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

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

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Synopsis<strong>Gravitational</strong> <strong>waves</strong> and their detection are becoming increasingly importantboth for the theoretical physicist and the astrophysicist. In fact, technologicaldevelopments have enabl<strong>ed</strong> the construction of such sensitive detectors (barsand interferometers) that the detection of gravitational radiation could becomea reality during the next few years. In these lectures we give a brief overview ofthis interesting and challenging field of modern physics.The topics cover<strong>ed</strong> are divid<strong>ed</strong> into six lectures. We begin (chapter 2) bydescribing gravitational <strong>waves</strong> in lineariz<strong>ed</strong> general relativity, where one canexamine most of the basic properties of gravitational radiation itself; propagation,gauge invariance and interactions with matter (and in particular with detectors).The second lecture (chapter 3) deals with gravitational-wave detectors:how they operate, what their most important sources of noise are, and whatmechanisms are us<strong>ed</strong> to overcome noise. We report here on the most importantdetectors plann<strong>ed</strong> or under construction (both ground-bas<strong>ed</strong> and space-bas<strong>ed</strong>ones), their likely sensitivity and their prospects for making detections. Otherspeakers will go into much more detail on specific detectors, such as LISA.The third lecture (chapter 4) deals with the astrophysics of likely sourcesof gravitational <strong>waves</strong>: binary systems, neutron stars, pulsars, x-ray sources,supernovae/hypernovae, γ -ray bursts and the big bang. We estimate the expect<strong>ed</strong>wave amplitude h and the suitability of specific detectors for seeing <strong>waves</strong> fromeach source.The fourth lecture (chapter 5) is much more theoretical. Here we developthe mathematical theory of gravitational <strong>waves</strong> in general, their effective stressenergytensor, the energy carri<strong>ed</strong> by gravitational <strong>waves</strong>, and the energy in arandom wave field (gravitational background generat<strong>ed</strong> by the big bang).The fifth lecture (chapter 6) takes the theory further and examines thegeneration of gravitational radiation in lineariz<strong>ed</strong> theory. We show in som<strong>ed</strong>etail how both mass-quadrupole and current-quadrupole radiation is generat<strong>ed</strong>,including how characteristics of the radiation such as its polarization are relat<strong>ed</strong>to the motion of the source. Current-quadrupole radiation has become importantvery recently and may inde<strong>ed</strong> be one of the first forms of gravitational radiation tobe detect<strong>ed</strong>. We attempt to give a physical description of the way it is generat<strong>ed</strong>.13

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