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Asteroseismology of old open clusters with Kepler: direct estimate of the integrated red giant branch mass-loss in NGC 6791 and 6819

Identifieur interne : 004842 ( PascalFrancis/Curation ); précédent : 004841; suivant : 004843

Asteroseismology of old open clusters with Kepler: direct estimate of the integrated red giant branch mass-loss in NGC 6791 and 6819

Auteurs : A. Miglio [Royaume-Uni] ; K. Brogaard [Canada] ; D. Stello [Australie] ; W. J. Chaplin [Royaume-Uni] ; F. D' Antona [Italie] ; J. Montalban [Belgique] ; S. Basu [États-Unis] ; A. Bressan [Italie] ; F. Grundahl [Danemark] ; M. Pinsonneault [États-Unis] ; A. M. Serenelli [Espagne] ; Y. Elsworth [Royaume-Uni] ; S. Hekker [Royaume-Uni, Pays-Bas] ; T. Kallinger [Canada] ; B. Mosser [France] ; P. Ventura [Italie] ; A. Bonanno [Italie] ; A. Noels [Belgique] ; V. Silva Aguirre [Allemagne] ; R. Szabo [Hongrie] ; J. Li [États-Unis] ; S. Mccauliff [États-Unis] ; C. K. Middour [États-Unis] ; H. Kjeldsen [Danemark]

Source :

RBID : Pascal:12-0049842

Descripteurs français

English descriptors

Abstract

Mass-loss of red giant branch (RGB) stars is still poorly determined, despite its crucial role in the chemical enrichment of galaxies. Thanks to the recent detection of solar-like oscillations in G-K giants in open clusters with Kepler, we can now directly determine stellar masses for a statistically significant sample of stars in the old open clusters NGC 6791 and 6819. The aim of this work is to constrain the integrated RGB mass-loss by comparing the average mass of stars in the red clump (RC) with that of stars in the low-luminosity portion of the RGB [i.e. stars with L ? L(RC)]. Stellar masses were determined by combining the available seismic parameters vmax and Δv with additional photometric constraints and with independent distance estimates. We measured the masses of 40 stars on the RGB and 19 in the RC of the old metal-rich cluster NGC 6791. We find that the difference between the average mass of RGB and RC stars is small, but significant [ΔM? = 0.09 ± 0.03 (random) ±0.04 (systematic) M◦.]. Interestingly, such a small ΔM? does not support scenarios of an extreme mass-loss for this metal-rich cluster. If we describe the mass-loss rate with Reimers prescription, a first comparison with isochrones suggests that the observed AM? is compatible with a mass-loss efficiency parameter in the range 0.1 ? η ? 0.3. Less stringent constraints on the RGB mass-loss rate are set by the analysis of the ˜2 Gyr old NGC 6819, largely due to the lower mass-loss expected for this cluster, and to the lack of an independent and accurate distance determination. In the near future, additional constraints from frequencies of individual pulsation modes and spectroscopic effective temperatures will allow further stringent tests of the Δv and vmax scaling relations, which provide a novel, and potentially very accurate, means of determining stellar radii and masses.
pA  
A01 01  1    @0 0035-8711
A02 01      @0 MNRAA4
A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 419
A06       @2 3
A08 01  1  ENG  @1 Asteroseismology of old open clusters with Kepler: direct estimate of the integrated red giant branch mass-loss in NGC 6791 and 6819
A11 01  1    @1 MIGLIO (A.)
A11 02  1    @1 BROGAARD (K.)
A11 03  1    @1 STELLO (D.)
A11 04  1    @1 CHAPLIN (W. J.)
A11 05  1    @1 ANTONA (F. D')
A11 06  1    @1 MONTALBAN (J.)
A11 07  1    @1 BASU (S.)
A11 08  1    @1 BRESSAN (A.)
A11 09  1    @1 GRUNDAHL (F.)
A11 10  1    @1 PINSONNEAULT (M.)
A11 11  1    @1 SERENELLI (A. M.)
A11 12  1    @1 ELSWORTH (Y.)
A11 13  1    @1 HEKKER (S.)
A11 14  1    @1 KALLINGER (T.)
A11 15  1    @1 MOSSER (B.)
A11 16  1    @1 VENTURA (P.)
A11 17  1    @1 BONANNO (A.)
A11 18  1    @1 NOELS (A.)
A11 19  1    @1 SILVA AGUIRRE (V.)
A11 20  1    @1 SZABO (R.)
A11 21  1    @1 LI (J.)
A11 22  1    @1 MCCAULIFF (S.)
A11 23  1    @1 MIDDOUR (C. K.)
A11 24  1    @1 KJELDSEN (H.)
A14 01      @1 School of Physics and Astronomy, University of Birmingham @2 Edgbaston, Birmingham B15 2TT @3 GBR @Z 1 aut. @Z 4 aut. @Z 12 aut. @Z 13 aut.
A14 02      @1 Department of Physics and Astronomy, University of Victoria, PO Box 3055 @2 Victoria, BC V8W 3P6 @3 CAN @Z 2 aut.
A14 03      @1 Sydney Institute for Astronomy (SIfA), School of Physics, University of Sydney @2 NSW 2006 @3 AUS @Z 3 aut.
A14 04      @1 INAF - Osservatorio Astronomico di Roma, via Frascati 33, Monteporzio Catone (RM @3 ITA @Z 5 aut. @Z 16 aut.
A14 05      @1 Institut d'Astrophysique et de Géophysique de l'Université de Liège, Allée du 6 Août, 17 @2 4000 Liège @3 BEL @Z 6 aut. @Z 18 aut.
A14 06      @1 Department of Astronomy, Yale University, PO Box 208101 @2 New Haven, CT 06520-8101 @3 USA @Z 7 aut.
A14 07      @1 SISSA, via Bonomea 265 @2 34136 Trieste @3 ITA @Z 8 aut.
A14 08      @1 INAF - Osservatorio Astronomico di Padova, Vicolo dell'Osservatorio 5 @2 35122 Padova @3 ITA @Z 8 aut.
A14 09      @1 Department of Physics and Astronomy, Building 1520, Aarhus University @2 8000 Aarhus @3 DNK @Z 9 aut. @Z 24 aut.
A14 10      @1 Department of Astronomy, Ohio State University, 140 West 18th Avenue @2 Columbus, OH 43210 @3 USA @Z 10 aut.
A14 11      @1 Institute for Space Sciences (CSIC-IEEC), Facultad de Ciencies, Campus UAB @2 08193 Bellaterra @3 ESP @Z 11 aut.
A14 12      @1 Astronomical Institute Anton Pannekoek, University of Amsterdam, Science Park 904 @2 1098 XH Amsterdam @3 NLD @Z 13 aut.
A14 13      @1 Department of Physics and Astronomy, University of British Colombia, 6224 Agricultural Road @2 Vancouver, BC V6T 1Z1 @3 CAN @Z 14 aut.
A14 14      @1 LESIA, CNRS, Université Pierre et Marie Curie, Université Denis Diderot, Observatoire de Paris @2 92195 Meudon @3 FRA @Z 15 aut.
A14 15      @1 INAF - Osservatorio Astrofisico di Catania, Via S.Sofia 78 @2 95123 Catania @3 ITA @Z 17 aut.
A14 16      @1 Max Planck Institute for Astrophysics, Karl-Schwarzschild-Str. 1 @2 85748 Garching bei München @3 DEU @Z 19 aut.
A14 17      @1 Konkoly Observatory of the Hungarian Academy of Sciences, Konkoly Thege Miklos út 15-17 @2 1121 Budapest @3 HUN @Z 20 aut.
A14 18      @1 SETI Institute/NASA Ames Research Center @2 Moffett Field, CA 94035 @3 USA @Z 21 aut.
A14 19      @1 Orbital Sciences Corporation/NASA Ames Research Center @2 Moffett Field, CA 94035 @3 USA @Z 22 aut. @Z 23 aut.
A20       @1 2077-2088
A21       @1 2012
A23 01      @0 ENG
A43 01      @1 INIST @2 2067 @5 354000506062930180
A44       @0 0000 @1 © 2012 INIST-CNRS. All rights reserved.
A45       @0 3/4 p.
A47 01  1    @0 12-0049842
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 Mass-loss of red giant branch (RGB) stars is still poorly determined, despite its crucial role in the chemical enrichment of galaxies. Thanks to the recent detection of solar-like oscillations in G-K giants in open clusters with Kepler, we can now directly determine stellar masses for a statistically significant sample of stars in the old open clusters NGC 6791 and 6819. The aim of this work is to constrain the integrated RGB mass-loss by comparing the average mass of stars in the red clump (RC) with that of stars in the low-luminosity portion of the RGB [i.e. stars with L ? L(RC)]. Stellar masses were determined by combining the available seismic parameters vmax and Δv with additional photometric constraints and with independent distance estimates. We measured the masses of 40 stars on the RGB and 19 in the RC of the old metal-rich cluster NGC 6791. We find that the difference between the average mass of RGB and RC stars is small, but significant [ΔM? = 0.09 ± 0.03 (random) ±0.04 (systematic) M◦.]. Interestingly, such a small ΔM? does not support scenarios of an extreme mass-loss for this metal-rich cluster. If we describe the mass-loss rate with Reimers prescription, a first comparison with isochrones suggests that the observed AM? is compatible with a mass-loss efficiency parameter in the range 0.1 ? η ? 0.3. Less stringent constraints on the RGB mass-loss rate are set by the analysis of the ˜2 Gyr old NGC 6819, largely due to the lower mass-loss expected for this cluster, and to the lack of an independent and accurate distance determination. In the near future, additional constraints from frequencies of individual pulsation modes and spectroscopic effective temperatures will allow further stringent tests of the Δv and vmax scaling relations, which provide a novel, and potentially very accurate, means of determining stellar radii and masses.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Astéroséismologie @5 26
C03 01  3  ENG  @0 Astroseismology @5 26
C03 02  3  FRE  @0 Amas ouvert @5 27
C03 02  3  ENG  @0 Open clusters @5 27
C03 03  3  FRE  @0 Géante rouge @5 28
C03 03  3  ENG  @0 Red giant stars @5 28
C03 04  3  FRE  @0 Perte masse @5 29
C03 04  3  ENG  @0 Mass loss @5 29
C03 05  3  FRE  @0 Etoile géante @5 30
C03 05  3  ENG  @0 Giant stars @5 30
C03 06  X  FRE  @0 Enrichissement chimique @5 31
C03 06  X  ENG  @0 Chemical enrichment @5 31
C03 06  X  SPA  @0 Enriquecimiento químico @5 31
C03 07  3  FRE  @0 Galaxies @5 32
C03 07  3  ENG  @0 Galaxies @5 32
C03 08  3  FRE  @0 Masse stellaire @5 33
C03 08  3  ENG  @0 Stellar mass @5 33
C03 09  3  FRE  @0 Luminosité @5 34
C03 09  3  ENG  @0 Luminosity @5 34
C03 10  X  FRE  @0 Taux perte @5 35
C03 10  X  ENG  @0 Loss rate @5 35
C03 10  X  SPA  @0 Porcentaje pérdida @5 35
C03 11  X  FRE  @0 Isochrone @5 36
C03 11  X  ENG  @0 Isochrone @5 36
C03 11  X  SPA  @0 Isocrono @5 36
C03 12  3  FRE  @0 Mesure distance @5 37
C03 12  3  ENG  @0 Distance measurement @5 37
C03 13  3  FRE  @0 Température effective @5 38
C03 13  3  ENG  @0 Effective temperature @5 38
C03 14  3  FRE  @0 Etoile type avancé @5 39
C03 14  3  ENG  @0 Late type stars @5 39
C03 15  3  FRE  @0 Amas stellaire @5 40
C03 15  3  ENG  @0 Star clusters @5 40
N21       @1 030
N44 01      @1 OTO
N82       @1 OTO

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Le document en format XML

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<name sortKey="Ventura, P" sort="Ventura, P" uniqKey="Ventura P" first="P." last="Ventura">P. Ventura</name>
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<name sortKey="Bonanno, A" sort="Bonanno, A" uniqKey="Bonanno A" first="A." last="Bonanno">A. Bonanno</name>
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<name sortKey="Silva Aguirre, V" sort="Silva Aguirre, V" uniqKey="Silva Aguirre V" first="V." last="Silva Aguirre">V. Silva Aguirre</name>
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<name sortKey="Szabo, R" sort="Szabo, R" uniqKey="Szabo R" first="R." last="Szabo">R. Szabo</name>
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<name sortKey="Mccauliff, S" sort="Mccauliff, S" uniqKey="Mccauliff S" first="S." last="Mccauliff">S. Mccauliff</name>
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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>
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<date when="2012">2012</date>
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<keywords scheme="KwdEn" xml:lang="en">
<term>Astroseismology</term>
<term>Chemical enrichment</term>
<term>Distance measurement</term>
<term>Effective temperature</term>
<term>Galaxies</term>
<term>Giant stars</term>
<term>Isochrone</term>
<term>Late type stars</term>
<term>Loss rate</term>
<term>Luminosity</term>
<term>Mass loss</term>
<term>Open clusters</term>
<term>Red giant stars</term>
<term>Star clusters</term>
<term>Stellar mass</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Astéroséismologie</term>
<term>Amas ouvert</term>
<term>Géante rouge</term>
<term>Perte masse</term>
<term>Etoile géante</term>
<term>Enrichissement chimique</term>
<term>Galaxies</term>
<term>Masse stellaire</term>
<term>Luminosité</term>
<term>Taux perte</term>
<term>Isochrone</term>
<term>Mesure distance</term>
<term>Température effective</term>
<term>Etoile type avancé</term>
<term>Amas stellaire</term>
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<front>
<div type="abstract" xml:lang="en">Mass-loss of red giant branch (RGB) stars is still poorly determined, despite its crucial role in the chemical enrichment of galaxies. Thanks to the recent detection of solar-like oscillations in G-K giants in open clusters with Kepler, we can now directly determine stellar masses for a statistically significant sample of stars in the old open clusters NGC 6791 and 6819. The aim of this work is to constrain the integrated RGB mass-loss by comparing the average mass of stars in the red clump (RC) with that of stars in the low-luminosity portion of the RGB [i.e. stars with L ? L(RC)]. Stellar masses were determined by combining the available seismic parameters v
<sub>max</sub>
and Δv with additional photometric constraints and with independent distance estimates. We measured the masses of 40 stars on the RGB and 19 in the RC of the old metal-rich cluster NGC 6791. We find that the difference between the average mass of RGB and RC stars is small, but significant [ΔM? = 0.09 ± 0.03 (random) ±0.04 (systematic) M
<sub>◦.</sub>
]. Interestingly, such a small ΔM? does not support scenarios of an extreme mass-loss for this metal-rich cluster. If we describe the mass-loss rate with Reimers prescription, a first comparison with isochrones suggests that the observed AM? is compatible with a mass-loss efficiency parameter in the range 0.1 ? η ? 0.3. Less stringent constraints on the RGB mass-loss rate are set by the analysis of the ˜2 Gyr old NGC 6819, largely due to the lower mass-loss expected for this cluster, and to the lack of an independent and accurate distance determination. In the near future, additional constraints from frequencies of individual pulsation modes and spectroscopic effective temperatures will allow further stringent tests of the Δv and v
<sub>max</sub>
scaling relations, which provide a novel, and potentially very accurate, means of determining stellar radii and masses.</div>
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<s1>Institut d'Astrophysique et de Géophysique de l'Université de Liège, Allée du 6 Août, 17</s1>
<s2>4000 Liège</s2>
<s3>BEL</s3>
<sZ>6 aut.</sZ>
<sZ>18 aut.</sZ>
</fA14>
<fA14 i1="06">
<s1>Department of Astronomy, Yale University, PO Box 208101</s1>
<s2>New Haven, CT 06520-8101</s2>
<s3>USA</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="07">
<s1>SISSA, via Bonomea 265</s1>
<s2>34136 Trieste</s2>
<s3>ITA</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="08">
<s1>INAF - Osservatorio Astronomico di Padova, Vicolo dell'Osservatorio 5</s1>
<s2>35122 Padova</s2>
<s3>ITA</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="09">
<s1>Department of Physics and Astronomy, Building 1520, Aarhus University</s1>
<s2>8000 Aarhus</s2>
<s3>DNK</s3>
<sZ>9 aut.</sZ>
<sZ>24 aut.</sZ>
</fA14>
<fA14 i1="10">
<s1>Department of Astronomy, Ohio State University, 140 West 18th Avenue</s1>
<s2>Columbus, OH 43210</s2>
<s3>USA</s3>
<sZ>10 aut.</sZ>
</fA14>
<fA14 i1="11">
<s1>Institute for Space Sciences (CSIC-IEEC), Facultad de Ciencies, Campus UAB</s1>
<s2>08193 Bellaterra</s2>
<s3>ESP</s3>
<sZ>11 aut.</sZ>
</fA14>
<fA14 i1="12">
<s1>Astronomical Institute Anton Pannekoek, University of Amsterdam, Science Park 904</s1>
<s2>1098 XH Amsterdam</s2>
<s3>NLD</s3>
<sZ>13 aut.</sZ>
</fA14>
<fA14 i1="13">
<s1>Department of Physics and Astronomy, University of British Colombia, 6224 Agricultural Road</s1>
<s2>Vancouver, BC V6T 1Z1</s2>
<s3>CAN</s3>
<sZ>14 aut.</sZ>
</fA14>
<fA14 i1="14">
<s1>LESIA, CNRS, Université Pierre et Marie Curie, Université Denis Diderot, Observatoire de Paris</s1>
<s2>92195 Meudon</s2>
<s3>FRA</s3>
<sZ>15 aut.</sZ>
</fA14>
<fA14 i1="15">
<s1>INAF - Osservatorio Astrofisico di Catania, Via S.Sofia 78</s1>
<s2>95123 Catania</s2>
<s3>ITA</s3>
<sZ>17 aut.</sZ>
</fA14>
<fA14 i1="16">
<s1>Max Planck Institute for Astrophysics, Karl-Schwarzschild-Str. 1</s1>
<s2>85748 Garching bei München</s2>
<s3>DEU</s3>
<sZ>19 aut.</sZ>
</fA14>
<fA14 i1="17">
<s1>Konkoly Observatory of the Hungarian Academy of Sciences, Konkoly Thege Miklos út 15-17</s1>
<s2>1121 Budapest</s2>
<s3>HUN</s3>
<sZ>20 aut.</sZ>
</fA14>
<fA14 i1="18">
<s1>SETI Institute/NASA Ames Research Center</s1>
<s2>Moffett Field, CA 94035</s2>
<s3>USA</s3>
<sZ>21 aut.</sZ>
</fA14>
<fA14 i1="19">
<s1>Orbital Sciences Corporation/NASA Ames Research Center</s1>
<s2>Moffett Field, CA 94035</s2>
<s3>USA</s3>
<sZ>22 aut.</sZ>
<sZ>23 aut.</sZ>
</fA14>
<fA20>
<s1>2077-2088</s1>
</fA20>
<fA21>
<s1>2012</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000506062930180</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>3/4 p.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>12-0049842</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>Mass-loss of red giant branch (RGB) stars is still poorly determined, despite its crucial role in the chemical enrichment of galaxies. Thanks to the recent detection of solar-like oscillations in G-K giants in open clusters with Kepler, we can now directly determine stellar masses for a statistically significant sample of stars in the old open clusters NGC 6791 and 6819. The aim of this work is to constrain the integrated RGB mass-loss by comparing the average mass of stars in the red clump (RC) with that of stars in the low-luminosity portion of the RGB [i.e. stars with L ? L(RC)]. Stellar masses were determined by combining the available seismic parameters v
<sub>max</sub>
and Δv with additional photometric constraints and with independent distance estimates. We measured the masses of 40 stars on the RGB and 19 in the RC of the old metal-rich cluster NGC 6791. We find that the difference between the average mass of RGB and RC stars is small, but significant [ΔM? = 0.09 ± 0.03 (random) ±0.04 (systematic) M
<sub>◦.</sub>
]. Interestingly, such a small ΔM? does not support scenarios of an extreme mass-loss for this metal-rich cluster. If we describe the mass-loss rate with Reimers prescription, a first comparison with isochrones suggests that the observed AM? is compatible with a mass-loss efficiency parameter in the range 0.1 ? η ? 0.3. Less stringent constraints on the RGB mass-loss rate are set by the analysis of the ˜2 Gyr old NGC 6819, largely due to the lower mass-loss expected for this cluster, and to the lack of an independent and accurate distance determination. In the near future, additional constraints from frequencies of individual pulsation modes and spectroscopic effective temperatures will allow further stringent tests of the Δv and v
<sub>max</sub>
scaling relations, which provide a novel, and potentially very accurate, means of determining stellar radii and masses.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Astéroséismologie</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Astroseismology</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Amas ouvert</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Open clusters</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Géante rouge</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Red giant stars</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Perte masse</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Mass loss</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Etoile géante</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Giant stars</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Enrichissement chimique</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Chemical enrichment</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Enriquecimiento químico</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Galaxies</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Galaxies</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Masse stellaire</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Stellar mass</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Luminosité</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Luminosity</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Taux perte</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Loss rate</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Porcentaje pérdida</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE">
<s0>Isochrone</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG">
<s0>Isochrone</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA">
<s0>Isocrono</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Mesure distance</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Distance measurement</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Température effective</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Effective temperature</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Etoile type avancé</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Late type stars</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Amas stellaire</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Star clusters</s0>
<s5>40</s5>
</fC03>
<fN21>
<s1>030</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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   |texte=   Asteroseismology of old open clusters with Kepler: direct estimate of the integrated red giant branch mass-loss in NGC 6791 and 6819
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