Gravitational waves from pulsars: emission by the magnetic field induced distortion

preprint1996arXivOpen access

Abstract

The gravitational wave emission by a distorted rotating fluid star is computed. The distortion is supposed to be symmetric around some axis inclined with respect to the rotation axis. In the general case, the gravitational radiation is emitted at two frequencies: ΩΩ and 2Ω2Ω, where ΩΩ is the rotation frequency. The obtained formulæ are applied to the specific case of a neutron star distorted by its own magnetic field. Assuming that the period derivative P˙\dot P of pulsars is a measure of their magnetic dipole moment, the gravitational wave amplitude can be related to the observable parameters PP and P˙\dot P and to a factor ββ which measures the efficiency of a given magnetic dipole moment in distorting the star. ββ depends on the nuclear matter equation of state and on the magnetic field distribution. The amplitude at the frequency 2Ω2Ω, expressed in terms of PP, P˙\dot P and ββ, is independent of the angle αα between the magnetic axis and the rotation axis, whereas at the frequency ΩΩ, the amplitude increases as αα decreases. The value of ββ for specific models of magnetic field distributions has been computed by means of a numerical code giving self-consistent models of magnetized neutron stars within general relativity. It is found that the distortion at fixed magnetic dipole moment is very dependent of the magnetic field distribution; a stochastic magnetic field or a superconductor stellar interior greatly increases ββ with respect to the uniformly magnetized perfect conductor case and might lead to gravitational waves detectable by the VIRGO or LIGO interferometers. The amplitude modulation of the signal induced by the daily rotation of the Earth has been computed and specified to the case of the Crab pulsar and VIRGO

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