1,149 research outputs found

    Intrinsic and extrinsic geometries of a tidally deformed black hole

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    A description of the event horizon of a perturbed Schwarzschild black hole is provided in terms of the intrinsic and extrinsic geometries of the null hypersurface. This description relies on a Gauss-Codazzi theory of null hypersurfaces embedded in spacetime, which extends the standard theory of spacelike and timelike hypersurfaces involving the first and second fundamental forms. We show that the intrinsic geometry of the event horizon is invariant under a reparameterization of the null generators, and that the extrinsic geometry depends on the parameterization. Stated differently, we show that while the extrinsic geometry depends on the choice of gauge, the intrinsic geometry is gauge invariant. We apply the formalism to solutions to the vacuum field equations that describe a tidally deformed black hole. In a first instance we consider a slowly-varying, quadrupolar tidal field imposed on the black hole, and in a second instance we examine the tide raised during a close parabolic encounter between the black hole and a small orbiting body.Comment: 27 pages, 4 figure

    Are Time-Domain Self-Force Calculations Contaminated by Jost Solutions?

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    The calculation of the self force in the modeling of the gravitational-wave emission from extreme-mass-ratio binaries is a challenging task. Here we address the question of the possible emergence of a persistent spurious solution in time-domain schemes, referred to as a {\em Jost junk solution} in the literature, that may contaminate self force calculations. Previous studies suggested that Jost solutions are due to the use of zero initial data, which is inconsistent with the singular sources associated with the small object, described as a point mass. However, in this work we show that the specific origin is an inconsistency in the translation of the singular sources into jump conditions. More importantly, we identify the correct implementation of the sources at late times as the sufficient condition guaranteeing the absence of Jost junk solutions.Comment: RevTeX. 5 pages, 2 figures. Version updated to match the contents of the published articl

    Solvable and/or integrable and/or linearizable N-body problems in ordinary (three-dimensional) space. I

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    Several N-body problems in ordinary (3-dimensional) space are introduced which are characterized by Newtonian equations of motion (``acceleration equal force;'' in most cases, the forces are velocity-dependent) and are amenable to exact treatment (``solvable'' and/or ``integrable'' and/or ``linearizable''). These equations of motion are always rotation-invariant, and sometimes translation-invariant as well. In many cases they are Hamiltonian, but the discussion of this aspect is postponed to a subsequent paper. We consider ``few-body problems'' (with, say, \textit{N}=1,2,3,4,6,8,12,16,...) as well as ``many-body problems'' (N an arbitrary positive integer). The main focus of this paper is on various techniques to uncover such N-body problems. We do not discuss the detailed behavior of the solutions of all these problems, but we do identify several models whose motions are completely periodic or multiply periodic, and we exhibit in rather explicit form the solutions in some cases

    Self force in 2+1 electrodynamics

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    The radiation reaction problem for an electric charge moving in flat space-time of three dimensions is discussed. The divergences stemming from the pointness of the particle are studied. A consistent regularization procedure is proposed, which exploits the Poincar\'e invariance of the theory. Effective equation of motion of radiating charge in an external electromagnetic field is obtained via the consideration of energy-momentum and angular momentum conservation. This equation includes the effect of the particle's own field. The radiation reaction is determined by the Lorentz force of point-like charge acting upon itself plus a non-local term which provides finiteness of the self-action.Comment: 20 pages, 3 figure

    Le thon : enjeux et stratégies pour l'océan Indien

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    La pĂȘche rĂ©unionnaise est, depuis les cinq derniĂšres annĂ©es, placĂ©e Ă  contre temps complet de l'immense majoritĂ© des autres pĂȘcheries communautaires (Union europĂ©enne), dans une situation de dĂ©veloppement rapide de l'ensemble de ses segments (pĂȘche artisanale, grande pĂȘche hauturiĂšre antarctique, pĂȘche palangriĂšre). Le plus rapide de ces dĂ©veloppements est certainement celui du segment palangrier qui, nĂ© il y a 5 ans, va cette annĂ©e 1996 Ă©galiser, voire dĂ©passer la pĂȘche artisanale, soit prĂšs de 1 500 t/an. Cette pĂȘcherie est composĂ©e par 9 armements alignant 28 navirees de 12 Ă  33 m dont 20 sont opĂ©rationnels en 1996. Sa production est constituĂ©e pour les espĂšces majeures, de 2/3 d'espadons et de 1/3 de thonidĂ©s. La zone de pĂȘche exploitĂ©e est trĂšs vaste, depuis l'Ă©quateur jusqu'au 35°Sud. Les rendements, aprĂšs avoir prĂ©sentĂ© une augmentation trĂšs significative de 1992 Ă  1994, prĂ©sentent un tassement certain de 1994 Ă  1996 pour tous les navires de la flotte. Ce dĂ©veloppement se poursuit aujourd'hui au niveau de la rĂ©gion COI par un dĂ©veloppement des flottilles palangriĂšres rĂ©gionales, amorcĂ© aux Seychelles et bientĂŽt Ă  Maurice. Un Ă©quilibre d'exploitation pĂ©renne doit impĂ©rativement s'appuyer sur les recherches halieutiques et socio-Ă©conomiques d'accompagnement de cette pĂȘcherie. (RĂ©sumĂ© d'auteur

    Absorption of mass and angular momentum by a black hole: Time-domain formalisms for gravitational perturbations, and the small-hole/slow-motion approximation

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    The first objective of this work is to obtain practical prescriptions to calculate the absorption of mass and angular momentum by a black hole when external processes produce gravitational radiation. These prescriptions are formulated in the time domain within the framework of black-hole perturbation theory. Two such prescriptions are presented. The first is based on the Teukolsky equation and it applies to general (rotating) black holes. The second is based on the Regge-Wheeler and Zerilli equations and it applies to nonrotating black holes. The second objective of this work is to apply the time-domain absorption formalisms to situations in which the black hole is either small or slowly moving. In the context of this small-hole/slow-motion approximation, the equations of black-hole perturbation theory can be solved analytically, and explicit expressions can be obtained for the absorption of mass and angular momentum. The changes in the black-hole parameters can then be understood in terms of an interaction between the tidal gravitational fields supplied by the external universe and the hole's tidally-induced mass and current quadrupole moments. For a nonrotating black hole the quadrupole moments are proportional to the rate of change of the tidal fields on the hole's world line. For a rotating black hole they are proportional to the tidal fields themselves.Comment: 36 pages, revtex4, no figures, final published versio

    Relativistic Effects in Extreme Mass Ratio Gravitational Wave Bursts

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    Extreme mass ratio bursts (EMRBs) have been proposed as a possible source for future space-borne gravitational wave detectors, such as the Laser Interferometer Space Antenna (LISA). These events are characterized by long-period, nearly-radial orbits of compact objects around a central massive black hole. The gravitational radiation emitted during such events consists of a short burst, corresponding to periapse passage, followed by a longer, silent interval. In this paper we investigate the impact of including relativistic corrections to the description of the compact object's trajectory via a geodesic treatment, as well as including higher-order multipole corrections in the waveform calculation. The degree to which the relativistic corrections are important depends on the EMRB's orbital parameters. We find that relativistic EMRBs (v_{max}}/c > 0.25) are not rare and actually account for approximately half of the events in our astrophysical model. The relativistic corrections tend to significantly change the waveform amplitude and phase relative to a Newtonian description, although some of this dephasing could be mimicked by parameter errors. The dephasing over several bursts could be of particular importance not only to gravitational wave detection, but also to parameter estimation, since it is highly correlated to the spin of the massive black hole. Consequently, we postulate that if a relativistic EMRB is detected, such dephasing might be used to probe the relativistic character of the massive black hole and obtain information about its spin.Comment: 13 pages, 8 figures, 2 tables. Replaced with version accepted for publication in the Ap.
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