Search results for "Nonsingular black hole models"

showing 5 items of 5 documents

Quantum-mechanical model of the Kerr-Newman black hole

2000

We consider a Hamiltonian quantum theory of stationary spacetimes containing a Kerr-Newman black hole. The physical phase space of such spacetimes is just six-dimensional, and it is spanned by the mass $M$, the electric charge $Q$ and angular momentum $J$ of the hole, together with the corresponding canonical momenta. In this six-dimensional phase space we perform a canonical transformation such that the resulting configuration variables describe the dynamical properties of Kerr-Newman black holes in a natural manner. The classical Hamiltonian written in terms of these variables and their conjugate momenta is replaced by the corresponding self-adjoint Hamiltonian operator and an eigenvalue …

PhysicsNuclear and High Energy PhysicsWhite holeFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)FuzzballGeneral Relativity and Quantum CosmologyBlack holeGeneral Relativity and Quantum CosmologyRotating black holeNonsingular black hole modelsQuantum mechanicsExtremal black holeBlack hole thermodynamicsHawking radiation
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How singular are black hole interiors?

1991

Abstract Ori has recently shown that an astronaut approaching the inner horizon of a black hole is not necessarily torn apart by tidal forces. This raises anew the possibility of astronavigation through black holes, perhaps to other universes. We re-examine this question in the light of hypotheses about probable conditions in the black hole core.

PhysicsGeneral relativityAstrophysics::High Energy Astrophysical PhenomenaWhite holeHorizonGeneral Physics and AstronomyAstrophysicsFuzzballPhysics::GeophysicsBlack holeGeneral Relativity and Quantum Cosmologyde Sitter–Schwarzschild metricNonsingular black hole modelsTidal forcePhysics Letters A
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Evaporation of Near-Extremal Reissner-Nordström Black Holes

2000

The formation of near-extremal Reissner-Nordstrom black holes in the S-wave approximation can be described, near the event horizon, by an effective solvable model. The corresponding one-loop quantum theory remains solvable and allows to follow analytically the evaporation process which is shown to require an infinite amount of time.

AstrofísicaHigh Energy Physics - TheoryPhysicsEvent horizonMembrane paradigmAstronomyAstronomical PhenomenaEvaporationFOS: Physical sciencesGeneral Physics and AstronomyGeneral Relativity and Quantum Cosmology (gr-qc)Models TheoreticalFuzzballGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyTheoretical physicsHigh Energy Physics - Theory (hep-th)Nonsingular black hole modelsAstronomiaCamps Teoria quàntica deBlack hole thermodynamicsMathematical physicsPhysical Review Letters
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Trapping Horizons as inner boundary conditions for black hole spacetimes

2007

We present a set of inner boundary conditions for the numerical construction of dynamical black hole space-times, when employing a 3+1 constrained evolution scheme and an excision technique. These inner boundary conditions are heuristically motivated by the dynamical trapping horizon framework and are enforced in an elliptic subsystem of the full Einstein equation. In the stationary limit they reduce to existing isolated horizon boundary conditions. A characteristic analysis completes the discussion of inner boundary conditions for the radiative modes.

PhysicsNuclear and High Energy PhysicsEvent horizonWhite holeBoundary conformal field theoryFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyClassical mechanicsRotating black holeNonsingular black hole modelsExtremal black holeFree boundary problemBoundary value problem
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Regular black hole metrics and the weak energy condition

2014

In this work we construct a family of spherically symmetric, static, charged regular black hole metrics in the context of Einstein-nonlinear electrodynamics theory. The construction of the charged regular black hole metrics is based on three requirements: (a) the weak energy condition should be satisfied, (b) the energy-momentum tensor should have the symmetry $T^{0}_{0}=T^{1}_{1}$, and (c) these metrics have to asymptotically behave as the Reissner-Nordstr\"{o}m black hole metric. In addition, these charged regular black hole metrics depend on two parameters which for specific values yield regular black hole metrics that already exist in the literature. Furthermore, by relaxing the third r…

PhysicsNuclear and High Energy PhysicsWhite holeAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyBlack hole electronBlack holeTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanicsde Sitter–Schwarzschild metricNonsingular black hole modelsExtremal black holeBlack braneEnergy conditionPhysics Letters B
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