizationoftheads2cft1holography AT nicoliss modulardiscretizationoftheads2cft1holography |