Epicyclic oscillations in the Hartle-Thorne external geometry

The external Hartle-Thorne geometry, which describes the space-time outside a slowly-rotating compact star, is characterized by the gravitational mass \(M\), angular momentum \(J\) and quadrupole moment \(Q\) of the star and gives a convenient description which, for the rotation frequencies of more...

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Veröffentlicht in:arXiv.org 2019-05
Hauptverfasser: Urbancová, Gabriela, Urbanec, Martin, Török, Gabriel, Stuchlík, Zdeněk, Blaschke, Martin, Miller, John C
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Sprache:eng
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Zusammenfassung:The external Hartle-Thorne geometry, which describes the space-time outside a slowly-rotating compact star, is characterized by the gravitational mass \(M\), angular momentum \(J\) and quadrupole moment \(Q\) of the star and gives a convenient description which, for the rotation frequencies of more than 95 % of known pulsars, is sufficiently accurate for most purposes. We focus here on the motion of particles in these space-times, presenting a detailed systematic analysis of the frequency properties of radial and vertical epicyclic motion and of orbital motion. Our investigation is motivated by X-ray observations of binary systems containing a rotating neutron star which is accreting matter from its binary companion. In these systems, twin high-frequency quasi-periodic oscillations are sometimes observed with a frequency ratio approaching \(3:2\) or \(5:4\) and these may be explained by models involving the orbital and epicyclic frequencies of quasi-circular geodesic motion. In our analysis, we use realistic equations of state for the stellar matter and proceed in a self-consistent way, following the Hartle-Thorne approach in calculating both the corresponding values of \(Q\), \(M\) and \(J\) for the stellar model and the properties of the surrounding spacetime. Our results are then applied to a range of geodetical models for QPOs. A key feature of our study is that it implements the recently-discovered universal relations among neutron star parameters so that the results can be directly used for models with different masses \(M\), radii \(R\) and rotational frequencies \(f_\mathrm{rot}\).
ISSN:2331-8422
DOI:10.48550/arxiv.1905.00730