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The kinematic identification of a thick stellar disc in M31

Identifieur interne : 004232 ( PascalFrancis/Curation ); précédent : 004231; suivant : 004233

The kinematic identification of a thick stellar disc in M31

Auteurs : M. L. M. Collins [États-Unis] ; S. C. Chapman [États-Unis] ; R. A. Ibata [France] ; M. J. Irwin [États-Unis] ; R. M. Rich [États-Unis] ; A. M. N. Ferguson [États-Unis] ; G. F. Lewis [Australie] ; N. Tanvir [Royaume-Uni] ; A. Koch [Royaume-Uni]

Source :

RBID : Pascal:11-0260679

Descripteurs français

English descriptors

Abstract

We present the first characterization of a thick-disc component in the Andromeda galaxy (M31) using kinematic data from the DEIMOS instrument on Keck II. Using 21 fields in the south-west of the galaxy, we measure the lag of this component with respect to the thin disc, as well as the dispersion, metallicity and scalelength of the component. We find an average lag between the two components of ?Δù? = 46.0 ± 3.9 km s-1. The velocity dispersion of the thick disc is σthick= 50.8±1.9 km s-1, greater than the value of dispersion we determine for the thin disc, σthin= 35.7 ± 1.0 km s-1. The thick disc is more metal poor than the thin disc, with [Fe/H]spec=-1.0±0.1 compared with [Fe/H]spec=-0.7 ± 0.05 for the thin disc. We measure a radial scalelength of the thin and thick discs of hr = 7.3±1.0 and 8.0 ± 1.2 kpc, respectively. From this, we infer scaleheights for both discs of 1.1±0.2 and 2.8± 0.6 kpc, both of which are approximately two to three times larger than those observed in the Milky Way. We estimate a mass range for the thick-disc component of 2.4 x1010 < M*,thick < 4.1× 1010 M◦.. This value provides a useful constraint on possible formation mechanisms, as any proposed method for forming a thick disc must be able to heat (or deposit) at least this amount of material.
pA  
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A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 413
A06       @2 3
A08 01  1  ENG  @1 The kinematic identification of a thick stellar disc in M31
A11 01  1    @1 COLLINS (M. L. M.)
A11 02  1    @1 CHAPMAN (S. C.)
A11 03  1    @1 IBATA (R. A.)
A11 04  1    @1 IRWIN (M. J.)
A11 05  1    @1 RICH (R. M.)
A11 06  1    @1 FERGUSON (A. M. N.)
A11 07  1    @1 LEWIS (G. F.)
A11 08  1    @1 TANVIR (N.)
A11 09  1    @1 KOCH (A.)
A14 01      @1 Institute of Astronomy, University of Cambridge, Madingley Road @2 Cambridge CB3 0HA @3 USA @Z 1 aut. @Z 2 aut. @Z 4 aut.
A14 02      @1 Observatoire de Strasbourg, 11 rue de l'Université @2 67000 Strasbourg @3 FRA @Z 3 aut.
A14 03      @1 Department of Physics and Astronomy, University of California @2 Los Angeles, CA 90095-1547 @3 USA @Z 5 aut.
A14 04      @1 Institute for Astronomy, University of Edinburgh, Royal Observatory, Blackford Hill @2 Edinburgh EH9 3HJ @3 USA @Z 6 aut.
A14 05      @1 Sydney Institute for Astronomy, School of Physics, A29, University of Sydney @2 NSW 2006 @3 AUS @Z 7 aut.
A14 06      @1 Department of Physics & Astronomy, University of Leicester, University Road @2 Leicester LE1 7RH @3 GBR @Z 8 aut. @Z 9 aut.
A20       @1 1548-1568
A21       @1 2011
A23 01      @0 ENG
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A44       @0 0000 @1 © 2011 INIST-CNRS. All rights reserved.
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A47 01  1    @0 11-0260679
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A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 USA
C01 01    ENG  @0 We present the first characterization of a thick-disc component in the Andromeda galaxy (M31) using kinematic data from the DEIMOS instrument on Keck II. Using 21 fields in the south-west of the galaxy, we measure the lag of this component with respect to the thin disc, as well as the dispersion, metallicity and scalelength of the component. We find an average lag between the two components of ?Δù? = 46.0 ± 3.9 km s-1. The velocity dispersion of the thick disc is σthick= 50.8±1.9 km s-1, greater than the value of dispersion we determine for the thin disc, σthin= 35.7 ± 1.0 km s-1. The thick disc is more metal poor than the thin disc, with [Fe/H]spec=-1.0±0.1 compared with [Fe/H]spec=-0.7 ± 0.05 for the thin disc. We measure a radial scalelength of the thin and thick discs of hr = 7.3±1.0 and 8.0 ± 1.2 kpc, respectively. From this, we infer scaleheights for both discs of 1.1±0.2 and 2.8± 0.6 kpc, both of which are approximately two to three times larger than those observed in the Milky Way. We estimate a mass range for the thick-disc component of 2.4 x1010 < M*,thick < 4.1× 1010 M◦.. This value provides a useful constraint on possible formation mechanisms, as any proposed method for forming a thick disc must be able to heat (or deposit) at least this amount of material.
C02 01  3    @0 001E03
C03 01  X  FRE  @0 Cinématique stellaire @5 26
C03 01  X  ENG  @0 Stellar kinematics @5 26
C03 01  X  SPA  @0 Cinematica estelar @5 26
C03 02  3  FRE  @0 Galaxies spirales @5 27
C03 02  3  ENG  @0 Spiral galaxies @5 27
C03 03  3  FRE  @0 Deimos @5 28
C03 03  3  ENG  @0 Deimos @5 28
C03 04  X  FRE  @0 Métallicité @5 29
C03 04  X  ENG  @0 Metallicity @5 29
C03 04  X  SPA  @0 Metalicidad @5 29
C03 05  X  FRE  @0 Dispersion vitesse @5 30
C03 05  X  ENG  @0 Velocity dispersion @5 30
C03 05  X  SPA  @0 Dispersión velocidad @5 30
C03 06  3  FRE  @0 Voie lactée @5 31
C03 06  3  ENG  @0 Milky Way @5 31
C03 07  X  FRE  @0 Mécanisme formation @5 32
C03 07  X  ENG  @0 Formation mechanism @5 32
C03 07  X  SPA  @0 Mecanismo formacion @5 32
C03 08  3  FRE  @0 Dynamique stellaire @5 33
C03 08  3  ENG  @0 Stellar dynamics @5 33
C03 09  3  FRE  @0 Abondance @5 34
C03 09  3  ENG  @0 Abundance @5 34
C03 10  X  FRE  @0 Evolution galaxies @5 35
C03 10  X  ENG  @0 Galaxy evolution @5 35
C03 10  X  SPA  @0 Evolución galaxias @5 35
C03 11  3  FRE  @0 Groupe local @5 36
C03 11  3  ENG  @0 Local group @5 36
C03 12  X  FRE  @0 Structure galaxies @5 37
C03 12  X  ENG  @0 Galaxy structure @5 37
C03 12  X  SPA  @0 Estructura galaxias @5 37
C03 13  X  FRE  @0 Satellite Mars @5 38
C03 13  X  ENG  @0 Mars satellite @5 38
C03 13  X  SPA  @0 Satélite Marte @5 38
N21       @1 178
N44 01      @1 OTO
N82       @1 OTO

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<div type="abstract" xml:lang="en">We present the first characterization of a thick-disc component in the Andromeda galaxy (M31) using kinematic data from the DEIMOS instrument on Keck II. Using 21 fields in the south-west of the galaxy, we measure the lag of this component with respect to the thin disc, as well as the dispersion, metallicity and scalelength of the component. We find an average lag between the two components of ?Δù? = 46.0 ± 3.9 km s
<sup>-1</sup>
. The velocity dispersion of the thick disc is σ
<sub>thick</sub>
= 50.8±1.9 km s
<sup>-1</sup>
, greater than the value of dispersion we determine for the thin disc, σ
<sub>thin</sub>
= 35.7 ± 1.0 km s
<sup>-1</sup>
. The thick disc is more metal poor than the thin disc, with [Fe/H]
<sub>spec</sub>
=-1.0±0.1 compared with [Fe/H]
<sub>spec</sub>
=-0.7 ± 0.05 for the thin disc. We measure a radial scalelength of the thin and thick discs of h
<sub>r</sub>
= 7.3±1.0 and 8.0 ± 1.2 kpc, respectively. From this, we infer scaleheights for both discs of 1.1±0.2 and 2.8± 0.6 kpc, both of which are approximately two to three times larger than those observed in the Milky Way. We estimate a mass range for the thick-disc component of 2.4 x10
<sup>10</sup>
< M
<sub>*,thick</sub>
< 4.1× 10
<sup>10</sup>
M
<sub>◦.</sub>
. This value provides a useful constraint on possible formation mechanisms, as any proposed method for forming a thick disc must be able to heat (or deposit) at least this amount of material.</div>
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<s2>Edinburgh EH9 3HJ</s2>
<s3>USA</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="05">
<s1>Sydney Institute for Astronomy, School of Physics, A29, University of Sydney</s1>
<s2>NSW 2006</s2>
<s3>AUS</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="06">
<s1>Department of Physics & Astronomy, University of Leicester, University Road</s1>
<s2>Leicester LE1 7RH</s2>
<s3>GBR</s3>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA20>
<s1>1548-1568</s1>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000192127200050</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>1 p.1/2</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0260679</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Monthly Notices of the Royal Astronomical Society</s0>
</fA64>
<fA66 i1="01">
<s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>We present the first characterization of a thick-disc component in the Andromeda galaxy (M31) using kinematic data from the DEIMOS instrument on Keck II. Using 21 fields in the south-west of the galaxy, we measure the lag of this component with respect to the thin disc, as well as the dispersion, metallicity and scalelength of the component. We find an average lag between the two components of ?Δù? = 46.0 ± 3.9 km s
<sup>-1</sup>
. The velocity dispersion of the thick disc is σ
<sub>thick</sub>
= 50.8±1.9 km s
<sup>-1</sup>
, greater than the value of dispersion we determine for the thin disc, σ
<sub>thin</sub>
= 35.7 ± 1.0 km s
<sup>-1</sup>
. The thick disc is more metal poor than the thin disc, with [Fe/H]
<sub>spec</sub>
=-1.0±0.1 compared with [Fe/H]
<sub>spec</sub>
=-0.7 ± 0.05 for the thin disc. We measure a radial scalelength of the thin and thick discs of h
<sub>r</sub>
= 7.3±1.0 and 8.0 ± 1.2 kpc, respectively. From this, we infer scaleheights for both discs of 1.1±0.2 and 2.8± 0.6 kpc, both of which are approximately two to three times larger than those observed in the Milky Way. We estimate a mass range for the thick-disc component of 2.4 x10
<sup>10</sup>
< M
<sub>*,thick</sub>
< 4.1× 10
<sup>10</sup>
M
<sub>◦.</sub>
. This value provides a useful constraint on possible formation mechanisms, as any proposed method for forming a thick disc must be able to heat (or deposit) at least this amount of material.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE">
<s0>Cinématique stellaire</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG">
<s0>Stellar kinematics</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA">
<s0>Cinematica estelar</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Galaxies spirales</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Spiral galaxies</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Deimos</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Deimos</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Métallicité</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Metallicity</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Metalicidad</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE">
<s0>Dispersion vitesse</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG">
<s0>Velocity dispersion</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA">
<s0>Dispersión velocidad</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Voie lactée</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG">
<s0>Milky Way</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE">
<s0>Mécanisme formation</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG">
<s0>Formation mechanism</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA">
<s0>Mecanismo formacion</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Dynamique stellaire</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Stellar dynamics</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Abondance</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Abundance</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Evolution galaxies</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Galaxy evolution</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Evolución galaxias</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Groupe local</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Local group</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Structure galaxies</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>Galaxy structure</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Estructura galaxias</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Satellite Mars</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Mars satellite</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Satélite Marte</s0>
<s5>38</s5>
</fC03>
<fN21>
<s1>178</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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