Search results for "General relativity and quantum cosmology"

showing 10 items of 941 documents

Role of gravity in the pair creation induced by electric fields

2018

We analyze the pair production induced by homogenous, time-dependent electric fields in an expanding space-time background. We point out that, in obtaining the semiclassical Maxwell equations, two distinct notions of adiabatic renormalization are possible. In Minkowski space the two recipes turn out to be equivalent. However, in the presence of gravity only the recipe requiring an adiabatic hierarchy between the gravitational and the gauge field is consistent with the conservation of the energy-momentum tensor.

PhysicsHigh Energy Physics - Theory010308 nuclear & particles physicsSemiclassical physicsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyRenormalizationGravitationsymbols.namesakeClassical mechanicsMaxwell's equationsHigh Energy Physics - Theory (hep-th)0103 physical sciencesMinkowski spacesymbolsTensorGauge theory010306 general physicsAdiabatic process
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Late time approach to Hawking radiation: Terms beyond leading order

2019

Black hole evaporation is studied using wave packets for the modes. These allow for approximate frequency and time resolution. The leading order late time behavior gives the well known Hawking radiation that is independent of how the black hole formed. The focus here is on the higher order terms and the rate at which they damp at late times. Some of these terms carry information about how the black hole formed. A general argument is given which shows that the damping is significantly slower (power law) than what might be naively expected from a stationary phase approximation (exponential). This result is verified by numerical calculations in the cases of 2D and 4D black holes that form from…

PhysicsHigh Energy Physics - Theory010308 nuclear & particles physicsWave packetAstrophysics::High Energy Astrophysical PhenomenaShell (structure)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesNull (physics)Power lawGeneral Relativity and Quantum CosmologyExponential functionBlack holeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Quantum electrodynamics0103 physical sciencesStationary phase approximation010306 general physicsHawking radiation
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Nonsingular Black Holes in $f(R)$ Theories

2015

We study the structure of a family of static, spherically symmetric space-times generated by an anisotropic fluid and governed by a particular type of $f(R)$ theory. We find that for a range of parameters with physical interest, such solutions represent black holes with the central singularity replaced by a finite size wormhole. We show that time-like geodesics and null geodesics with nonzero angular momentum never reach the wormhole throat due to an infinite potential barrier. For null radial geodesics, it takes an infinite affine time to reach the wormhole. This means that the resulting space-time is geodesically complete and, therefore, nonsingular despite the generic existence of curvat…

PhysicsHigh Energy Physics - TheoryAngular momentumGeodesicNull (mathematics)General Physics and AstronomyFOS: Physical sciencesnonsingular black holesGeneral Relativity and Quantum Cosmology (gr-qc)Type (model theory)CurvaturewormholesGeneral Relativity and Quantum Cosmologylaw.inventionGeneral Relativity and Quantum CosmologySingularityInvertible matrixHigh Energy Physics - Theory (hep-th)lawWormholemodified gravityMathematical physics
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Hawking Radiation by Kerr Black Holes and Conformal Symmetry

2010

The exponential blueshift associated with the event horizon of a black hole makes conformal symmetry play a fundamental role in accounting for its thermal properties. Using a derivation based on two-point functions, we show that the full spectrum of thermal radiation of scalar particles by Kerr black holes can be explicitly derived on the basis of a conformal symmetry arising in the wave equation near the horizon. The simplicity of our approach emphasizes the depth of the connection between conformal symmetry and black hole radiance.

PhysicsHigh Energy Physics - TheoryAstrofísicaEvent horizonAstrophysics::High Energy Astrophysical PhenomenaConformal anomalyFOS: Physical sciencesGeneral Physics and AstronomyGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyPartícules (Física nuclear)Black holeMicro black holeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Conformal symmetryQuantum mechanicsExtremal black holeCamps Teoria quàntica deBlack hole thermodynamicsHawking radiation
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Holography, degenerate horizons and entropy

1999

We show that a realization of the correspondence AdS_2/CFT_1 for near extremal Reissner-Nordstrom black holes in arbitrary dimensional Einstein-Maxwell gravity exactly reproduces, via Cardy's formula, the deviation of the Bekenstein-Hawking entropy from extremality. We also show that this mechanism is valid for Schwarzschild-de Sitter black holes around the degenerate solution dS_2xS^n. These results reinforce the idea that the Bekenstein-Hawking entropy can be derived from symmetry principles.

PhysicsHigh Energy Physics - TheoryAstrofísicaNuclear and High Energy PhysicsGravitacióCosmologiaDegenerate energy levelsHolographyFOS: Physical scienceslaw.inventionHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)lawEntropy (arrow of time)Mathematical physics
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Solvable Models for radiating Black Holes and Area-preserving Diffeomorphisms

1995

Solvable theories of 2D dilaton gravity can be obtained from a Liouville theory by suitable field redefinitions. In this paper we propose a new framework to generate 2D dilaton gravity models which can also be exactly solved in the semiclassical approximation. Our approach is based on the recently introduced scheme to quantize massless scalar fields coupled to 2D gravity maintaining invariance under area-preserving diffeomorphisms and Weyl transformations. Starting from the CGHS model with the new effective action we reestablish the full diffeomorphism invariance by means of an adequate family of field redefinitions. The original theory is therefore mapped into a large family of solvable mo…

PhysicsHigh Energy Physics - TheoryAstrofísicaNuclear and High Energy PhysicsGravitacióField (physics)CGHS modelScalar (physics)Semiclassical physicsFOS: Physical sciencessymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)symbolsDilatonDiffeomorphismEinsteinEffective actionMathematical physics
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Backlund transformations in 2-D dilaton gravity

1998

We give a B\"acklund transformation connecting a generic 2D dilaton gravity theory to a generally covariant free field theory. This transformation provides an explicit canonical transformation relating both theories.

PhysicsHigh Energy Physics - TheoryAstrofísicaNuclear and High Energy PhysicsGravity (chemistry)GravitacióGeneral Physics and AstronomyAstronomy and AstrophysicsCanonical transformationFree fieldGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyTransformation (function)Covariant transformationDilatonMathematical physics
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Synchrotron Radiation from the Crab Nebula Discriminates between Models of Space-Time Foam

2003

It has been argued by Jacobson, Liberati and Mattingly that synchrotron radiation from the Crab Nebula imposes a stringent constraint on any modification of the dispersion relations of the electron that might be induced by quantum gravity. We supplement their analysis by deriving the spectrum of synchrotron radiation from the coupling of an electrically-charged particle to an external magnetic fields in the presence of quantum-gravity effects of the general form $(E/M_{QG})^\alpha$. We find that the synchrotron constraint from the Crab Nebula practically excludes $\alpha \lsim 1.74$ for $M_{QG} \sim m_P = 1.2 \times 10^{19}$ GeV. On the other hand, this analysis does not constrain any modif…

PhysicsHigh Energy Physics - TheoryAstrophysics and AstronomyPhotonAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Synchrotron radiationFOS: Physical sciencesAstronomy and AstrophysicsElectronGeneral Relativity and Quantum Cosmology (gr-qc)AstrophysicsSynchrotronGeneral Relativity and Quantum CosmologyComputational physicslaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyCrab NebulaHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)lawDispersion relationQuantum gravityEquivalence principle
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Bimetric Renormalization Group Flows in Quantum Einstein Gravity

2011

The formulation of an exact functional renormalization group equation for Quantum Einstein Gravity necessitates that the underlying effective average action depends on two metrics, a dynamical metric giving the vacuum expectation value of the quantum field, and a background metric supplying the coarse graining scale. The central requirement of "background independence" is met by leaving the background metric completely arbitrary. This bimetric structure entails that the effective average action may contain three classes of interactions: those built from the dynamical metric only, terms which are purely background, and those involving a mixture of both metrics. This work initiates the first …

PhysicsHigh Energy Physics - TheoryBackground field methodAsymptotic safety in quantum gravityGeneral Physics and AstronomyFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Renormalization groupGeneral Relativity and Quantum CosmologyGravitationTheoretical physicsHigh Energy Physics - Theory (hep-th)Functional renormalization groupQuantum gravityBackground independenceEffective action
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Generalized curvature and the equations of D=11 supergravity

2005

It is known that, for zero fermionic sector, the bosonic equations of Cremmer-Julia-Scherk eleven-dimensional supergravity can be collected in a compact expression which is a condition on the curvature of the generalized connection. Here we peresent the equation which collects all the bosonic equations of D=11 supergravity when the gravitino is nonvanishing.

PhysicsHigh Energy Physics - TheoryCondensed Matter::Quantum GasesNuclear and High Energy PhysicsSupergravityHigh Energy Physics::PhenomenologyZero (complex analysis)FOS: Physical sciencesExpression (computer science)CurvatureCovariant derivativeConnection (mathematics)High Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Quantum electrodynamicsGravitinoMathematics::Differential GeometryMathematical physics
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