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dc.contributor.authorWinget, Donald Earlpt_BR
dc.contributor.authorNather, R. Edwardpt_BR
dc.contributor.authorClemens, J. Christopherpt_BR
dc.contributor.authorProvencal, Judith L.pt_BR
dc.contributor.authorKleinman, Scot Jamespt_BR
dc.contributor.authorBradley, Paul A.pt_BR
dc.contributor.authorWood, Matthew A.pt_BR
dc.contributor.authorClaver, C.F.pt_BR
dc.contributor.authorRobinson, E.L.pt_BR
dc.contributor.authorGrauer, Albert D.pt_BR
dc.contributor.authorHine, B.P.pt_BR
dc.contributor.authorFontaine, Gillespt_BR
dc.contributor.authorAchilleos, Nicholaspt_BR
dc.contributor.authorMarar, T.M. Krishnanpt_BR
dc.contributor.authorSeetha, S.pt_BR
dc.contributor.authorAshoka, B.N.pt_BR
dc.contributor.authorO'Donoghue, Darraghpt_BR
dc.contributor.authorWarner, B.pt_BR
dc.contributor.authorKurtz, Donald W.pt_BR
dc.contributor.authorMartinez, Peterpt_BR
dc.contributor.authorVauclair, Gérardpt_BR
dc.contributor.authorChevreton, Michelpt_BR
dc.contributor.authorAugusteijn, T.pt_BR
dc.contributor.authorParadijs, J. vanpt_BR
dc.contributor.authorHansen, Carl J.pt_BR
dc.contributor.authorLiebert, Jamespt_BR
dc.contributor.authorKanaan Neto, Antonio Nemerpt_BR
dc.contributor.authorKepler, Souza Oliveirapt_BR
dc.date.accessioned2014-12-31T02:10:48Zpt_BR
dc.date.issued1990pt_BR
dc.identifier.issn0004-637Xpt_BR
dc.identifier.urihttp://hdl.handle.net/10183/108715pt_BR
dc.description.abstractUsing an extensive set of high-speed photometric observations obtained with the Whole Earth Telescope network, we show that the complex light curve of the ZZ Ceti (DAV) star G29-38 is dominated by a single, constant amplitude period of 615 s during the time span of our observations. The pulse arrival times for this period exhibit a systematic variation in phase readily explained by light-travel time effects produced by reflex orbital motion about an unseen companion. Our best-fit model to the observations indicates a highly eccen­ tric orbit, a period of 109 ± 13 days and a minimum mass of 0.5 Mʘ for the companion. Radial velocity variations predicted by this model are not observed, however, nor are these phase variations seen in another independent pulsation, so the origin of the phase variation remains a mystery. Any model involving intrinsic pulsation mechanisms must explain the large (~200 s) phase change with no corresponding change in pulsation amplitude, and it shape, which mimics quite exactly the effects of binary orbital motion.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofThe astrophysical journal. Chicago. Vol. 357, no. 2, pt. 1 (July 1990), p. 630-637pt_BR
dc.rightsOpen Accessen
dc.subjectAstrofísicapt_BR
dc.subjectStars: binariesen
dc.subjectStars: individual (G29-38)en
dc.subjectAnãs brancaspt_BR
dc.subjectStars: pulsationen
dc.subjectEstrelas binariaspt_BR
dc.subjectPulsacoes estelarespt_BR
dc.subjectStars: white dwarfsen
dc.titleWhole Earth Telescope observations of the white dwarf G29-38 : phase variations of the 615 second periodpt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000015354pt_BR
dc.type.originEstrangeiropt_BR


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