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

Identifieur interne : 000149 ( Istex/Corpus ); précédent : 000148; suivant : 000150

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

Auteurs : M. P. Di Mauro ; D. Cardini ; G. Catanzaro ; R. Ventura ; C. Barban ; T. R. Bedding ; J. Christensen-Dalsgaard ; J. De Ridder ; S. Hekker ; D. Huber ; T. Kallinger ; A. Miglio ; J. Montalban ; B. Mosser ; D. Stello ; K. Uytterhoeven ; K. Kinemuchi ; H. Kjeldsen ; F. Mullally ; M. Still

Source :

RBID : ISTEX:07BE3F2CCF5C06BE96E33B9BFBA85A834D23251C

English descriptors

Abstract

We present the results of the asteroseismic analysis of the red‐giant star KIC 4351319 (TYC 3124‐914‐1), observed for 30 d in short‐cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Hz and Hz, respectively, and the frequency of maximum oscillation power, Hz. The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to Hz. 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 ∼1.3 M⊙, a radius of 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.

Url:
DOI: 10.1111/j.1365-2966.2011.18996.x

Links to Exploration step

ISTEX:07BE3F2CCF5C06BE96E33B9BFBA85A834D23251C

Le document en format XML

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<name sortKey="Kallinger, T" sort="Kallinger, T" uniqKey="Kallinger T" first="T." last="Kallinger">T. Kallinger</name>
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<name sortKey="Mosser, B" sort="Mosser, B" uniqKey="Mosser B" first="B." last="Mosser">B. Mosser</name>
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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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<affiliation>
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<term>Adiabatic frequencies</term>
<term>Allende prieto</term>
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<term>Atlas9 code</term>
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<term>Background model</term>
<term>Bedding</term>
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<term>Binned power spectrum</term>
<term>Blue triangles</term>
<term>Bottom panel</term>
<term>Buoyancy frequency</term>
<term>Cambridge univ</term>
<term>Central frequency</term>
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<term>Convective envelope</term>
<term>Direct modelling</term>
<term>Echelle</term>
<term>Echelle diagram</term>
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<term>Effective temperature</term>
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<term>Frequency range</term>
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<term>Gravity character</term>
<term>Gravity waves</term>
<term>Grey dots</term>
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<term>Harmonic degree</term>
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<term>Individual frequencies</term>
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<term>Oscillation properties</term>
<term>Oscillation spectra</term>
<term>Oscillation spectrum</term>
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<term>Period spacings</term>
<term>Photon noise</term>
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<term>Present analysis</term>
<term>Pressure scaleheight</term>
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<term>Publications division</term>
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<term>Radial order</term>
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<term>Results show</term>
<term>Rotational</term>
<term>Rotational splitting</term>
<term>Rotational splittings</term>
<term>Same frequency</term>
<term>Second ionization</term>
<term>Sharp features</term>
<term>Sharp variation</term>
<term>Similar frequencies</term>
<term>Small frequency separation</term>
<term>Small frequency separations</term>
<term>Small separation</term>
<term>Small separations</term>
<term>Solid lines</term>
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<term>Spectroscopic constraints</term>
<term>Spectroscopic observations</term>
<term>Spectrum</term>
<term>Standard deviation</term>
<term>Stellar</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 30 d in short‐cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Hz and Hz, respectively, and the frequency of maximum oscillation power, Hz. The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to Hz. 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 ∼1.3 M⊙, a radius of 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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<abstract>We present the results of the asteroseismic analysis of the red‐giant star KIC 4351319 (TYC 3124‐914‐1), observed for 30 d in short‐cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Hz and Hz, respectively, and the frequency of maximum oscillation power, Hz. The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to Hz. 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 ∼1.3 M⊙, a radius of 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.</abstract>
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<title>Solar‐like oscillations from the depths of the red‐giant star KIC 4351319 observed with Kepler</title>
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<head>ABSTRACT</head>
<p>We present the results of the asteroseismic analysis of the red‐giant star KIC 4351319 (TYC 3124‐914‐1), observed for 30 d in short‐cadence mode with the 
<hi rend="italic">Kepler</hi>
 satellite. The analysis has allowed us to determine the large and small frequency separations,
<graphic url="equation/MNR_18996_mu1.gif" rend="inline image"></graphic>
Hz and
<graphic url="equation/MNR_18996_mu2.gif" rend="inline image"></graphic>
Hz, respectively, and the frequency of maximum oscillation power,
<graphic url="equation/MNR_18996_mu3.gif" rend="inline image"></graphic>
Hz.</p>
<p>The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to
<graphic url="equation/MNR_18996_mu4.gif" rend="inline image"></graphic>
Hz.</p>
<p>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.</p>
<p>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.</p>
<p>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 ∼1.3 M
<hi rend="subscript"></hi>
, a radius of
<graphic url="equation/MNR_18996_mu5.gif" rend="inline image"></graphic>
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.</p>
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<p>We present the results of the asteroseismic analysis of the red‐giant star KIC 4351319 (TYC 3124‐914‐1), observed for 30 d in short‐cadence mode with the 
<i>Kepler</i>
 satellite. The analysis has allowed us to determine the large and small frequency separations,
<inlineGraphic alt="inline image" location="equation/MNR_18996_mu1.gif" href=""></inlineGraphic>
Hz and
<inlineGraphic alt="inline image" location="equation/MNR_18996_mu2.gif" href=""></inlineGraphic>
Hz, respectively, and the frequency of maximum oscillation power,
<inlineGraphic alt="inline image" location="equation/MNR_18996_mu3.gif" href=""></inlineGraphic>
Hz.</p>
<p>The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to
<inlineGraphic alt="inline image" location="equation/MNR_18996_mu4.gif" href=""></inlineGraphic>
Hz.</p>
<p>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.</p>
<p>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.</p>
<p>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 ∼1.3 M
<sub></sub>
, a radius of
<inlineGraphic alt="inline image" location="equation/MNR_18996_mu5.gif" href=""></inlineGraphic>
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.</p>
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<namePart type="given">T. R.</namePart>
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<abstract lang="en">We present the results of the asteroseismic analysis of the red‐giant star KIC 4351319 (TYC 3124‐914‐1), observed for 30 d in short‐cadence mode with the Kepler satellite. The analysis has allowed us to determine the large and small frequency separations, Hz and Hz, respectively, and the frequency of maximum oscillation power, Hz. The high signal‐to‐noise ratio of the observations allowed us to identify 25 independent pulsation modes whose frequencies range approximately from 300 to Hz. 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 ∼1.3 M⊙, a radius of 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.</abstract>
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