Serveur d'exploration sur les relations entre la France et l'Australie

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Population synthesis of double neutron stars

Identifieur interne : 004124 ( PascalFrancis/Curation ); précédent : 004123; suivant : 004125

Population synthesis of double neutron stars

Auteurs : S. Oslowski [Australie] ; T. Bulik [Pologne] ; D. Gondek-Rosinska [Pologne, France] ; K. Belczynski [Pologne, États-Unis]

Source :

RBID : Pascal:11-0208604

Descripteurs français

English descriptors

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.
pA  
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A03   1    @0 Mon. Not. R. Astron. Soc.
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A06       @2 1
A08 01  1  ENG  @1 Population synthesis of double neutron stars
A11 01  1    @1 OSLOWSKI (S.)
A11 02  1    @1 BULIK (T.)
A11 03  1    @1 GONDEK-ROSINSKA (D.)
A11 04  1    @1 BELCZYNSKI (K.)
A14 01      @1 Swinburne University of Technology, Centre for Astrophysics and Supercomputing. Mail H39, PO Box 218 @2 VIC 3122 @3 AUS @Z 1 aut.
A14 02      @1 CSIRO Astronomy and Space Sciences, Australia Telescope National Facility, PO Box 76 @2 Epping, NSW 1710 @3 AUS @Z 1 aut.
A14 03      @1 Astronomical Observatory, University of Warsaw, Aleje Ujazdowskie 4 @2 00-478 Warsaw @3 POL @Z 2 aut. @Z 4 aut.
A14 04      @1 Nicolaus Copernicus Astronomical Centre, Bartvcka 18 @2 00716 Warszawa @3 POL @Z 2 aut. @Z 3 aut.
A14 05      @1 Institute of Astronomy, University of Zielona Gòra, Lubuska 2 @2 65-265 Zielona Gòra @3 POL @Z 3 aut.
A14 06      @1 LUTH, Observatoire de Paris, Universite Paris 7, Place Jules Janssen @2 92195 Meudon @3 FRA @Z 3 aut.
A14 07      @1 Department of Physics and Astronomy, University of Texas @2 Brownsville, TX 78520 @3 USA @Z 4 aut.
A20       @1 461-479
A21       @1 2011
A23 01      @0 ENG
A43 01      @1 INIST @2 2067 @5 354000192958730340
A44       @0 0000 @1 © 2011 INIST-CNRS. All rights reserved.
A45       @0 1 p.1/2
A47 01  1    @0 11-0208604
A60       @1 P
A61       @0 A
A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 USA
C01 01    ENG  @0 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.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Etoile neutron @5 26
C03 01  3  ENG  @0 Neutron stars @5 26
C03 02  X  FRE  @0 Modèle @5 27
C03 02  X  ENG  @0 Models @5 27
C03 02  X  SPA  @0 Modelo @5 27
C03 03  3  FRE  @0 Galaxies @5 28
C03 03  3  ENG  @0 Galaxies @5 28
C03 04  3  FRE  @0 Pulsar @5 29
C03 04  3  ENG  @0 Pulsars @5 29
C03 05  3  FRE  @0 Accrétion @5 30
C03 05  3  ENG  @0 Accretion @5 30
C03 06  3  FRE  @0 Champ magnétique @5 31
C03 06  3  ENG  @0 Magnetic fields @5 31
C03 07  3  FRE  @0 Répartition spatiale @5 32
C03 07  3  ENG  @0 Spatial distribution @5 32
C03 08  3  FRE  @0 Potentiel gravitationnel @5 33
C03 08  3  ENG  @0 Gravitational potential @5 33
C03 09  X  FRE  @0 Effet sélection @5 34
C03 09  X  ENG  @0 Selection effect @5 34
C03 09  X  SPA  @0 Efecto selección @5 34
C03 10  3  FRE  @0 Binaire @5 35
C03 10  3  ENG  @0 Binary stars @5 35
C03 11  3  FRE  @0 Onde gravitationnelle @5 36
C03 11  3  ENG  @0 Gravitational waves @5 36
C03 12  X  FRE  @0 Rapport masse @5 37
C03 12  X  ENG  @0 Mass ratio @5 37
C03 12  X  SPA  @0 Relación masa @5 37
C03 13  3  FRE  @0 Onde radio @5 38
C03 13  3  ENG  @0 Radiowave radiation @5 38
C03 14  X  FRE  @0 Emission onde @5 39
C03 14  X  ENG  @0 Wave emission @5 39
C03 14  X  SPA  @0 Emisión onda @5 39
N21       @1 136
N44 01      @1 OTO
N82       @1 OTO

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Pascal:11-0208604

Le document en format XML

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<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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<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Répartition spatiale</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Spatial distribution</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Potentiel gravitationnel</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Gravitational potential</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Effet sélection</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Selection effect</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Efecto selección</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Binaire</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Binary stars</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Onde gravitationnelle</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Gravitational waves</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Rapport masse</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>Mass ratio</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Relación masa</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Onde radio</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Radiowave radiation</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE">
<s0>Emission onde</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG">
<s0>Wave emission</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA">
<s0>Emisión onda</s0>
<s5>39</s5>
</fC03>
<fN21>
<s1>136</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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