Search results for "Geodesic"

showing 10 items of 131 documents

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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Geodesic completeness in a wormhole spacetime with horizons

2015

The geometry of a spacetime containing a wormhole generated by a spherically symmetric electric field is investigated in detail. These solutions arise in high-energy extensions of General Relativity formulated within the Palatini approach and coupled to Maxwell electrodynamics. Even though curvature divergences generically arise at the wormhole throat, we find that these spacetimes are geodesically complete. This provides an explicit example where curvature divergences do not imply spacetime singularities.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsGeodesicSpacetimeGeneral relativityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)CurvatureGeneral Relativity and Quantum CosmologyTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanicsHigh Energy Physics - Theory (hep-th)Completeness (order theory)Horizon (general relativity)Gravitational singularityWormhole
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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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A Remark on an Overdetermined Problem in Riemannian Geometry

2016

Let (M, g) be a Riemannian manifold with a distinguished point O and assume that the geodesic distance d from O is an isoparametric function. Let \(\varOmega \subset M\) be a bounded domain, with \(O \in \varOmega \), and consider the problem \(\varDelta _p u = -1\ \mathrm{in}\ \varOmega \) with \(u=0\ \mathrm{on}\ \partial \varOmega \), where \(\varDelta _p\) is the p-Laplacian of g. We prove that if the normal derivative \(\partial _{\nu }u\) of u along the boundary of \(\varOmega \) is a function of d satisfying suitable conditions, then \(\varOmega \) must be a geodesic ball. In particular, our result applies to open balls of \(\mathbb {R}^n\) equipped with a rotationally symmetric metr…

PhysicsIsoparametric functionComparison principleGeodesic010102 general mathematicsRotationally symmetric spacesRiemannian manifoldRiemannian geometry01 natural sciencesRotationally symmetric spaceCombinatoricsOverdetermined systemsymbols.namesakeBounded function0103 physical sciencessymbolsComparison principle; Isoparametric functions; Overdetermined PDE; Riemannian Geometry; Rotationally symmetric spaces; Mathematics (all)Isoparametric functionsMathematics (all)Overdetermined PDEMathematics::Differential Geometry010307 mathematical physics0101 mathematicsRiemannian Geometry
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Positioning with stationary emitters in a two-dimensional space-time

2006

The basic elements of the relativistic positioning systems in a two-dimensional space-time have been introduced in a previous work [Phys. Rev. D {\bf 73}, 084017 (2006)] where geodesic positioning systems, constituted by two geodesic emitters, have been considered in a flat space-time. Here, we want to show in what precise senses positioning systems allow to make {\em relativistic gravimetry}. For this purpose, we consider stationary positioning systems, constituted by two uniformly accelerated emitters separated by a constant distance, in two different situations: absence of gravitational field (Minkowski plane) and presence of a gravitational mass (Schwarzschild plane). The physical coord…

PhysicsNuclear and High Energy PhysicsGeodesicSpace timeCoordinate systemFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyMinkowski planeGravitationClassical mechanicsTwo-dimensional spaceGravitational fieldProper time[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]
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Two-dimensional approach to relativistic positioning systems

2006

A relativistic positioning system is a physical realization of a coordinate system consisting in four clocks in arbitrary motion broadcasting their proper times. The basic elements of the relativistic positioning systems are presented in the two-dimensional case. This simplified approach allows to explain and to analyze the properties and interest of these new systems. The positioning system defined by geodesic emitters in flat metric is developed in detail. The information that the data generated by a relativistic positioning system give on the space-time metric interval is analyzed, and the interest of these results in gravimetry is pointed out.

PhysicsNuclear and High Energy PhysicsPositioning systemGeodesicCoordinate systemFOS: Physical sciencesEnergy–momentum relationGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyRelativistic particleClassical mechanicsMetric (mathematics)Relativistic mechanics[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Realization (systems)
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Lens Effect and CMB Anisotropies: Simulations

2003

Cosmological structures deviate the photons of the Cosmic Microwave Background (CMB). The resulting deviations can be calculated moving photons in the gravitational field of realistic lens distributions obtained from numerical simulations. The main goal of this paper is answering the following question: Which types of numerical simulations are appropriate to study angular CMB deformations caused by lensing?

PhysicsPhotonGeodesics in general relativitybusiness.industryCosmic microwave backgroundAstrophysics::Cosmology and Extragalactic Astrophysicslaw.inventionLens (optics)OpticsGravitational fieldlawLens effectAnisotropybusiness
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A Rainich-like approach to the Killing-Yano tensors

2002

The Rainich problem for the Killing-Yano tensors posed by Collinson \cite{col} is solved. In intermediate steps, we first obtain the necessary and sufficient conditions for a 2+2 almost-product structure to determine the principal 2--planes of a skew-symmetric Killing-Yano tensor and then we give the additional conditions on a symmetric Killing tensor for it to be the square of a Killing-Yano tensor.We also analyze a similar problem for the conformal Killing-Yano and the conformal Killing tensors. Our results show that, in both cases, the principal 2--planes define a maxwellian structure. The associated Maxwell fields are obtained and we outline how this approach is of interest in studying …

PhysicsPhysics and Astronomy (miscellaneous)GeodesicFirst integralsStructure (category theory)FOS: Physical sciencesConformal mapGeneral Relativity and Quantum Cosmology (gr-qc)Square (algebra)General Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyKilling tensorTensorMathematics::Differential GeometryMathematical physics
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Accelerated observers and the notion of singular spacetime

2017

Geodesic completeness is typically regarded as a basic criterion to determine whether a given spacetime is regular or singular. However, the principle of general covariance does not privilege any family of observers over the others and, therefore, observers with arbitrary motions should be able to provide a complete physical description of the world. This suggests that in a regular spacetime, all physically acceptable observers should have complete paths. In this work we explore this idea by studying the motion of accelerated observers in spherically symmetric spacetimes and illustrate it by considering two geodesically complete black hole spacetimes recently described in the literature. We…

PhysicsPhysics and Astronomy (miscellaneous)SpacetimeGeodesic010308 nuclear & particles physicsMotion (geometry)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyBlack holeTheoretical physicsGeneral Relativity and Quantum CosmologyGeneral covarianceCompleteness (order theory)0103 physical sciences010306 general physics
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Features of quark and lepton mixing from differential geometry of curves on surfaces

1998

It is noted that the CKM matrix elements for both quarks and leptons as conceived in the Dualized Standard Model (DSM) can be interpreted as direction cosines obtained by moving the Darboux trihedron (a 3-frame) along a trajectory on a sphere traced out through changing energy scales by a 3-vector factorized from the mass matrix. From the `Darboux' analogues of the well-known Serret--Frenet formulae for space curves, it is seen that the corner elements ($V_{ub}, V_{td}$ for quarks, and $U_{e3}, U_{\tau 1}$ for leptons) are associated with the (geodesic) torsion, while the other off-diagonal elements ($V_{us}, V_{cd}$ and $V_{cb}, V_{ts}$ for quarks, and $U_{e2}, U_{\mu 1}$ and $U_{\mu 3}, U…

PhysicsQuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsGeodesicCabibbo–Kobayashi–Maskawa matrixHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaMass matrixMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentNeutrino oscillationLepton
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