Search results for "Einstein"

showing 10 items of 246 documents

What is a singular black hole beyond general relativity?

2017

Exploring the characterization of singular black hole spacetimes, we study the relation between energy density, curvature invariants, and geodesic completeness using a quadratic $f(R)$ gravity theory coupled to an anisotropic fluid. Working in a metric-affine approach, our models and solutions represent minimal extensions of General Relativity (GR) in the sense that they rapidly recover the usual Reissner-Nordstr\"{o}m solution from near the inner horizon outwards. The anisotropic fluid helps modify only the innermost geometry. Depending on the values and signs of two parameters on the gravitational and matter sectors, a breakdown of the correlations between the finiteness/divergence of the…

High Energy Physics - TheoryPhysicsMODIFIED THEORIES OF GRAVITY010308 nuclear & particles physicsGeneral relativityCiencias FísicasFOS: Physical sciences//purl.org/becyt/ford/1.3 [https]General Relativity and Quantum Cosmology (gr-qc)COSMIC CENSORSHIPOtras Ciencias Físicas01 natural sciencesCLASSICAL BLACK HOLESGeneral Relativity and Quantum Cosmology//purl.org/becyt/ford/1 [https]General Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)EINSTEIN-MAXWELL SPACETIMEQuantum mechanics0103 physical sciences010306 general physicsHumanitiesCIENCIAS NATURALES Y EXACTASPhysical Review D
researchProduct

Cosmon Lumps and Horizonless Black Holes

2008

We investigate non-linear, spherically symmetric solutions to the coupled system of a quintessence field and Einstein gravity. In the presence of a scalar potential, we find regular solutions that to an outside observer very closely resemble Schwarzschild black holes. However, these cosmon lumps have neither a horizon nor a central singularity. A stability analysis reveals that our static solutions are dynamically unstable. It remains an open question whether analogous stable solutions exist.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsAstrophysics (astro-ph)FOS: Physical sciencesScalar potentialAstrophysicssymbols.namesakeGeneral Relativity and Quantum CosmologyClassical mechanicsSingularityHigh Energy Physics - Theory (hep-th)symbolsSchwarzschild metricGravitational singularityCircular symmetryEinsteinSchwarzschild radiusQuintessence
researchProduct

Born-Infeld gravity and its functional extensions

2014

We investigate the dynamics of a family of functional extensions of the (Eddington-inspired) Born-Infeld gravity theory, constructed with the inverse of the metric and the Ricci tensor. We provide a generic formal solution for the connection and an Einstein-like representation for the metric field equations of this family of theories. For particular cases we consider applications to the early-time cosmology and find that non-singular universes with a cosmic bounce are very generic and robust solutions.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesClassical field theoryRicci flowGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyClassical unified field theoriesTheoretical physicsEinstein tensorsymbols.namesakeHigh Energy Physics - Theory (hep-th)Born–Infeld modelsymbolsRicci decompositionf(R) gravityRicci curvaturePhysical Review D
researchProduct

A note on Einstein gravity on AdS(3) and boundary conformal field theory

1998

We find a simple relation between the first subleading terms in the asymptotic expansion of the metric field in AdS$_3$, obeying the Brown-Henneaux boundary conditions, and the stress tensor of the underlying Liouville theory on the boundary. We can also provide an more explicit relation between the bulk metric and the boundary conformal field theory when it is described in terms of a free field with a background charge.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsField (physics)Cauchy stress tensorBoundary (topology)Boundary conformal field theoryFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Free fieldGeneral Relativity and Quantum Cosmologysymbols.namesakeHigh Energy Physics - Theory (hep-th)symbolsAstronomiaBoundary value problemCamps Teoria quàntica deEinsteinAsymptotic expansionMathematical physics
researchProduct

Cosmological Horizon Modes and Linear Response in de Sitter Spacetime

2009

Linearized fluctuations of quantized matter fields and the spacetime geometry around de Sitter space are considered in the case that the matter fields are conformally invariant. Taking the unperturbed state of the matter to be the de Sitter invariant Bunch-Davies state, the linear variation of the stress tensor about its self-consistent mean value serves as a source for fluctuations in the geometry through the semiclassical Einstein equations. This linear response framework is used to investigate both the importance of quantum backreaction and the validity of the semiclassical approximation in cosmology. The full variation of the stress tensor delta bi contains two kinds of terms: (1) those…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsQuantum field theory in curved spacetimeCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsCauchy stress tensorDe Sitter spaceSemiclassical physicsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyAuxiliary fieldGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)De Sitter universeQuantum cosmologyQuantum mechanics0103 physical sciencesEinstein field equations010306 general physicsAstrophysics - Cosmology and Nongalactic AstrophysicsMathematical physics
researchProduct

Proper Time Flow Equation for Gravity

2004

We analyze a proper time renormalization group equation for Quantum Einstein Gravity in the Einstein-Hilbert truncation and compare its predictions to those of the conceptually different exact renormalization group equation of the effective average action. We employ a smooth infrared regulator of a special type which is known to give rise to extremely precise critical exponents in scalar theories. We find perfect consistency between the proper time and the average action renormalization group equations. In particular the proper time equation, too, predicts the existence of a non-Gaussian fixed point as it is necessary for the conjectured nonperturbative renormalizability of Quantum Einstein…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsScalar (physics)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Fixed pointRenormalization groupGeneral Relativity and Quantum CosmologyAction (physics)High Energy Physics - PhenomenologyGeneral Relativity and Quantum Cosmologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Flow (mathematics)symbolsProper timeEinsteinCritical exponentMathematical physicsJournal of High Energy Physics
researchProduct

Scale-dependent metric and causal structures in Quantum Einstein Gravity

2006

Within the asymptotic safety scenario for gravity various conceptual issues related to the scale dependence of the metric are analyzed. The running effective field equations implied by the effective average action of Quantum Einstein Gravity (QEG) and the resulting families of resolution dependent metrics are discussed. The status of scale dependent vs. scale independent diffeomorphisms is clarified, and the difference between isometries implemented by scale dependent and independent Killing vectors is explained. A concept of scale dependent causality is proposed and illustrated by various simple examples. The possibility of assigning an "intrinsic length" to objects in a QEG spacetime is a…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsScale (ratio)SpacetimeAsymptotic safety in quantum gravityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyAction (physics)Causality (physics)Theoretical physicssymbols.namesakeHigh Energy Physics - Theory (hep-th)Metric (mathematics)symbolsEinsteinQuantumJournal of High Energy Physics
researchProduct

Free field realization of cylindrically symmetric Einstein gravity

1998

Cylindrically reduced Einstein gravity can be regarded as an $SL(2,R)/SO(2)$ sigma model coupled to 2D dilaton gravity. By using the corresponding 2D diffeomorphism algebra of constraints and the asymptotic behaviour of the Ernst equation we show that the theory can be mapped by a canonical transformation into a set of free fields with a Minkowskian target space. We briefly discuss the quantization in terms of these free-field variables, which is considerably simpler than in the other approaches.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSigma modelFOS: Physical sciencesCanonical transformationGeneral Relativity and Quantum Cosmology (gr-qc)Free fieldGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum Cosmologysymbols.namesakeQuantization (physics)High Energy Physics - Theory (hep-th)symbolsFísica nuclearDilatonNernst equationDiffeomorphismEinsteinMathematical physicsPhysics Letters B
researchProduct

Fractal Spacetime Structure in Asymptotically Safe Gravity

2005

Four-dimensional Quantum Einstein Gravity (QEG) is likely to be an asymptotically safe theory which is applicable at arbitrarily small distance scales. On sub-Planckian distances it predicts that spacetime is a fractal with an effective dimensionality of 2. The original argument leading to this result was based upon the anomalous dimension of Newton's constant. In the present paper we demonstrate that also the spectral dimension equals 2 microscopically, while it is equal to 4 on macroscopic scales. This result is an exact consequence of asymptotic safety and does not rely on any truncation. Contact is made with recent Monte Carlo simulations.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSpacetimeTruncationMonte Carlo methodAsymptotic safety in quantum gravityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum Cosmologysymbols.namesakeClassical mechanicsFractalHigh Energy Physics - Theory (hep-th)symbolsEinsteinConstant (mathematics)Quantum
researchProduct

Gravity, Non-Commutative Geometry and the Wodzicki Residue

1993

We derive an action for gravity in the framework of non-commutative geometry by using the Wodzicki residue. We prove that for a Dirac operator $D$ on an $n$ dimensional compact Riemannian manifold with $n\geq 4$, $n$ even, the Wodzicki residue Res$(D^{-n+2})$ is the integral of the second coefficient of the heat kernel expansion of $D^{2}$. We use this result to derive a gravity action for commutative geometry which is the usual Einstein Hilbert action and we also apply our results to a non-commutative extension which, is given by the tensor product of the algebra of smooth functions on a manifold and a finite dimensional matrix algebra. In this case we obtain gravity with a cosmological co…

High Energy Physics - TheoryPhysicsResidue (complex analysis)General Physics and AstronomyFOS: Physical sciencesGeometryCosmological constantGeneral Relativity and Quantum Cosmology (gr-qc)Riemannian manifoldDirac operatorGeneral Relativity and Quantum Cosmologysymbols.namesakeGeneral Relativity and Quantum CosmologyTensor productHigh Energy Physics - Theory (hep-th)Einstein–Hilbert actionsymbolsGeometry and TopologyCommutative propertyMathematical PhysicsHeat kernel
researchProduct