Population synthesis of double neutron stars
Identifieur interne : 006349 ( Main/Curation ); précédent : 006348; suivant : 006350Population synthesis of double neutron stars
Auteurs : S. Osłowski [Australie] ; T. Bulik [Pologne] ; D. Gondek-Rosi Ska [Pologne, France] ; K. Belczy Ski [Pologne, États-Unis]Source :
- Monthly Notices of the Royal Astronomical Society [ 0035-8711 ] ; 2011-05-01.
Descripteurs français
- Pascal (Inist)
English descriptors
- KwdEn :
- Accretion, Accretion rate, Alfv, Angular velocity, Astron, Belczy, Belczynski, Best model, Bhattacharya, Binary, Binary evolution, Binary radio pulsars, Binary stars, Black points, Bmin, Bulik, Chirp, Chirp mass, Chirp masses, Cordes, Death line, Death lines, Dnss, Double neutron stars, Galaxies, Gonthier, Gravitational, Gravitational potential, Gravitational wave, Gravitational waves, Hubble time, Initial masses, Kalogera, Kaspi, Kiel, Konar, Lipunov, Luminosity, Lyne, Magnetic fields, Main sequence, Mass ratio, Mass ratios, Mass scale, Mass transfer, Maximum mass, Merger times, Millisecond pulsars, Mnras, Modelled, Modelling, Models, Monthly notices, Neutron, Neutron star, Neutron star binaries, Neutron stars, Orbital period, Ostriker, Phys, Pmbps, Population synthesis, Probability density, Propeller, Propeller effect, Pulsar, Pulsar evolution, Pulsars, Radio pulsars, Radio selection effects, Radiowave radiation, Recycling, Rudak, Same time, Second pulsar, Selection effect, Selection effects, Semimajor axis, Spatial distribution, Startrack, Startrack code, Stellar, Stellar evolution, Supernova, Urpin, Wave emission, Woosley.
- Teeft :
- Accretion, Accretion rate, Alfv, Angular velocity, Astron, Belczy, Belczynski, Best model, Bhattacharya, Binary, Binary evolution, Binary radio pulsars, Black points, Bmin, Bulik, Chirp, Chirp mass, Chirp masses, Cordes, Death line, Death lines, Dnss, Double neutron stars, Gonthier, Gravitational, Gravitational wave, Gravitational waves, Hubble time, Initial masses, Kalogera, Kaspi, Kiel, Konar, Lipunov, Luminosity, Lyne, Main sequence, Mass ratio, Mass ratios, Mass scale, Mass transfer, Maximum mass, Merger times, Millisecond pulsars, Mnras, Modelled, Modelling, Monthly notices, Neutron, Neutron star, Neutron star binaries, Neutron stars, Orbital period, Ostriker, Phys, Pmbps, Population synthesis, Probability density, Propeller, Propeller effect, Pulsar, Pulsar evolution, Radio pulsars, Radio selection effects, Recycling, Rudak, Same time, Second pulsar, Selection effects, Semimajor axis, Startrack, Startrack code, Stellar, Stellar evolution, Supernova, Urpin, Woosley.
Abstract
Using the StarTrack binary population synthesis code we model the population of double neutron stars in the Galaxy. We include a detailed treatment of the spin evolution of each pulsar due to processes such as spin‐down and spin‐up during accretion events as well as magnetic field decay. We also model the spatial distribution of double neutron stars by including their natal kicks and subsequent propagation in the Galactic gravitational potential. This synthetic pulsar population is compared to the observed sample of double neutron stars taking into account the selection effects of detection in the radio band, to determine the most likely evolutionary parameters. With these parameters we determine the properties of the double neutron star binaries detectable in gravitational waves by the high‐frequency interferometers LIGO and VIRGO. In particular, we discuss the distributions of chirp masses and mass ratios in samples selected by their radio or gravitational wave emission.
Url:
DOI: 10.1111/j.1365-2966.2010.18147.x
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<term>Astron</term>
<term>Belczy</term>
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<term>Chirp</term>
<term>Chirp mass</term>
<term>Chirp masses</term>
<term>Cordes</term>
<term>Death line</term>
<term>Death lines</term>
<term>Dnss</term>
<term>Double neutron stars</term>
<term>Galaxies</term>
<term>Gonthier</term>
<term>Gravitational</term>
<term>Gravitational potential</term>
<term>Gravitational wave</term>
<term>Gravitational waves</term>
<term>Hubble time</term>
<term>Initial masses</term>
<term>Kalogera</term>
<term>Kaspi</term>
<term>Kiel</term>
<term>Konar</term>
<term>Lipunov</term>
<term>Luminosity</term>
<term>Lyne</term>
<term>Magnetic fields</term>
<term>Main sequence</term>
<term>Mass ratio</term>
<term>Mass ratios</term>
<term>Mass scale</term>
<term>Mass transfer</term>
<term>Maximum mass</term>
<term>Merger times</term>
<term>Millisecond pulsars</term>
<term>Mnras</term>
<term>Modelled</term>
<term>Modelling</term>
<term>Models</term>
<term>Monthly notices</term>
<term>Neutron</term>
<term>Neutron star</term>
<term>Neutron star binaries</term>
<term>Neutron stars</term>
<term>Orbital period</term>
<term>Ostriker</term>
<term>Phys</term>
<term>Pmbps</term>
<term>Population synthesis</term>
<term>Probability density</term>
<term>Propeller</term>
<term>Propeller effect</term>
<term>Pulsar</term>
<term>Pulsar evolution</term>
<term>Pulsars</term>
<term>Radio pulsars</term>
<term>Radio selection effects</term>
<term>Radiowave radiation</term>
<term>Recycling</term>
<term>Rudak</term>
<term>Same time</term>
<term>Second pulsar</term>
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<term>Selection effects</term>
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<term>Startrack</term>
<term>Startrack code</term>
<term>Stellar</term>
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<term>Supernova</term>
<term>Urpin</term>
<term>Wave emission</term>
<term>Woosley</term>
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<term>Binaire</term>
<term>Champ magnétique</term>
<term>Effet sélection</term>
<term>Emission onde</term>
<term>Etoile neutron</term>
<term>Galaxies</term>
<term>Modèle</term>
<term>Onde gravitationnelle</term>
<term>Onde radio</term>
<term>Potentiel gravitationnel</term>
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<term>Rapport masse</term>
<term>Répartition spatiale</term>
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<term>Belczy</term>
<term>Belczynski</term>
<term>Best model</term>
<term>Bhattacharya</term>
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<term>Bulik</term>
<term>Chirp</term>
<term>Chirp mass</term>
<term>Chirp masses</term>
<term>Cordes</term>
<term>Death line</term>
<term>Death lines</term>
<term>Dnss</term>
<term>Double neutron stars</term>
<term>Gonthier</term>
<term>Gravitational</term>
<term>Gravitational wave</term>
<term>Gravitational waves</term>
<term>Hubble time</term>
<term>Initial masses</term>
<term>Kalogera</term>
<term>Kaspi</term>
<term>Kiel</term>
<term>Konar</term>
<term>Lipunov</term>
<term>Luminosity</term>
<term>Lyne</term>
<term>Main sequence</term>
<term>Mass ratio</term>
<term>Mass ratios</term>
<term>Mass scale</term>
<term>Mass transfer</term>
<term>Maximum mass</term>
<term>Merger times</term>
<term>Millisecond pulsars</term>
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<term>Modelled</term>
<term>Modelling</term>
<term>Monthly notices</term>
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<term>Population synthesis</term>
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<term>Propeller effect</term>
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<term>Pulsar evolution</term>
<term>Radio pulsars</term>
<term>Radio selection effects</term>
<term>Recycling</term>
<term>Rudak</term>
<term>Same time</term>
<term>Second pulsar</term>
<term>Selection effects</term>
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<front><div type="abstract" xml:lang="en">Using the StarTrack binary population synthesis code we model the population of double neutron stars in the Galaxy. We include a detailed treatment of the spin evolution of each pulsar due to processes such as spin‐down and spin‐up during accretion events as well as magnetic field decay. We also model the spatial distribution of double neutron stars by including their natal kicks and subsequent propagation in the Galactic gravitational potential. This synthetic pulsar population is compared to the observed sample of double neutron stars taking into account the selection effects of detection in the radio band, to determine the most likely evolutionary parameters. With these parameters we determine the properties of the double neutron star binaries detectable in gravitational waves by the high‐frequency interferometers LIGO and VIRGO. In particular, we discuss the distributions of chirp masses and mass ratios in samples selected by their radio or gravitational wave emission.</div>
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<front><div type="abstract" xml:lang="en">Using the STARTRACK binary population synthesis code we model the population of double neutron stars in the Galaxy. We include a detailed treatment of the spin evolution of each pulsar due to processes such as spin-down and spin-up during accretion events as well as magnetic field decay. We also model the spatial distribution of double neutron stars by including their natal kicks and subsequent propagation in the Galactic gravitational potential. This synthetic pulsar population is compared to the observed sample of double neutron stars taking into account the selection effects of detection in the radio band, to determine the most likely evolutionary parameters. With these parameters we determine the properties of the double neutron star binaries detectable in gravitational waves by the high-frequency interferometers LIGO and VIRGO. In particular, we discuss the distributions of chirp masses and mass ratios in samples selected by their radio or gravitational wave emission.</div>
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<term>Modelling</term>
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<term>Death line</term>
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<term>Population synthesis</term>
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<term>Propeller</term>
<term>Propeller effect</term>
<term>Pulsar</term>
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<term>Rudak</term>
<term>Same time</term>
<term>Second pulsar</term>
<term>Selection effects</term>
<term>Semimajor axis</term>
<term>Startrack</term>
<term>Startrack code</term>
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<front><div type="abstract" xml:lang="en">Using the StarTrack binary population synthesis code we model the population of double neutron stars in the Galaxy. We include a detailed treatment of the spin evolution of each pulsar due to processes such as spin‐down and spin‐up during accretion events as well as magnetic field decay. We also model the spatial distribution of double neutron stars by including their natal kicks and subsequent propagation in the Galactic gravitational potential. This synthetic pulsar population is compared to the observed sample of double neutron stars taking into account the selection effects of detection in the radio band, to determine the most likely evolutionary parameters. With these parameters we determine the properties of the double neutron star binaries detectable in gravitational waves by the high‐frequency interferometers LIGO and VIRGO. In particular, we discuss the distributions of chirp masses and mass ratios in samples selected by their radio or gravitational wave emission.</div>
</front>
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