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(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

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Chapter 17Post-Newtonian computation of binaryinspiral waveformsLuc BlanchetDépartement d’Astrophysique Relativiste et de Cosmologie,Centre National de la Recherche Scientifique (UMR 8629),Observatoire de Paris, 92195 Meudon C<strong>ed</strong>ex, France17.1 IntroductionAstrophysical systems known as inspiralling compact binaries are among themost interesting sources to hunt for gravitational radiation in the future networkof laser-interferometric detectors, compos<strong>ed</strong> of the large-scale interferometersVIRGO and LIGO, and the m<strong>ed</strong>ium-scale ones GEO and TAMA (see the books[1–3] for reviews, and the contribution of B Schutz in this volume). Thesesystems are compos<strong>ed</strong> of two compact objects, i.e. gravitationally-condens<strong>ed</strong>neutron stars or black holes, whose orbit follows an inward spiral, with decreasingorbital radius r and increasing orbital frequency ω. The inspiral is driven bythe loss of energy associat<strong>ed</strong> with the gravitational-wave emission. Because th<strong>ed</strong>ynamics of a binary is essentially aspherical, inspiralling compact binaries arestrong emitters of gravitational radiation. Tidal interactions between the compactobjects are expect<strong>ed</strong> to play a little role during most of the inspiral phase; themass transfer (in the case of neutron stars) does not occur until very late, nearthe final coalescence. Inspiralling compact binaries are very clean systems,essentially dominat<strong>ed</strong> by gravitational forces. Therefore, the relevant model fordescribing the inspiral phase consists of two point-masses moving under theirmutual gravitational attraction. As a simplification for the theoretical analysis,the orbit of inspiralling binaries can be consider<strong>ed</strong> to be circular, apart from thegradual inspiral, with a good approximation. At some point in the evolution, therewill be a transition from the adiabatic inspiral to the plunge of the two objectsfollow<strong>ed</strong> by the collision and final merger. Evidently the model of point-masses338

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