Search results for "Einstein"

showing 10 items of 246 documents

A Lemaitre-Tolman-Bondi cosmological wormhole

2010

We present a new analytical solution of the Einstein field equations describing a wormhole shell of zero thickness joining two Lema{\i}tre-Tolman-Bondi universes, with no radial accretion. The material on the shell satisfies the energy conditions and, at late times, the shell becomes comoving with the dust-dominated cosmic substratum.

PhysicsNuclear and High Energy PhysicsAccretion (meteorology)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaShell (structure)Zero (complex analysis)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)Astrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesCosmologyGeneral Relativity and Quantum CosmologyStarsGeneral Relativity and Quantum CosmologyClassical mechanics0103 physical sciencesEinstein field equationsAstrophysics::Earth and Planetary AstrophysicsWormholeField equation010303 astronomy & astrophysicsMathematical Physics
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Mathematical Issues in a Fully-Constrained Formulation of Einstein Equations

2008

Bonazzola, Gourgoulhon, Grandcl\'ement, and Novak [Phys. Rev. D {\bf 70}, 104007 (2004)] proposed a new formulation for 3+1 numerical relativity. Einstein equations result, according to that formalism, in a coupled elliptic-hyperbolic system. We have carried out a preliminary analysis of the mathematical structure of that system, in particular focusing on the equations governing the evolution for the deviation of a conformal metric from a flat fiducial one. The choice of a Dirac's gauge for the spatial coordinates guarantees the mathematical characterization of that system as a (strongly) hyperbolic system of conservation laws. In the presence of boundaries, this characterization also depen…

PhysicsNuclear and High Energy PhysicsConservation lawPartial differential equationSpace timeMathematical analysisFOS: Physical sciencesConformal mapGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyNumerical relativityClassical mechanicsEinstein field equationsBoundary value problemMathematical structure
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Relativistic second-order perturbations of the Einstein-de Sitter universe

1998

We consider the evolution of relativistic perturbations in the Einstein-de Sitter cosmological model, including second-order effects. The perturbations are considered in two different settings: the widely used synchronous gauge and the Poisson (generalized longitudinal) one. Since, in general, perturbations are gauge dependent, we start by considering gauge transformations at second order. Next, we give the evolution of perturbations in the synchronous gauge, taking into account both scalar and tensor modes in the initial conditions. Using the second-order gauge transformation previously defined, we are then able to transform these perturbations to the Poisson gauge. The most important feat…

PhysicsNuclear and High Energy PhysicsEinstein–de Sitter universeGravitational waveAstrophysics (astro-ph)Cosmic microwave backgroundFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Cosmological modelPoisson distributionAstrophysicsGeneral Relativity and Quantum CosmologyFormalism (philosophy of mathematics)symbols.namesakeClassical mechanicssymbolsGauge theoryAnisotropyMathematical physics
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Improved constrained scheme for the Einstein equations: An approach to the uniqueness issue

2008

Uniqueness problems in the elliptic sector of constrained formulations of Einstein equations have a dramatic effect on the physical validity of some numerical solutions, for instance when calculating the spacetime of very compact stars or nascent black holes. The fully constrained formulation (FCF) proposed by Bonazzola, Gourgoulhon, Grandcl\'ement, and Novak is one of these formulations. It contains, as a particular case, the approximation of the conformal flatness condition (CFC) which, in the last ten years, has been used in many astrophysical applications. The elliptic part of the FCF basically shares the same differential operators as the elliptic equations in CFC scheme. We present he…

PhysicsNuclear and High Energy PhysicsGeneral relativityEquations of motionFOS: Physical sciencesConformal mapGeneral Relativity and Quantum Cosmology (gr-qc)Differential operatorGeneral Relativity and Quantum Cosmologysymbols.namesakeClassical mechanicsEinstein field equationssymbolsApplied mathematicsUniquenessEinsteinFlatness (mathematics)
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Inconsistencies in four-dimensional Einstein-Gauss-Bonnet gravity

2021

We attempt to clarify several aspects concerning the recently presented four-dimensional Einstein-Gauss-Bonnet gravity. We argue that the limiting procedure outlined in [Phys. Rev. Lett. 124, 081301 (2020)] generally involves ill-defined terms in the four dimensional field equations. Potential ways to circumvent this issue are discussed, alongside remarks regarding specific solutions of the theory. We prove that, although linear perturbations are well behaved around maximally symmetric backgrounds, the equations for second-order perturbations are ill-defined even around a Minkowskian background. Additionally, we perform a detailed analysis of the spherically symmetric solutions and find tha…

PhysicsNuclear and High Energy PhysicsGovernment010308 nuclear & particles physicsCenter of excellenceFOS: Physical sciencesAstronomy and AstrophysicsGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyManagementsymbols.namesakeState agencyWork (electrical)0103 physical sciencessymbolsChristian ministryEinstein010306 general physicsInstrumentation
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Combining spectral and shock-capturing methods: A new numerical approach for 3D relativistic core collapse simulations

2005

We present a new three-dimensional general relativistic hydrodynamics code which is intended for simulations of stellar core collapse to a neutron star, as well as pulsations and instabilities of rotating relativistic stars. Contrary to the common approach followed in most existing three-dimensional numerical relativity codes which are based in Cartesian coordinates, in this code both the metric and the hydrodynamics equations are formulated and solved numerically using spherical polar coordinates. A distinctive feature of this new code is the combination of two types of accurate numerical schemes specifically designed to solve each system of equations. More precisely, the code uses spectra…

PhysicsNuclear and High Energy PhysicsNumerical relativityClassical mechanicsGravitational collapseEinstein field equationsFinite difference methodFinite differenceApplied mathematicsSystem of linear equationsSpectral methodNumerical stabilityPhysical Review D
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Two-pion Bose–Einstein correlations in central Pb–Pb collisions at sNN=2.76 TeV

2011

The first measurement of two-pion Bose-Einstein correlations in central Pb-Pb collisions at root(NN)-N-S = 2.76 TeV at the Large Hadron Collider is presented. We observe a growing trend with energy now not only for the longitudinal and the outward but also for the sideward pion source radius. The pion homogeneity volume and the decoupling time are significantly larger than those measured at RHIC. (C) 2010 CERN. Published by Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsNuclear TheoryBose–Einstein correlationsDecoupling (cosmology)01 natural sciencesNuclear physicsPion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics Letters B
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Two-pion Bose-Einstein correlations inppcollisions ats=900  GeV

2010

We report on the measurement of two-pion correlation functions from pp collisions at root s = 900 GeV performed by the ALICE experiment at the Large Hadron Collider. Our analysis shows an increase of the Hanbury Brown-Twiss radius with increasing event multiplicity, in line with other measurements done in particle- and nuclear collisions. Conversely, the strong decrease of the radius with increasing transverse momentum, as observed at the Relativistic Heavy Ion Collider and at Tevatron, is not manifest in our data.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMeson010308 nuclear & particles physicsNuclear TheoryHadronTevatronParticle acceleratorBose–Einstein correlations01 natural scienceslaw.inventionNuclear physicsPionlaw0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review D
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Femtoscopy ofppcollisions ats=0.9and 7 TeV at the LHC with two-pion Bose-Einstein correlations

2011

We report on the high statistics two-pion correlation functions from pp collisions at root s = 0.9 TeV and root s = 7 TeV, measured by the ALICE experiment at the Large Hadron Collider. The correlation functions as well as the extracted source radii scale with event multiplicity and pair momentum. When analyzed in the same multiplicity and pair transverse momentum range, the correlation is similar at the two collision energies. A three-dimensional femtoscopic analysis shows an increase of the emission zone with increasing event multiplicity as well as decreasing homogeneity lengths with increasing transverse momentum. The latter trend gets more pronounced as multiplicity increases. This sug…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsHadronElementary particleMultiplicity (mathematics)Bose–Einstein correlations01 natural sciencesMomentumNuclear physicssymbols.namesakePionBose–Einstein statistics0103 physical sciencessymbolsNuclear Experiment010306 general physicsPhysical Review D
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Duality-invariant Einstein-Planck relation and the speed of light at very short wavelengths

2011

We propose a generalized Einstein-Planck relation for photons which is invariant under the change $\ensuremath{\lambda}/a{l}_{P}$ to $a{l}_{P}/\ensuremath{\lambda}$, $\ensuremath{\lambda}$ being the photon wavelength, ${l}_{P}$ Planck's length, and $a$ a numerical constant. This yields a wavelength-dependent speed of light $v(\ensuremath{\lambda})=c/(1+{a}^{2}({l}_{P}/\ensuremath{\lambda}{)}^{2})$, with $c$ the usual speed of light in vacuo, indicating that the speed of light should decrease for sufficiently short wavelengths. We discuss the conceptual differences with the previous proposals related to a possible decrease of the speed of light for very short wavelengths based on quantum flu…

PhysicsNuclear and High Energy PhysicsPhotonUncertainty principleInvariant (physics)Lambdasymbols.namesakeWavelengthQuantum mechanicssymbolsQuantum gravityPlanckLight velocity Einstein-Planck relation duality relationsSettore MAT/07 - Fisica MatematicaQuantum fluctuation
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