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Solar-like oscillations from the depths of the red-giant star KIC 4351319 observed with Kepler

Identifieur interne : 004503 ( PascalFrancis/Curation ); précédent : 004502; suivant : 004504

Solar-like oscillations from the depths of the red-giant star KIC 4351319 observed with Kepler

Auteurs : M. P. Di Mauro [Italie] ; D. Cardini [Italie] ; G. Catanzaro [Italie] ; R. Ventura [Italie] ; C. Barban [France] ; T. R. Bedding [Australie] ; J. Christensen-Dalsgaard [Danemark] ; J. De Ridder [Belgique] ; S. Hekker [Royaume-Uni, Pays-Bas] ; D. Huber [Australie] ; T. Kallinger [Canada, Autriche] ; A. Miglio [Royaume-Uni, Belgique] ; J. Montalban [Belgique] ; B. Mosser [France] ; D. Stello [Australie] ; K. Uytterhoeven [France, Allemagne] ; K. Kinemuchi [États-Unis] ; H. Kjeldsen [Danemark] ; F. Mullally [États-Unis] ; M. Still [États-Unis]

Source :

RBID : Pascal:11-0372382

Descripteurs français

English descriptors

Abstract

We present the results of the asteroseismic analysis of the red-giant star KIC 4351319 (TYC 3124-914-1), observed for 30d in short-cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Δν0 = 24.6 ± 0.2 μHz and δν02 = 2.2 ± 0.3 μHz, respectively, and the frequency of maximum oscillation power, νmax = 386.5 ± 4.0 μHz. The high signal-to-noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to 500 μHz. The observed oscillation frequencies together with the accurate determination of the atmospheric parameters (effective temperature, gravity and metallicity), provided by additional ground-based spectroscopic observations, enabled us to theoretically interpret the observed oscillation spectrum. KIC 4351319 appears to oscillate with a well-defined solar-type p-mode pattern due to radial acoustic modes and non-radial nearly pure p modes. In addition, several non-radial mixed modes have been identified. Theoretical models well reproduce the observed oscillation frequencies and indicate that this star, located at the base of the ascending red-giant branch, is in the hydrogen-shell-burning phase, with a mass of ∼1.3M◦., a radius of ∼3.4R◦. and an age of ∼5.6 Gyr. The main parameters of this star have been determined with an unprecedented level of precision for a red-giant star, with uncertainties of 2 per cent for mass, 7 per cent for age, 1 per cent for radius and 4 per cent for luminosity.
pA  
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A02 01      @0 MNRAA4
A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 415
A06       @2 4
A08 01  1  ENG  @1 Solar-like oscillations from the depths of the red-giant star KIC 4351319 observed with Kepler
A11 01  1    @1 DI MAURO (M. P.)
A11 02  1    @1 CARDINI (D.)
A11 03  1    @1 CATANZARO (G.)
A11 04  1    @1 VENTURA (R.)
A11 05  1    @1 BARBAN (C.)
A11 06  1    @1 BEDDING (T. R.)
A11 07  1    @1 CHRISTENSEN-DALSGAARD (J.)
A11 08  1    @1 DE RIDDER (J.)
A11 09  1    @1 HEKKER (S.)
A11 10  1    @1 HUBER (D.)
A11 11  1    @1 KALLINGER (T.)
A11 12  1    @1 MIGLIO (A.)
A11 13  1    @1 MONTALBAN (J.)
A11 14  1    @1 MOSSER (B.)
A11 15  1    @1 STELLO (D.)
A11 16  1    @1 UYTTERHOEVEN (K.)
A11 17  1    @1 KINEMUCHI (K.)
A11 18  1    @1 KJELDSEN (H.)
A11 19  1    @1 MULLALLY (F.)
A11 20  1    @1 STILL (M.)
A14 01      @1 INAF - IASF, Istituto di Astrofisíca Spaziale e Fisica Cosmica, Via del Fosso del Cavaliere 100 @2 00133 Roma @3 ITA @Z 1 aut. @Z 2 aut.
A14 02      @1 INAF - Osservatorio Astrofisico di Catania, Via S. Sofia 78 @2 95123 Catania @3 ITA @Z 3 aut. @Z 4 aut.
A14 03      @1 LESIA, CNRS, Université Pierre et Marie Curie, Université Denis, Diderot, Observatoire de Paris @2 92195 Meudon @3 FRA @Z 5 aut. @Z 14 aut.
A14 04      @1 Sydney Institute for Astronomy (SIfA), School of Physics, University of Sydney @2 NSW 2006 @3 AUS @Z 6 aut. @Z 10 aut. @Z 15 aut.
A14 05      @1 Institutfor Fysik og Astronomi, Bygn. 1520, Aarhus Universitet, Ny Munkegade @2 8000 Aarhus C @3 DNK @Z 7 aut. @Z 18 aut.
A14 06      @1 Institut voor Sterrenkunde, K. U. Leuven, Celestijnenlaan 200D @2 3001 Leuven @3 BEL @Z 8 aut.
A14 07      @1 School of Physics and Astronomy, University of Birmingham @2 Birmingham B15 2TT @3 GBR @Z 9 aut. @Z 12 aut.
A14 08      @1 Astronomical Institute 'Anton Pannekoek', University of Amsterdam, Science Park 904 @2 1098 XH Amsterdam @3 NLD @Z 9 aut.
A14 09      @1 Department of Physics and Astronomy, University of British Columbia @2 Vancouver @3 CAN @Z 11 aut.
A14 10      @1 Institute of Astronomy, University of Vienna @2 1180 Vienna @3 AUT @Z 11 aut.
A14 11      @1 Institut d'Astrophysique et de Géofisique de l'Universitè de Liège, Allè du 6 Aout 17-B 4000 Liège @3 BEL @Z 12 aut. @Z 13 aut.
A14 12      @1 Laboratoire AIM, CEA/DSM-CNRS-Université Paris Diderot, CEA, IRFU, SAp, Centre de Saclay @2 91191 Gif-sur-Yvette @3 FRA @Z 16 aut.
A14 13      @1 Kiepenheuer-Institut für Sonnenphysik, Schöneckstrasse 6, 79104 Freiburg im Breisgau @3 DEU @Z 16 aut.
A14 14      @1 Bay Area Environmental Research Institute/NASA Ames Research Center, Moffett Field @2 CA 94035 @3 USA @Z 17 aut. @Z 20 aut.
A14 15      @1 SETI Institute/NASA Ames Research Center, Moffett Field @2 CA 94035 @3 USA @Z 19 aut.
A20       @1 3783-3797
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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A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 USA
C01 01    ENG  @0 We present the results of the asteroseismic analysis of the red-giant star KIC 4351319 (TYC 3124-914-1), observed for 30d in short-cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Δν0 = 24.6 ± 0.2 μHz and δν02 = 2.2 ± 0.3 μHz, respectively, and the frequency of maximum oscillation power, νmax = 386.5 ± 4.0 μHz. The high signal-to-noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to 500 μHz. The observed oscillation frequencies together with the accurate determination of the atmospheric parameters (effective temperature, gravity and metallicity), provided by additional ground-based spectroscopic observations, enabled us to theoretically interpret the observed oscillation spectrum. KIC 4351319 appears to oscillate with a well-defined solar-type p-mode pattern due to radial acoustic modes and non-radial nearly pure p modes. In addition, several non-radial mixed modes have been identified. Theoretical models well reproduce the observed oscillation frequencies and indicate that this star, located at the base of the ascending red-giant branch, is in the hydrogen-shell-burning phase, with a mass of ∼1.3M◦., a radius of ∼3.4R◦. and an age of ∼5.6 Gyr. The main parameters of this star have been determined with an unprecedented level of precision for a red-giant star, with uncertainties of 2 per cent for mass, 7 per cent for age, 1 per cent for radius and 4 per cent for luminosity.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Etoile rouge @5 26
C03 01  3  ENG  @0 Red stars @5 26
C03 02  3  FRE  @0 Géante rouge @5 27
C03 02  3  ENG  @0 Red giant stars @5 27
C03 03  3  FRE  @0 Etoile géante @5 28
C03 03  3  ENG  @0 Giant stars @5 28
C03 04  X  FRE  @0 Satellite Kepler @5 29
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C03 05  3  FRE  @0 Rapport signal bruit @5 30
C03 05  3  ENG  @0 Signal-to-noise ratio @5 30
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C03 06  X  ENG  @0 Oscillation frequency @5 31
C03 06  X  SPA  @0 Frecuencia oscilación @5 31
C03 07  3  FRE  @0 Température atmosphérique @5 32
C03 07  3  ENG  @0 Atmospheric temperature @5 32
C03 08  3  FRE  @0 Température effective @5 33
C03 08  3  ENG  @0 Effective temperature @5 33
C03 09  3  FRE  @0 Gravité @5 34
C03 09  3  ENG  @0 Gravity @5 34
C03 10  X  FRE  @0 Métallicité @5 35
C03 10  X  ENG  @0 Metallicity @5 35
C03 10  X  SPA  @0 Metalicidad @5 35
C03 11  X  FRE  @0 Observation spectroscopique @5 36
C03 11  X  ENG  @0 Spectroscopical observation @5 36
C03 11  X  SPA  @0 Observación espectroscópica @5 36
C03 12  X  FRE  @0 Mode p @5 37
C03 12  X  ENG  @0 p mode @5 37
C03 12  X  SPA  @0 Modo p @5 37
C03 13  X  FRE  @0 Modèle théorique @5 38
C03 13  X  ENG  @0 Theoretical model @5 38
C03 13  X  SPA  @0 Modelo teórico @5 38
C03 14  3  FRE  @0 Combustion hydrogène @5 39
C03 14  3  ENG  @0 Hydrogen burning @5 39
C03 15  X  FRE  @0 Age @5 40
C03 15  X  ENG  @0 Age @5 40
C03 15  X  SPA  @0 Edad @5 40
C03 16  X  FRE  @0 Incertitude @5 41
C03 16  X  ENG  @0 Uncertainty @5 41
C03 16  X  SPA  @0 Incertidumbre @5 41
C03 17  3  FRE  @0 Luminosité @5 42
C03 17  3  ENG  @0 Luminosity @5 42
C03 18  X  FRE  @0 Branche géante asymptotique @5 43
C03 18  X  ENG  @0 Asymptotic giant branch @5 43
C03 18  X  SPA  @0 Rama gigante asintótica @5 43
C03 19  3  FRE  @0 Evolution stellaire @5 44
C03 19  3  ENG  @0 Stellar evolution @5 44
C03 20  X  FRE  @0 Etoile type solaire @5 45
C03 20  X  ENG  @0 Solar type star @5 45
C03 20  X  SPA  @0 Estrella tipo solar @5 45
N21       @1 255
N44 01      @1 OTO
N82       @1 OTO

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Pascal:11-0372382

Le document en format XML

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<name sortKey="Stello, D" sort="Stello, D" uniqKey="Stello D" first="D." last="Stello">D. Stello</name>
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<name sortKey="Kinemuchi, K" sort="Kinemuchi, K" uniqKey="Kinemuchi K" first="K." last="Kinemuchi">K. Kinemuchi</name>
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<term>Age</term>
<term>Asymptotic giant branch</term>
<term>Atmospheric temperature</term>
<term>Effective temperature</term>
<term>Giant stars</term>
<term>Gravity</term>
<term>Hydrogen burning</term>
<term>Kepler satellite</term>
<term>Luminosity</term>
<term>Metallicity</term>
<term>Oscillation frequency</term>
<term>Red giant stars</term>
<term>Red stars</term>
<term>Signal-to-noise ratio</term>
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<term>Etoile rouge</term>
<term>Géante rouge</term>
<term>Etoile géante</term>
<term>Satellite Kepler</term>
<term>Rapport signal bruit</term>
<term>Fréquence oscillation</term>
<term>Température atmosphérique</term>
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<term>Modèle théorique</term>
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<div type="abstract" xml:lang="en">We present the results of the asteroseismic analysis of the red-giant star KIC 4351319 (TYC 3124-914-1), observed for 30d in short-cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Δν0 = 24.6 ± 0.2 μHz and δν02 = 2.2 ± 0.3 μHz, respectively, and the frequency of maximum oscillation power, νmax = 386.5 ± 4.0 μHz. The high signal-to-noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to 500 μHz. The observed oscillation frequencies together with the accurate determination of the atmospheric parameters (effective temperature, gravity and metallicity), provided by additional ground-based spectroscopic observations, enabled us to theoretically interpret the observed oscillation spectrum. KIC 4351319 appears to oscillate with a well-defined solar-type p-mode pattern due to radial acoustic modes and non-radial nearly pure p modes. In addition, several non-radial mixed modes have been identified. Theoretical models well reproduce the observed oscillation frequencies and indicate that this star, located at the base of the ascending red-giant branch, is in the hydrogen-shell-burning phase, with a mass of ∼1.3M◦., a radius of ∼3.4R◦. and an age of ∼5.6 Gyr. The main parameters of this star have been determined with an unprecedented level of precision for a red-giant star, with uncertainties of 2 per cent for mass, 7 per cent for age, 1 per cent for radius and 4 per cent for luminosity.</div>
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<s2>CA 94035</s2>
<s3>USA</s3>
<sZ>17 aut.</sZ>
<sZ>20 aut.</sZ>
</fA14>
<fA14 i1="15">
<s1>SETI Institute/NASA Ames Research Center, Moffett Field</s1>
<s2>CA 94035</s2>
<s3>USA</s3>
<sZ>19 aut.</sZ>
</fA14>
<fA20>
<s1>3783-3797</s1>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000508919600700</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>1 p.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0372382</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 results of the asteroseismic analysis of the red-giant star KIC 4351319 (TYC 3124-914-1), observed for 30d in short-cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Δν0 = 24.6 ± 0.2 μHz and δν02 = 2.2 ± 0.3 μHz, respectively, and the frequency of maximum oscillation power, νmax = 386.5 ± 4.0 μHz. The high signal-to-noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to 500 μHz. The observed oscillation frequencies together with the accurate determination of the atmospheric parameters (effective temperature, gravity and metallicity), provided by additional ground-based spectroscopic observations, enabled us to theoretically interpret the observed oscillation spectrum. KIC 4351319 appears to oscillate with a well-defined solar-type p-mode pattern due to radial acoustic modes and non-radial nearly pure p modes. In addition, several non-radial mixed modes have been identified. Theoretical models well reproduce the observed oscillation frequencies and indicate that this star, located at the base of the ascending red-giant branch, is in the hydrogen-shell-burning phase, with a mass of ∼1.3M◦., a radius of ∼3.4R◦. and an age of ∼5.6 Gyr. The main parameters of this star have been determined with an unprecedented level of precision for a red-giant star, with uncertainties of 2 per cent for mass, 7 per cent for age, 1 per cent for radius and 4 per cent for luminosity.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Etoile rouge</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Red stars</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Géante rouge</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Red giant stars</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Etoile géante</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Giant stars</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Satellite Kepler</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Kepler satellite</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Satélite Kepler</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Rapport signal bruit</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Signal-to-noise ratio</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Fréquence oscillation</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Oscillation frequency</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Frecuencia oscilación</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Température atmosphérique</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Atmospheric temperature</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Température effective</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Effective temperature</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Gravité</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Gravity</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Métallicité</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Metallicity</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Metalicidad</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE">
<s0>Observation spectroscopique</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG">
<s0>Spectroscopical observation</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA">
<s0>Observación espectroscópica</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Mode p</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>p mode</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Modo p</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Modèle théorique</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Theoretical model</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Modelo teórico</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Combustion hydrogène</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Hydrogen burning</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE">
<s0>Age</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG">
<s0>Age</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA">
<s0>Edad</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE">
<s0>Incertitude</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG">
<s0>Uncertainty</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA">
<s0>Incertidumbre</s0>
<s5>41</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Luminosité</s0>
<s5>42</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG">
<s0>Luminosity</s0>
<s5>42</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE">
<s0>Branche géante asymptotique</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="ENG">
<s0>Asymptotic giant branch</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="SPA">
<s0>Rama gigante asintótica</s0>
<s5>43</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE">
<s0>Evolution stellaire</s0>
<s5>44</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG">
<s0>Stellar evolution</s0>
<s5>44</s5>
</fC03>
<fC03 i1="20" i2="X" l="FRE">
<s0>Etoile type solaire</s0>
<s5>45</s5>
</fC03>
<fC03 i1="20" i2="X" l="ENG">
<s0>Solar type star</s0>
<s5>45</s5>
</fC03>
<fC03 i1="20" i2="X" l="SPA">
<s0>Estrella tipo solar</s0>
<s5>45</s5>
</fC03>
<fN21>
<s1>255</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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   |wiki=    Wicri/Asie
   |area=    AustralieFrV1
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   |texte=   Solar-like oscillations from the depths of the red-giant star KIC 4351319 observed with Kepler
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