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DETECTION OF SOLAR-LIKE OSCILLATIONS, OBSERVATIONAL CONSTRAINTS, AND STELLAR MODELS FOR θ CYG, THE BRIGHTEST STAR OBSERVED BY THE KEPLER MISSION
ABSTRACT θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star observed by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June-September) and subsequently in...
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Published in: | The Astrophysical journal 2016-11, Vol.831 (1), p.17 |
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creator | Guzik, J. A. Houdek, G. Chaplin, W. J. Smalley, B. Kurtz, D. W. Gilliland, R. L. Mullally, F. Rowe, J. F. Bryson, S. T. Still, M. D. Antoci, V. Appourchaux, T. Basu, S. Bedding, T. R. Benomar, O. Garcia, R. A. Huber, D. Kjeldsen, H. Latham, D. W. Metcalfe, T. S. Pápics, P. I. White, T. R. Aerts, C. Ballot, J. Boyajian, T. S. Briquet, M. Bruntt, H. Buchhave, L. A. Campante, T. L. Catanzaro, G. Christensen-Dalsgaard, J. Davies, G. R. Doğan, G. Dragomir, D. Doyle, A. P. Elsworth, Y. Frasca, A. Gaulme, P. Gruberbauer, M. Handberg, R. Hekker, S. Karoff, C. Lehmann, H. Mathias, P. Mathur, S. Miglio, A. Molenda- akowicz, J. Mosser, B. Murphy, S. J. Régulo, C. Ripepi, V. Salabert, D. Sousa, S. G. Stello, D. Uytterhoeven, K. |
description | ABSTRACT θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star observed by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June-September) and subsequently in Quarters 8 and 12-17. We present analyses of solar-like oscillations based on Q6 and Q8 data, identifying angular degree l = 0, 1, and 2 modes with frequencies of 1000-2700 Hz, a large frequency separation of 83.9 0.4 Hz, and maximum oscillation amplitude at frequency max = 1829 54 Hz. We also present analyses of new ground-based spectroscopic observations, which, combined with interferometric angular diameter measurements, give Teff = 6697 78 K, radius 1.49 0.03 R , [Fe/H] = −0.02 0.06 dex, and log g = 4.23 0.03. We calculate stellar models matching these constraints using the Yale Rotating Evolution Code and the Asteroseismic Modeling Portal. The best-fit models have masses of 1.35-1.39 M and ages of 1.0-1.6 Gyr. θ Cyg's Teff and log g place it cooler than the red edge of the γ Doradus instability region established from pre-Kepler ground-based observations, but just at the red edge derived from pulsation modeling. The pulsation models show γ Dor gravity modes driven by the convective blocking mechanism, with frequencies of 1-3 cycles per day (11 to 33 Hz). However, gravity modes were not seen in Kepler data; one signal at 1.776 cycles per day (20.56 Hz) may be attributable to a faint, possibly background, binary. |
doi_str_mv | 10.3847/0004-637X/831/1/17 |
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A. ; Houdek, G. ; Chaplin, W. J. ; Smalley, B. ; Kurtz, D. W. ; Gilliland, R. L. ; Mullally, F. ; Rowe, J. F. ; Bryson, S. T. ; Still, M. D. ; Antoci, V. ; Appourchaux, T. ; Basu, S. ; Bedding, T. R. ; Benomar, O. ; Garcia, R. A. ; Huber, D. ; Kjeldsen, H. ; Latham, D. W. ; Metcalfe, T. S. ; Pápics, P. I. ; White, T. R. ; Aerts, C. ; Ballot, J. ; Boyajian, T. S. ; Briquet, M. ; Bruntt, H. ; Buchhave, L. A. ; Campante, T. L. ; Catanzaro, G. ; Christensen-Dalsgaard, J. ; Davies, G. R. ; Doğan, G. ; Dragomir, D. ; Doyle, A. P. ; Elsworth, Y. ; Frasca, A. ; Gaulme, P. ; Gruberbauer, M. ; Handberg, R. ; Hekker, S. ; Karoff, C. ; Lehmann, H. ; Mathias, P. ; Mathur, S. ; Miglio, A. ; Molenda- akowicz, J. ; Mosser, B. ; Murphy, S. J. ; Régulo, C. ; Ripepi, V. ; Salabert, D. ; Sousa, S. G. ; Stello, D. ; Uytterhoeven, K.</creator><creatorcontrib>Guzik, J. A. ; Houdek, G. ; Chaplin, W. J. ; Smalley, B. ; Kurtz, D. W. ; Gilliland, R. L. ; Mullally, F. ; Rowe, J. F. ; Bryson, S. T. ; Still, M. D. ; Antoci, V. ; Appourchaux, T. ; Basu, S. ; Bedding, T. R. ; Benomar, O. ; Garcia, R. A. ; Huber, D. ; Kjeldsen, H. ; Latham, D. W. ; Metcalfe, T. S. ; Pápics, P. I. ; White, T. R. ; Aerts, C. ; Ballot, J. ; Boyajian, T. S. ; Briquet, M. ; Bruntt, H. ; Buchhave, L. A. ; Campante, T. L. ; Catanzaro, G. ; Christensen-Dalsgaard, J. ; Davies, G. R. ; Doğan, G. ; Dragomir, D. ; Doyle, A. P. ; Elsworth, Y. ; Frasca, A. ; Gaulme, P. ; Gruberbauer, M. ; Handberg, R. ; Hekker, S. ; Karoff, C. ; Lehmann, H. ; Mathias, P. ; Mathur, S. ; Miglio, A. ; Molenda- akowicz, J. ; Mosser, B. ; Murphy, S. J. ; Régulo, C. ; Ripepi, V. ; Salabert, D. ; Sousa, S. G. ; Stello, D. ; Uytterhoeven, K. ; Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</creatorcontrib><description>ABSTRACT θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star observed by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June-September) and subsequently in Quarters 8 and 12-17. We present analyses of solar-like oscillations based on Q6 and Q8 data, identifying angular degree l = 0, 1, and 2 modes with frequencies of 1000-2700 Hz, a large frequency separation of 83.9 0.4 Hz, and maximum oscillation amplitude at frequency max = 1829 54 Hz. We also present analyses of new ground-based spectroscopic observations, which, combined with interferometric angular diameter measurements, give Teff = 6697 78 K, radius 1.49 0.03 R , [Fe/H] = −0.02 0.06 dex, and log g = 4.23 0.03. We calculate stellar models matching these constraints using the Yale Rotating Evolution Code and the Asteroseismic Modeling Portal. The best-fit models have masses of 1.35-1.39 M and ages of 1.0-1.6 Gyr. θ Cyg's Teff and log g place it cooler than the red edge of the γ Doradus instability region established from pre-Kepler ground-based observations, but just at the red edge derived from pulsation modeling. The pulsation models show γ Dor gravity modes driven by the convective blocking mechanism, with frequencies of 1-3 cycles per day (11 to 33 Hz). However, gravity modes were not seen in Kepler data; one signal at 1.776 cycles per day (20.56 Hz) may be attributable to a faint, possibly background, binary.</description><identifier>ISSN: 0004-637X</identifier><identifier>ISSN: 1538-4357</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.3847/0004-637X/831/1/17</identifier><language>eng</language><publisher>Philadelphia: The American Astronomical Society</publisher><subject>Apertures ; asteroseismology ; Astronomical models ; ASTRONOMY AND ASTROPHYSICS ; Astrophysics ; Binary stars ; Constraint modelling ; Diameters ; Gravitation ; Ground-based observation ; Main sequence stars ; Model matching ; Oscillations ; Physics ; Pulsation ; Solar oscillations ; Spacecraft ; Stars & galaxies ; stars: fundamental parameters ; stars: interiors ; stars: solar-type ; Stellar evolution ; Stellar models</subject><ispartof>The Astrophysical journal, 2016-11, Vol.831 (1), p.17</ispartof><rights>2016. 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(LANL), Los Alamos, NM (United States)</creatorcontrib><title>DETECTION OF SOLAR-LIKE OSCILLATIONS, OBSERVATIONAL CONSTRAINTS, AND STELLAR MODELS FOR θ CYG, THE BRIGHTEST STAR OBSERVED BY THE KEPLER MISSION</title><title>The Astrophysical journal</title><addtitle>APJ</addtitle><addtitle>Astrophys. J</addtitle><description>ABSTRACT θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star observed by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June-September) and subsequently in Quarters 8 and 12-17. We present analyses of solar-like oscillations based on Q6 and Q8 data, identifying angular degree l = 0, 1, and 2 modes with frequencies of 1000-2700 Hz, a large frequency separation of 83.9 0.4 Hz, and maximum oscillation amplitude at frequency max = 1829 54 Hz. We also present analyses of new ground-based spectroscopic observations, which, combined with interferometric angular diameter measurements, give Teff = 6697 78 K, radius 1.49 0.03 R , [Fe/H] = −0.02 0.06 dex, and log g = 4.23 0.03. We calculate stellar models matching these constraints using the Yale Rotating Evolution Code and the Asteroseismic Modeling Portal. The best-fit models have masses of 1.35-1.39 M and ages of 1.0-1.6 Gyr. θ Cyg's Teff and log g place it cooler than the red edge of the γ Doradus instability region established from pre-Kepler ground-based observations, but just at the red edge derived from pulsation modeling. The pulsation models show γ Dor gravity modes driven by the convective blocking mechanism, with frequencies of 1-3 cycles per day (11 to 33 Hz). However, gravity modes were not seen in Kepler data; one signal at 1.776 cycles per day (20.56 Hz) may be attributable to a faint, possibly background, binary.</description><subject>Apertures</subject><subject>asteroseismology</subject><subject>Astronomical models</subject><subject>ASTRONOMY AND ASTROPHYSICS</subject><subject>Astrophysics</subject><subject>Binary stars</subject><subject>Constraint modelling</subject><subject>Diameters</subject><subject>Gravitation</subject><subject>Ground-based observation</subject><subject>Main sequence stars</subject><subject>Model matching</subject><subject>Oscillations</subject><subject>Physics</subject><subject>Pulsation</subject><subject>Solar oscillations</subject><subject>Spacecraft</subject><subject>Stars & galaxies</subject><subject>stars: fundamental parameters</subject><subject>stars: interiors</subject><subject>stars: solar-type</subject><subject>Stellar evolution</subject><subject>Stellar models</subject><issn>0004-637X</issn><issn>1538-4357</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp9kd9u0zAUxi3EJMrGC3BlwRXSsvpv7FymqdtGMw2KDWJXVnBTLdNoSpIh7TH2NjwFzzRnmcYdOhfWOef3ffLRB8B7jC6oZGKOEGJRTMX3uaR4Hkq8AjPMqYwY5eI1mL0Ab8Dbvr8ZW5IkM_CwVFZlNi-2sFhBU-i0jHR-qWBhslzrdNyYc1gsjCq_PXWphlmY2TLNtzas0u0SGqsCW8LPxVJpA1dFCf_-gdnV-hzajYKLMl9vrDI2gIGazNQSLq6e1pfqi1ZBnBsT_M_Ayb667et3z-8p-LpSNttEuljnWaojTwUfIo_riv6IOauxR3u2Q3u-q2LPkOCCJGSHKZOEhjN3lZSiorFMOJE08bQmgjJKT8GHybfth8b1vhlqf-3bw6H2gwtqjpkI0KcJuq5u3bFrflbdvWurxm1S7cYZIowniaC_cWA_Tuyxa3_d1f3gbtq77hBucITGPImlQChQZKJ81_Z9V-9fbDFyY5ZuzMaNUbmQpQs1fuNiEjXt8Z_rfwSPLd6Rug</recordid><startdate>20161101</startdate><enddate>20161101</enddate><creator>Guzik, J. 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A. ; Houdek, G. ; Chaplin, W. J. ; Smalley, B. ; Kurtz, D. W. ; Gilliland, R. L. ; Mullally, F. ; Rowe, J. F. ; Bryson, S. T. ; Still, M. D. ; Antoci, V. ; Appourchaux, T. ; Basu, S. ; Bedding, T. R. ; Benomar, O. ; Garcia, R. A. ; Huber, D. ; Kjeldsen, H. ; Latham, D. W. ; Metcalfe, T. S. ; Pápics, P. I. ; White, T. R. ; Aerts, C. ; Ballot, J. ; Boyajian, T. S. ; Briquet, M. ; Bruntt, H. ; Buchhave, L. A. ; Campante, T. L. ; Catanzaro, G. ; Christensen-Dalsgaard, J. ; Davies, G. R. ; Doğan, G. ; Dragomir, D. ; Doyle, A. P. ; Elsworth, Y. ; Frasca, A. ; Gaulme, P. ; Gruberbauer, M. ; Handberg, R. ; Hekker, S. ; Karoff, C. ; Lehmann, H. ; Mathias, P. ; Mathur, S. ; Miglio, A. ; Molenda- akowicz, J. ; Mosser, B. ; Murphy, S. J. ; Régulo, C. ; Ripepi, V. ; Salabert, D. ; Sousa, S. G. ; Stello, D. ; Uytterhoeven, K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c375t-c1ea3b654e1c0f4d0f5da6c40757292d134823004da887a368952839c3e273433</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Apertures</topic><topic>asteroseismology</topic><topic>Astronomical models</topic><topic>ASTRONOMY AND ASTROPHYSICS</topic><topic>Astrophysics</topic><topic>Binary stars</topic><topic>Constraint modelling</topic><topic>Diameters</topic><topic>Gravitation</topic><topic>Ground-based observation</topic><topic>Main sequence stars</topic><topic>Model matching</topic><topic>Oscillations</topic><topic>Physics</topic><topic>Pulsation</topic><topic>Solar oscillations</topic><topic>Spacecraft</topic><topic>Stars & galaxies</topic><topic>stars: fundamental parameters</topic><topic>stars: interiors</topic><topic>stars: solar-type</topic><topic>Stellar evolution</topic><topic>Stellar models</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guzik, J. A.</creatorcontrib><creatorcontrib>Houdek, G.</creatorcontrib><creatorcontrib>Chaplin, W. J.</creatorcontrib><creatorcontrib>Smalley, B.</creatorcontrib><creatorcontrib>Kurtz, D. W.</creatorcontrib><creatorcontrib>Gilliland, R. L.</creatorcontrib><creatorcontrib>Mullally, F.</creatorcontrib><creatorcontrib>Rowe, J. F.</creatorcontrib><creatorcontrib>Bryson, S. T.</creatorcontrib><creatorcontrib>Still, M. D.</creatorcontrib><creatorcontrib>Antoci, V.</creatorcontrib><creatorcontrib>Appourchaux, T.</creatorcontrib><creatorcontrib>Basu, S.</creatorcontrib><creatorcontrib>Bedding, T. R.</creatorcontrib><creatorcontrib>Benomar, O.</creatorcontrib><creatorcontrib>Garcia, R. A.</creatorcontrib><creatorcontrib>Huber, D.</creatorcontrib><creatorcontrib>Kjeldsen, H.</creatorcontrib><creatorcontrib>Latham, D. W.</creatorcontrib><creatorcontrib>Metcalfe, T. S.</creatorcontrib><creatorcontrib>Pápics, P. I.</creatorcontrib><creatorcontrib>White, T. R.</creatorcontrib><creatorcontrib>Aerts, C.</creatorcontrib><creatorcontrib>Ballot, J.</creatorcontrib><creatorcontrib>Boyajian, T. S.</creatorcontrib><creatorcontrib>Briquet, M.</creatorcontrib><creatorcontrib>Bruntt, H.</creatorcontrib><creatorcontrib>Buchhave, L. A.</creatorcontrib><creatorcontrib>Campante, T. L.</creatorcontrib><creatorcontrib>Catanzaro, G.</creatorcontrib><creatorcontrib>Christensen-Dalsgaard, J.</creatorcontrib><creatorcontrib>Davies, G. R.</creatorcontrib><creatorcontrib>Doğan, G.</creatorcontrib><creatorcontrib>Dragomir, D.</creatorcontrib><creatorcontrib>Doyle, A. P.</creatorcontrib><creatorcontrib>Elsworth, Y.</creatorcontrib><creatorcontrib>Frasca, A.</creatorcontrib><creatorcontrib>Gaulme, P.</creatorcontrib><creatorcontrib>Gruberbauer, M.</creatorcontrib><creatorcontrib>Handberg, R.</creatorcontrib><creatorcontrib>Hekker, S.</creatorcontrib><creatorcontrib>Karoff, C.</creatorcontrib><creatorcontrib>Lehmann, H.</creatorcontrib><creatorcontrib>Mathias, P.</creatorcontrib><creatorcontrib>Mathur, S.</creatorcontrib><creatorcontrib>Miglio, A.</creatorcontrib><creatorcontrib>Molenda- akowicz, J.</creatorcontrib><creatorcontrib>Mosser, B.</creatorcontrib><creatorcontrib>Murphy, S. J.</creatorcontrib><creatorcontrib>Régulo, C.</creatorcontrib><creatorcontrib>Ripepi, V.</creatorcontrib><creatorcontrib>Salabert, D.</creatorcontrib><creatorcontrib>Sousa, S. G.</creatorcontrib><creatorcontrib>Stello, D.</creatorcontrib><creatorcontrib>Uytterhoeven, K.</creatorcontrib><creatorcontrib>Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guzik, J. A.</au><au>Houdek, G.</au><au>Chaplin, W. J.</au><au>Smalley, B.</au><au>Kurtz, D. W.</au><au>Gilliland, R. L.</au><au>Mullally, F.</au><au>Rowe, J. F.</au><au>Bryson, S. T.</au><au>Still, M. D.</au><au>Antoci, V.</au><au>Appourchaux, T.</au><au>Basu, S.</au><au>Bedding, T. R.</au><au>Benomar, O.</au><au>Garcia, R. A.</au><au>Huber, D.</au><au>Kjeldsen, H.</au><au>Latham, D. W.</au><au>Metcalfe, T. S.</au><au>Pápics, P. I.</au><au>White, T. R.</au><au>Aerts, C.</au><au>Ballot, J.</au><au>Boyajian, T. S.</au><au>Briquet, M.</au><au>Bruntt, H.</au><au>Buchhave, L. A.</au><au>Campante, T. L.</au><au>Catanzaro, G.</au><au>Christensen-Dalsgaard, J.</au><au>Davies, G. R.</au><au>Doğan, G.</au><au>Dragomir, D.</au><au>Doyle, A. P.</au><au>Elsworth, Y.</au><au>Frasca, A.</au><au>Gaulme, P.</au><au>Gruberbauer, M.</au><au>Handberg, R.</au><au>Hekker, S.</au><au>Karoff, C.</au><au>Lehmann, H.</au><au>Mathias, P.</au><au>Mathur, S.</au><au>Miglio, A.</au><au>Molenda- akowicz, J.</au><au>Mosser, B.</au><au>Murphy, S. J.</au><au>Régulo, C.</au><au>Ripepi, V.</au><au>Salabert, D.</au><au>Sousa, S. G.</au><au>Stello, D.</au><au>Uytterhoeven, K.</au><aucorp>Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>DETECTION OF SOLAR-LIKE OSCILLATIONS, OBSERVATIONAL CONSTRAINTS, AND STELLAR MODELS FOR θ CYG, THE BRIGHTEST STAR OBSERVED BY THE KEPLER MISSION</atitle><jtitle>The Astrophysical journal</jtitle><stitle>APJ</stitle><addtitle>Astrophys. J</addtitle><date>2016-11-01</date><risdate>2016</risdate><volume>831</volume><issue>1</issue><spage>17</spage><pages>17-</pages><issn>0004-637X</issn><issn>1538-4357</issn><eissn>1538-4357</eissn><abstract>ABSTRACT θ Cygni is an F3 spectral type magnitude V = 4.48 main-sequence star that was the brightest star observed by the original Kepler spacecraft mission. Short-cadence (58.8 s) photometric data using a custom aperture were first obtained during Quarter 6 (2010 June-September) and subsequently in Quarters 8 and 12-17. We present analyses of solar-like oscillations based on Q6 and Q8 data, identifying angular degree l = 0, 1, and 2 modes with frequencies of 1000-2700 Hz, a large frequency separation of 83.9 0.4 Hz, and maximum oscillation amplitude at frequency max = 1829 54 Hz. We also present analyses of new ground-based spectroscopic observations, which, combined with interferometric angular diameter measurements, give Teff = 6697 78 K, radius 1.49 0.03 R , [Fe/H] = −0.02 0.06 dex, and log g = 4.23 0.03. We calculate stellar models matching these constraints using the Yale Rotating Evolution Code and the Asteroseismic Modeling Portal. The best-fit models have masses of 1.35-1.39 M and ages of 1.0-1.6 Gyr. θ Cyg's Teff and log g place it cooler than the red edge of the γ Doradus instability region established from pre-Kepler ground-based observations, but just at the red edge derived from pulsation modeling. The pulsation models show γ Dor gravity modes driven by the convective blocking mechanism, with frequencies of 1-3 cycles per day (11 to 33 Hz). However, gravity modes were not seen in Kepler data; one signal at 1.776 cycles per day (20.56 Hz) may be attributable to a faint, possibly background, binary.</abstract><cop>Philadelphia</cop><pub>The American Astronomical Society</pub><doi>10.3847/0004-637X/831/1/17</doi><tpages>22</tpages><orcidid>https://orcid.org/0000-0003-1291-1533</orcidid><orcidid>https://orcid.org/0000-0003-1801-426X</orcidid><orcidid>https://orcid.org/0000-0001-9879-9313</orcidid><orcidid>https://orcid.org/0000-0002-9037-0018</orcidid><orcidid>https://orcid.org/0000-0002-4588-5389</orcidid><orcidid>https://orcid.org/0000-0003-1460-6663</orcidid><orcidid>https://orcid.org/0000-0001-5137-0966</orcidid><orcidid>https://orcid.org/0000-0002-0474-0896</orcidid><orcidid>https://orcid.org/0000-0003-2313-467X</orcidid><orcidid>https://orcid.org/0000-0001-9047-2965</orcidid><orcidid>https://orcid.org/0000-0002-0129-0316</orcidid><orcidid>https://orcid.org/0000-0003-1822-7126</orcidid><orcidid>https://orcid.org/0000-0002-9649-1013</orcidid><orcidid>https://orcid.org/0000000312911533</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0004-637X |
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issn | 0004-637X 1538-4357 1538-4357 |
language | eng |
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subjects | Apertures asteroseismology Astronomical models ASTRONOMY AND ASTROPHYSICS Astrophysics Binary stars Constraint modelling Diameters Gravitation Ground-based observation Main sequence stars Model matching Oscillations Physics Pulsation Solar oscillations Spacecraft Stars & galaxies stars: fundamental parameters stars: interiors stars: solar-type Stellar evolution Stellar models |
title | DETECTION OF SOLAR-LIKE OSCILLATIONS, OBSERVATIONAL CONSTRAINTS, AND STELLAR MODELS FOR θ CYG, THE BRIGHTEST STAR OBSERVED BY THE KEPLER MISSION |
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