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

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

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<strong>Gravitational</strong> <strong>waves</strong>, theory and experiment (an overview) 3a mixture of the two, and may hold itself together by its own gravitationalattraction. A collection of radiation held together in this way, is call<strong>ed</strong> a geon(gravitational electromagnetic entity) and studi<strong>ed</strong> from a distance, such an objectwould present the same kind of gravitational attraction as any other mass. Yet,nowhere inside the geon is there a place where there is ‘mass’ in the conventionalsense of the term. In particular, for a geon made of pure gravitational radiation—a gravitational geon—there is no local measure of energy, yet there is globalenergy. The gravitational geon owes its existence to a dynamical localiz<strong>ed</strong>—buteverywhere regular—curvature of spacetime, and to nothing more. Thus, a geonis a collection of electromagnetic or gravitational-wave energy, or a mixture ofthe two, held together by its own gravitational attraction, that was describ<strong>ed</strong> byWheeler as ‘mass without mass’.In the 1960s, Joseph Weber began the experimental work to detectgravitational <strong>waves</strong>. He was essentially alone in this field of research [10]. Then,the theoretical work of Wheeler, Bondi, Landau and Lifshitz, Isaacson, Thorneand others and the experimental work of Weber, Braginski, Amaldi and othersopen<strong>ed</strong> a new era of research in this field. In 1972 Steven Weinberg wrote ‘. . .gravitational radiation would be interesting even if there were no chance of everdetecting any, for the theory of gravitational radiation provides a crucial linkbetween general relativity and the microscopic frontiers of physics’ [11].Today gravitational <strong>waves</strong>, both theory and experiment, are one of the maintopics of research in general relativity and gravitation [3].In the same way as electromagnetic <strong>waves</strong> other than visible light, that isradio, millimetre, infrar<strong>ed</strong>, ultraviolet, x-ray and gamma-ray astronomy open<strong>ed</strong>new windows and brought radical changes in our knowl<strong>ed</strong>ge of the universe,gravitational-wave astronomy is expect<strong>ed</strong> to bring a revolution in our knowl<strong>ed</strong>geof the universe by observing new exotic phenomena such as formation andcollision of black holes, fall of stars into supermassive black holes, primordialgravitational <strong>waves</strong> emitt<strong>ed</strong> just after the big bang .... Nevertheless, today,about 85 years after the pr<strong>ed</strong>iction of gravitational <strong>waves</strong> by Einstein, the onlyevidence for their actual existence is indirect and comes from the observationof the energy loss from the binary pulsar system PSR 1913+16, discover<strong>ed</strong> in1974 by Hulse and Taylor [12]. Quite remarkably, though of no surprise, theobserv<strong>ed</strong> energy loss of the binary pulsar is in agreement with the theoreticalpr<strong>ed</strong>iction by general relativity for the energy loss by gravitational radiationemitt<strong>ed</strong> by a binary system, to within less than 0.3% error (in this respect, itmight be interesting to note here that, in regard to the field that in generalrelativity is formally analogous to the magnetic field in electrodynamics, i.e. theso-call<strong>ed</strong> gravitomagnetic field, pr<strong>ed</strong>ict<strong>ed</strong> by Lense and Thirring in 1916, thefirst evidence and measurement of the existence of such an effect on Earth’ssatellites, due to the Earth’s rotation, was publish<strong>ed</strong> only in 1996, that is 80years after the derivation of the effect [13]). Thus, today, together with theenormous experimental efforts to detect gravitational <strong>waves</strong>, from bar detectorsto laser interferometers on Earth, GEO-600, LIGO, VIRGO, ..., and from laser

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