Search results for "General relativity and quantum cosmology"

showing 10 items of 941 documents

RG flows of Quantum Einstein Gravity in the linear-geometric approximation

2014

We construct a novel Wetterich-type functional renormalization group equation for gravity which encodes the gravitational degrees of freedom in terms of gauge-invariant fluctuation fields. Applying a linear-geometric approximation the structure of the new flow equation is considerably simpler than the standard Quantum Einstein Gravity construction since only transverse-traceless and trace part of the metric fluctuations propagate in loops. The geometric flow reproduces the phase-diagram of the Einstein-Hilbert truncation including the non-Gaussian fixed point essential for Asymptotic Safety. Extending the analysis to the polynomial $f(R)$-approximation establishes that this fixed point come…

PhysicsHigh Energy Physics - Theory; High Energy Physics - Theory; General Relativity and Quantum CosmologyHigh Energy Physics - TheoryEntropic gravityGeneral relativityAsymptotic safety in quantum gravityGeneral Physics and AstronomyFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Euclidean quantum gravityGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyClassical mechanicsHigh Energy Physics - Theory (hep-th)Linearized gravityTheoretical High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGQuantum gravitySemiclassical gravityf(R) gravityAnnals of Physics
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Remarks on the reduced phase space of -dimensional gravity on a torus in the Ashtekar formulation

1998

We examine the reduced phase space of the Barbero-Varadarajan solutions of the Ashtekar formulation of (2 + 1)-dimensional general relativity on a torus. We show that it is a finite-dimensional space due to the existence of an infinite-dimensional residual gauge invariance which reduces the infinite-dimensional space of solutions to a finite-dimensional space of gauge-inequivalent solutions. This is in agreement with general arguments which imply that the number of physical degrees of freedom for (2 + 1)-dimensional Ashtekar gravity on a torus is finite.

PhysicsHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyGravity (chemistry)Physics and Astronomy (miscellaneous)General relativityPhase spaceDegrees of freedom (physics and chemistry)TorusGauge theorySpace (mathematics)ResidualMathematical physicsClassical and Quantum Gravity
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Phase space coordinates and the Hamiltonian constraint of Regge calculus.

1994

We suggest that the phase space of Regge calculus is spanned by the areas and the deficit angles corresponding to the two-simplexes on the spacelike hypersurface of simplicial spacetime. Our proposal is based on a slight modification of the Ashtekar formulation of canonical gravity. In terms of these phase space coordinates we write an equation which we suggest to be a simplicial version of the Hamiltonian constraint of canonical gravity.

PhysicsHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHypersurfaceClassical mechanicsHamiltonian constraintSpacetimeGeneral relativityPhase spaceSpace timeRegge calculusCovariant Hamiltonian field theoryMathematical physicsPhysical review. D, Particles and fields
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High Resolution and Broad Band Spectra of Low Mass X-ray Binaries: A Comparison between Black Holes and Neutron Stars

2005

A common question about compact objects in high energy astrophysics is whether it is possible to distinguish black hole from neutron star systems with some other property that is not the mass of the compact object. Up to now a few characteristics have been found which are typical of neutron stars (like quasi periodic oscillations at kHz frequencies or type-I X-ray bursts), but in many respects black hole and neutron star systems show very similar behaviors. We present here a spectral study of low mass X-ray binaries containing neutron stars and show that these systems have spectral characteristics that are very similar to what is found for black hole systems. This implies that it is unlikel…

PhysicsHigh-energy astronomyAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)X-rayFOS: Physical sciencesBroad bandAstronomy and AstrophysicsAstrophysicsindividual : Sco X-1 4U 1705-44; stars : neutron; X-rays : stars; X-rays : binaries; X-rays : general [accretion accretion disks; stars]Compact staraccretion accretion diskAstrophysicsstars : neutronSpectral lineBlack holeNeutron starGeneral Relativity and Quantum Cosmologystars : individual : Sco X-1 4U 1705-44Space and Planetary ScienceX-rays : starX-rays : binarieLow MassX-rays : general
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Dynamical spacetimes and gravitational radiation in a Fully Constrained Formulation

2010

This contribution summarizes the recent work carried out to analyze the behavior of the hyperbolic sector of the Fully Constrained Formulation (FCF) derived in Bonazzola et al. 2004. The numerical experiments presented here allows one to be confident in the performances of the upgraded version of CoCoNuT's code by replacing the Conformally Flat Condition (CFC) approximation of the Einstein equations by the FCF.

PhysicsHistoryCode (set theory)Work (thermodynamics)Theoretical physicsHyperbolic sectorGravitational waveEinstein equationsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyComputer Science ApplicationsEducation
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Emission and null coordinates: geometrical properties and physical construction

2011

A Relativistic Positioning System is defined by four clocks (emitters) broadcasting their proper time. Then, every event reached by the signals is naturally labeled by these four times which are the emission coordinates of this event. The coordinate hypersurfaces of the emission coordinates are the future light cones based on the emitter trajectories. For this reason the emission coordinates have been also named null coordinates or light coordinates. Nevertheless, other coordinate systems used in different relativistic contexts have the own right to be named null or light coordinates. Here we analyze when one can say that a coordinate is a null coordinate and when one can say that a coordin…

PhysicsHistoryConical coordinatesParaboloidal coordinatesAstrophysics::High Energy Astrophysical PhenomenaLog-polar coordinatesProlate spheroidal coordinatesAction-angle coordinatesParabolic coordinatesComputer Science ApplicationsEducationGeneral Relativity and Quantum CosmologyClassical mechanicsOrthogonal coordinatesBipolar coordinatesJournal of Physics: Conference Series
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Black hole entropy in loop quantum gravity

2012

4 pags., 2 figs. -- Loops 11: Non-Perturbative / Background Independent Quantum Gravity 23–28 May 2011, Madrid, Spain

PhysicsHistoryEvent horizonAstrophysics::High Energy Astrophysical PhenomenaWhite holeImmirzi parameterComputer Science ApplicationsEducationGeneral Relativity and Quantum CosmologyMicro black holeClassical mechanicsExtremal black holeddc:530Black hole thermodynamicsBlack hole complementarityHawking radiation
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3-D collapse of rotating stars to Kerr black holes

2005

We study gravitational collapse of uniformly rotating neutron stars to Kerr black holes, using a new three-dimensional, fully general relativistic hydrodynamics code, which uses high-resolution shock-capturing techniques and a conformal traceless formulation of the Einstein equations. We investigate the gravitational collapse by carefully studying not only the dynamics of the matter, but also that of the trapped surfaces, i.e. of both the apparent and event horizons formed during the collapse. The use of these surfaces, together with the dynamical horizon framework, allows for a precise measurement of the black-hole mass and spin. The ability to successfully perform these simulations for su…

PhysicsHistoryEvent horizonWhite holeMagnetospheric eternally collapsing objectCompact starComputer Science ApplicationsEducationBlack holeGeneral Relativity and Quantum CosmologyNumerical relativityClassical mechanicsRotating black holeGravitational collapseJournal of Physics: Conference Series
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Non-Riemannian geometry: towards new avenues for the physics of modified gravity

2015

Less explored than their metric (Riemannian) counterparts, metric-affine (or Palatini) theories bring an unexpected phenomenology for gravitational physics beyond General Relativity. Lessons of crystalline structures, where the presence of defects in their microstructure requires the use of non-Riemannian geometry for the proper description of their properties in the macroscopic continuum level, are discussed. In this analogy, concepts such as wormholes and geons play a fundamental role. Applications of the metric-affine formalism developed by the authors in the last three years are reviewed.

PhysicsHistoryGeneral relativityFOS: Physical sciencesAnalogyGeneral Relativity and Quantum Cosmology (gr-qc)Riemannian geometryGeneral Relativity and Quantum CosmologyComputer Science ApplicationsEducationGravitationFormalism (philosophy of mathematics)symbols.namesakeTheoretical physicsGeneral Relativity and Quantum CosmologysymbolsWormholePhenomenology (particle physics)
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Geometric aspects of charged black holes in Palatini theories

2015

Charged black holes in gravity theories in the Palatini formalism present a number of unique properties. Their innermost structure is topologically nontrivial, representing a wormhole supported by a sourceless electric flux. For certain values of their effective mass and charge curvature divergences may be absent, and their event horizon may also disappear yielding a remnant. We give an overview of the mathematical derivation of these solutions and discuss their geodesic structure and other geometric properties.

PhysicsHistoryGeodesicEvent horizonAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)CurvatureElectric fluxGeneral Relativity and Quantum CosmologyComputer Science ApplicationsEducationFormalism (philosophy of mathematics)Theoretical physicsGeneral Relativity and Quantum CosmologyEffective mass (solid-state physics)Wormhole
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