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Black Hole Astrophysics in AdS Braneworlds

We consider astrophysics of large black holes localized on the brane in the infinite Randall-Sundrum model. Using their description in terms of a conformal field theory (CFT) coupled to gravity, deduced in Ref. [1], we show that they undergo a period of rapid decay via Hawking radiation of CFT modes...

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Autores principales: Emparan, Roberto, Garcia-Bellido, Juan, Kaloper, Nemanja
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2003/01/079
http://cds.cern.ch/record/596231
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author Emparan, Roberto
Garcia-Bellido, Juan
Kaloper, Nemanja
author_facet Emparan, Roberto
Garcia-Bellido, Juan
Kaloper, Nemanja
author_sort Emparan, Roberto
collection CERN
description We consider astrophysics of large black holes localized on the brane in the infinite Randall-Sundrum model. Using their description in terms of a conformal field theory (CFT) coupled to gravity, deduced in Ref. [1], we show that they undergo a period of rapid decay via Hawking radiation of CFT modes. For example, a black hole of mass ${\rm few} \times M_\odot$ would shed most of its mass in $\sim 10^4 - 10^5$ years if the AdS radius is $L \sim 10^{-1}$ mm, currently the upper bound from table-top experiments. Since this is within the mass range of X-ray binary systems containing a black hole, the evaporation enhanced by the hidden sector CFT modes could cause the disappearance of X-ray sources on the sky. This would be a striking signature of RS2 with a large AdS radius. Alternatively, for shorter AdS radii, the evaporation would be slower. In such cases, the persistence of X-ray binaries with black holes already implies an upper bound on the AdS radius of $L \la 10^{-2}$ mm, an order of magnitude better than the bounds from table-top experiments. The observation of primordial black holes with a mass in the MACHO range $M \sim 0.1 - 0.5 M_\odot$ and an age comparable to the age of the universe would further strengthen the bound on the AdS radius to $L \la {\rm few} \times 10^{-6} $ mm.
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spelling cern-5962312023-03-14T20:20:40Zdoi:10.1088/1126-6708/2003/01/079http://cds.cern.ch/record/596231engEmparan, RobertoGarcia-Bellido, JuanKaloper, NemanjaBlack Hole Astrophysics in AdS BraneworldsParticle Physics - TheoryWe consider astrophysics of large black holes localized on the brane in the infinite Randall-Sundrum model. Using their description in terms of a conformal field theory (CFT) coupled to gravity, deduced in Ref. [1], we show that they undergo a period of rapid decay via Hawking radiation of CFT modes. For example, a black hole of mass ${\rm few} \times M_\odot$ would shed most of its mass in $\sim 10^4 - 10^5$ years if the AdS radius is $L \sim 10^{-1}$ mm, currently the upper bound from table-top experiments. Since this is within the mass range of X-ray binary systems containing a black hole, the evaporation enhanced by the hidden sector CFT modes could cause the disappearance of X-ray sources on the sky. This would be a striking signature of RS2 with a large AdS radius. Alternatively, for shorter AdS radii, the evaporation would be slower. In such cases, the persistence of X-ray binaries with black holes already implies an upper bound on the AdS radius of $L \la 10^{-2}$ mm, an order of magnitude better than the bounds from table-top experiments. The observation of primordial black holes with a mass in the MACHO range $M \sim 0.1 - 0.5 M_\odot$ and an age comparable to the age of the universe would further strengthen the bound on the AdS radius to $L \la {\rm few} \times 10^{-6} $ mm.We consider astrophysics of large black holes localized on the brane in the infinite Randall-Sundrum model. Using their description in terms of a conformal field theory (CFT) coupled to gravity, deduced in Ref. [1], we show that they undergo a period of rapid decay via Hawking radiation of CFT modes. For example, a black hole of mass ${\rm few} \times M_\odot$ would shed most of its mass in $\sim 10^4 - 10^5$ years if the AdS radius is $L \sim 10^{-1}$ mm, currently the upper bound from table-top experiments. Since this is within the mass range of X-ray binary systems containing a black hole, the evaporation enhanced by the hidden sector CFT modes could cause the disappearance of X-ray sources on the sky. This would be a striking signature of RS2 with a large AdS radius. Alternatively, for shorter AdS radii, the evaporation would be slower. In such cases, the persistence of X-ray binaries with black holes already implies an upper bound on the AdS radius of $L \la 10^{-2}$ mm, an order of magnitude better than the bounds from table-top experiments. The observation of primordial black holes with a mass in the MACHO range $M \sim 0.1 - 0.5 M_\odot$ and an age comparable to the age of the universe would further strengthen the bound on the AdS radius to $L \la {\rm few} \times 10^{-6} $ mm.hep-th/0212132IFT-UAM-CSIC-02-56IFT-UAM-CSIC-2002-56oai:cds.cern.ch:5962312002-12-11
spellingShingle Particle Physics - Theory
Emparan, Roberto
Garcia-Bellido, Juan
Kaloper, Nemanja
Black Hole Astrophysics in AdS Braneworlds
title Black Hole Astrophysics in AdS Braneworlds
title_full Black Hole Astrophysics in AdS Braneworlds
title_fullStr Black Hole Astrophysics in AdS Braneworlds
title_full_unstemmed Black Hole Astrophysics in AdS Braneworlds
title_short Black Hole Astrophysics in AdS Braneworlds
title_sort black hole astrophysics in ads braneworlds
topic Particle Physics - Theory
url https://dx.doi.org/10.1088/1126-6708/2003/01/079
http://cds.cern.ch/record/596231
work_keys_str_mv AT emparanroberto blackholeastrophysicsinadsbraneworlds
AT garciabellidojuan blackholeastrophysicsinadsbraneworlds
AT kalopernemanja blackholeastrophysicsinadsbraneworlds