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The RAVE survey : constraining the local Galactic escape speed

Identifieur interne : 002595 ( PascalFrancis/Curation ); précédent : 002594; suivant : 002596

The RAVE survey : constraining the local Galactic escape speed

Auteurs : Martin C. Smith [Pays-Bas] ; Gregory R. Ruchti [États-Unis] ; Amina Helmi [Pays-Bas] ; Rosemary F. G. Wyse [États-Unis] ; J. P. Fulbright [États-Unis] ; K. C. Freeman [Australie] ; J. F. Navarro [Canada] ; G. M. Seabroke [Royaume-Uni] ; M. Steinmetz [Allemagne] ; M. Williams [Australie] ; O. Bienayme [France] ; J. Binney [Royaume-Uni] ; J. Bland-Hawthorn [Australie] ; W. Dehnen [Royaume-Uni] ; B. K. Gibson [Royaume-Uni] ; G. Gilmore [Royaume-Uni] ; E. K. Grebel [Suisse] ; U. Munari [Italie] ; Q. A. Parker [Australie] ; R.-D. Scholz [Allemagne] ; A. Siebert [Allemagne] ; F. G. Watson [Australie] ; T. Zwitter [Slovénie]

Source :

RBID : Pascal:07-0361816

Descripteurs français

English descriptors

Abstract

We report new constraints on the local escape speed of our Galaxy. Our analysis is based on a sample of high-velocity stars from the RAVE survey and two previously published data sets. We use cosmological simulations of disc galaxy formation to motivate our assumptions on the shape of the velocity distribution, allowing for a significantly more precise measurement of the escape velocity compared to previous studies. We find that the escape velocity lies within the range 498 < ùesc < 608 km s-1 (90 per cent confidence), with a median likelihood of 544 km s-1. The fact that ù2esc is significantly greater than 2ù2circ (where ùcirc = 220km s-1 is the local circular velocity) implies that there must be a significant amount of mass exterior to the solar circle, that is, this convincingly demonstrates the presence of a dark halo in the Galaxy. We use our constraints on ùesc to determine the mass of the Milky Way halo for three halo profiles. For example, an adiabatically contracted NFW halo model results in a virial mass of 1.42+1.44-0.54 x 1012 M◦. and virial radius of 305+66-45 kpc (90 per cent confidence). For this model the circular velocity at the virial radius is 142+31-21 km s-1. Although our halo masses are model dependent, we find that they are in good agreement with each other.
pA  
A01 01  1    @0 0035-8711
A02 01      @0 MNRAA4
A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 379
A06       @2 2
A08 01  1  ENG  @1 The RAVE survey : constraining the local Galactic escape speed
A11 01  1    @1 SMITH (Martin C.)
A11 02  1    @1 RUCHTI (Gregory R.)
A11 03  1    @1 HELMI (Amina)
A11 04  1    @1 WYSE (Rosemary F. G.)
A11 05  1    @1 FULBRIGHT (J. P.)
A11 06  1    @1 FREEMAN (K. C.)
A11 07  1    @1 NAVARRO (J. F.)
A11 08  1    @1 SEABROKE (G. M.)
A11 09  1    @1 STEINMETZ (M.)
A11 10  1    @1 WILLIAMS (M.)
A11 11  1    @1 BIENAYME (O.)
A11 12  1    @1 BINNEY (J.)
A11 13  1    @1 BLAND-HAWTHORN (J.)
A11 14  1    @1 DEHNEN (W.)
A11 15  1    @1 GIBSON (B. K.)
A11 16  1    @1 GILMORE (G.)
A11 17  1    @1 GREBEL (E. K.)
A11 18  1    @1 MUNARI (U.)
A11 19  1    @1 PARKER (Q. A.)
A11 20  1    @1 SCHOLZ (R.-D.)
A11 21  1    @1 SIEBERT (A.)
A11 22  1    @1 WATSON (F. G.)
A11 23  1    @1 ZWITTER (T.)
A14 01      @1 Kapteyn Astronomical Institute, University of Groningen, PO Box 800 @2 9700 AV Groningen @3 NLD @Z 1 aut. @Z 3 aut.
A14 02      @1 Johns Hopkins University, 366 Bloomberg Center, 3400 North Charles Street @2 Baltimore, MD 21218 @3 USA @Z 2 aut. @Z 4 aut. @Z 5 aut.
A14 03      @1 Research School of Astronomy and Astrophysics, Mount Stromlo Observatory, Cotter Road, Weston Creek @2 Canberra, ACT 72611 @3 AUS @Z 6 aut. @Z 10 aut.
A14 04      @1 University of Victoria, PO Box 3055, Station CSC @2 Victoria, BC, V8W 3P6 @3 CAN @Z 7 aut.
A14 05      @1 Institute of Astronomy, University of Cambridge, Madingley Road @2 Cambridge CB3 0HA @3 GBR @Z 8 aut. @Z 16 aut.
A14 06      @1 Astrophysikalisches Institut Potsdam, An der Sterwarte 16 @2 14482 Potsdam @3 DEU @Z 9 aut. @Z 20 aut. @Z 21 aut.
A14 07      @1 Observatoire de Strasbourg, 11 Rue de L'Université @2 67000 Strasbourg @3 FRA @Z 11 aut.
A14 08      @1 Rudolf Peierls Centre for Theoretical Physics, University of Oxford, I Keble Road @2 Oxford OX1 3NP @3 GBR @Z 12 aut.
A14 09      @1 Anglo-Australian Observatory, PO Box 296 @2 Epping, NSW 1710 @3 AUS @Z 13 aut. @Z 19 aut. @Z 22 aut.
A14 10      @1 University of Leicester, University Road @2 Leicester LE1 7RH @3 GBR @Z 14 aut.
A14 11      @1 University of Central Lancashire @2 Preston PR1 2HE @3 GBR @Z 15 aut.
A14 12      @1 Astronomisches Institut, Universität Basel, Venusstrasse 7 @2 Binningen 4102 @3 CHE @Z 17 aut.
A14 13      @1 INAF Osservatorio Astronomico di Padova, Via dell'Osservatorio 8 @2 Asiago 36012 @3 ITA @Z 18 aut.
A14 14      @1 Macquarie University @2 Sydney, NSW 2109 @3 AUS @Z 19 aut.
A14 15      @1 Department of Physics, University of Ljubljana, Jadranska 19 @2 Ljubljana @3 SVN @Z 23 aut.
A20       @1 755-772
A21       @1 2007
A23 01      @0 ENG
A43 01      @1 INIST @2 2067 @5 354000149977960230
A44       @0 0000 @1 © 2007 INIST-CNRS. All rights reserved.
A45       @0 3/4 p.
A47 01  1    @0 07-0361816
A60       @1 P
A61       @0 A
A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 GBR
C01 01    ENG  @0 We report new constraints on the local escape speed of our Galaxy. Our analysis is based on a sample of high-velocity stars from the RAVE survey and two previously published data sets. We use cosmological simulations of disc galaxy formation to motivate our assumptions on the shape of the velocity distribution, allowing for a significantly more precise measurement of the escape velocity compared to previous studies. We find that the escape velocity lies within the range 498 < ùesc < 608 km s-1 (90 per cent confidence), with a median likelihood of 544 km s-1. The fact that ù2esc is significantly greater than 2ù2circ (where ùcirc = 220km s-1 is the local circular velocity) implies that there must be a significant amount of mass exterior to the solar circle, that is, this convincingly demonstrates the presence of a dark halo in the Galaxy. We use our constraints on ùesc to determine the mass of the Milky Way halo for three halo profiles. For example, an adiabatically contracted NFW halo model results in a virial mass of 1.42+1.44-0.54 x 1012 M◦. and virial radius of 305+66-45 kpc (90 per cent confidence). For this model the circular velocity at the virial radius is 142+31-21 km s-1. Although our halo masses are model dependent, we find that they are in good agreement with each other.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Galaxies disques @5 26
C03 01  3  ENG  @0 Disk galaxies @5 26
C03 02  X  FRE  @0 Etoile grande vitesse @5 27
C03 02  X  ENG  @0 High velocity star @5 27
C03 02  X  SPA  @0 Estrella gran velocidad @5 27
C03 03  3  FRE  @0 Formation galaxies @5 28
C03 03  3  ENG  @0 Galaxy formation @5 28
C03 04  3  FRE  @0 Distribution vitesse @5 29
C03 04  3  ENG  @0 Velocity distribution @5 29
C03 05  3  FRE  @0 Vitesse fuite @5 30
C03 05  3  ENG  @0 Escape velocity @5 30
C03 06  X  FRE  @0 Cercle @5 31
C03 06  X  ENG  @0 Circle @5 31
C03 06  X  SPA  @0 Circulo @5 31
C03 07  3  FRE  @0 Halo galactique @5 32
C03 07  3  ENG  @0 Galactic halos @5 32
C03 08  X  FRE  @0 Modèle @5 33
C03 08  X  ENG  @0 Models @5 33
C03 08  X  SPA  @0 Modelo @5 33
C03 09  X  FRE  @0 Masse viriel @5 34
C03 09  X  ENG  @0 Virial mass @5 34
C03 09  X  SPA  @0 Masa virial @5 34
C03 10  3  FRE  @0 Cinématique @5 35
C03 10  3  ENG  @0 Kinematics @5 35
C03 11  3  FRE  @0 Dynamique @5 36
C03 11  3  ENG  @0 Dynamics @5 36
C03 12  3  FRE  @0 Voie lactée @5 37
C03 12  3  ENG  @0 Milky Way @5 37
C03 13  3  FRE  @0 Halo galaxies @4 CD @5 96
C03 13  3  ENG  @0 Galaxy halo @4 CD @5 96
C03 13  3  SPA  @0 Halo galaxia @4 CD @5 96
N21       @1 232
N44 01      @1 OTO
N82       @1 OTO

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Pascal:07-0361816

Le document en format XML

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<title xml:lang="en" level="a">The RAVE survey : constraining the local Galactic escape speed</title>
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<country>Suisse</country>
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<name sortKey="Watson, F G" sort="Watson, F G" uniqKey="Watson F" first="F. G." last="Watson">F. G. Watson</name>
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<name sortKey="Zwitter, T" sort="Zwitter, T" uniqKey="Zwitter T" first="T." last="Zwitter">T. Zwitter</name>
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<s1>Department of Physics, University of Ljubljana, Jadranska 19</s1>
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<series>
<title level="j" type="main">Monthly Notices of the Royal Astronomical Society</title>
<title level="j" type="abbreviated">Mon. Not. R. Astron. Soc.</title>
<idno type="ISSN">0035-8711</idno>
<imprint>
<date when="2007">2007</date>
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<title level="j" type="main">Monthly Notices of the Royal Astronomical Society</title>
<title level="j" type="abbreviated">Mon. Not. R. Astron. Soc.</title>
<idno type="ISSN">0035-8711</idno>
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<keywords scheme="KwdEn" xml:lang="en">
<term>Circle</term>
<term>Disk galaxies</term>
<term>Dynamics</term>
<term>Escape velocity</term>
<term>Galactic halos</term>
<term>Galaxy formation</term>
<term>Galaxy halo</term>
<term>High velocity star</term>
<term>Kinematics</term>
<term>Milky Way</term>
<term>Models</term>
<term>Velocity distribution</term>
<term>Virial mass</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Galaxies disques</term>
<term>Etoile grande vitesse</term>
<term>Formation galaxies</term>
<term>Distribution vitesse</term>
<term>Vitesse fuite</term>
<term>Cercle</term>
<term>Halo galactique</term>
<term>Modèle</term>
<term>Masse viriel</term>
<term>Cinématique</term>
<term>Dynamique</term>
<term>Voie lactée</term>
<term>Halo galaxies</term>
</keywords>
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<front>
<div type="abstract" xml:lang="en">We report new constraints on the local escape speed of our Galaxy. Our analysis is based on a sample of high-velocity stars from the RAVE survey and two previously published data sets. We use cosmological simulations of disc galaxy formation to motivate our assumptions on the shape of the velocity distribution, allowing for a significantly more precise measurement of the escape velocity compared to previous studies. We find that the escape velocity lies within the range 498 < ù
<sub>esc</sub>
< 608 km s
<sup>-1</sup>
(90 per cent confidence), with a median likelihood of 544 km s
<sup>-1</sup>
. The fact that ù
<sup>2</sup>
<sub>esc</sub>
is significantly greater than 2ù
<sup>2</sup>
<sub>circ</sub>
(where ù
<sub>circ</sub>
= 220km s
<sup>-1</sup>
is the local circular velocity) implies that there must be a significant amount of mass exterior to the solar circle, that is, this convincingly demonstrates the presence of a dark halo in the Galaxy. We use our constraints on ù
<sub>esc</sub>
to determine the mass of the Milky Way halo for three halo profiles. For example, an adiabatically contracted NFW halo model results in a virial mass of 1.42
<sup>+1.44</sup>
<sub>-0.54</sub>
x 1012 M
<sub>◦.</sub>
and virial radius of 305
<sup>+66</sup>
<sub>-45</sub>
kpc (90 per cent confidence). For this model the circular velocity at the virial radius is 142
<sup>+31</sup>
<sub>-21</sub>
km s
<sup>-1</sup>
. Although our halo masses are model dependent, we find that they are in good agreement with each other.</div>
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<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Monthly Notices of the Royal Astronomical Society</s0>
</fA64>
<fA66 i1="01">
<s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>We report new constraints on the local escape speed of our Galaxy. Our analysis is based on a sample of high-velocity stars from the RAVE survey and two previously published data sets. We use cosmological simulations of disc galaxy formation to motivate our assumptions on the shape of the velocity distribution, allowing for a significantly more precise measurement of the escape velocity compared to previous studies. We find that the escape velocity lies within the range 498 < ù
<sub>esc</sub>
< 608 km s
<sup>-1</sup>
(90 per cent confidence), with a median likelihood of 544 km s
<sup>-1</sup>
. The fact that ù
<sup>2</sup>
<sub>esc</sub>
is significantly greater than 2ù
<sup>2</sup>
<sub>circ</sub>
(where ù
<sub>circ</sub>
= 220km s
<sup>-1</sup>
is the local circular velocity) implies that there must be a significant amount of mass exterior to the solar circle, that is, this convincingly demonstrates the presence of a dark halo in the Galaxy. We use our constraints on ù
<sub>esc</sub>
to determine the mass of the Milky Way halo for three halo profiles. For example, an adiabatically contracted NFW halo model results in a virial mass of 1.42
<sup>+1.44</sup>
<sub>-0.54</sub>
x 1012 M
<sub>◦.</sub>
and virial radius of 305
<sup>+66</sup>
<sub>-45</sub>
kpc (90 per cent confidence). For this model the circular velocity at the virial radius is 142
<sup>+31</sup>
<sub>-21</sub>
km s
<sup>-1</sup>
. Although our halo masses are model dependent, we find that they are in good agreement with each other.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Galaxies disques</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Disk galaxies</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE">
<s0>Etoile grande vitesse</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG">
<s0>High velocity star</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA">
<s0>Estrella gran velocidad</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Formation galaxies</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Galaxy formation</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Distribution vitesse</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Velocity distribution</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Vitesse fuite</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Escape velocity</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Cercle</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Circle</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Circulo</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Halo galactique</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Galactic halos</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE">
<s0>Modèle</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Models</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Modelo</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Masse viriel</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Virial mass</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Masa virial</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Cinématique</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Kinematics</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Dynamique</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Dynamics</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Voie lactée</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Milky Way</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Halo galaxies</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Galaxy halo</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="13" i2="3" l="SPA">
<s0>Halo galaxia</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21>
<s1>232</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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