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dc.contributor.authorMukadam, Anjum Shaguftapt_BR
dc.contributor.authorBischoff-Kim, Agnèspt_BR
dc.contributor.authorFraser, Oliverpt_BR
dc.contributor.authorCórsico, Alejandro Hugopt_BR
dc.contributor.authorMontgomery, Michael Houstonpt_BR
dc.contributor.authorKepler, Souza Oliveirapt_BR
dc.contributor.authorRomero, Alejandra Danielapt_BR
dc.contributor.authorKronberg, M. E.pt_BR
dc.contributor.authorWinget, K. I.pt_BR
dc.contributor.authorFalcon, Ross E.pt_BR
dc.contributor.authorChandler, Dean W.pt_BR
dc.contributor.authorKuehne, J. W.pt_BR
dc.contributor.authorSullivan, Denis J.pt_BR
dc.contributor.authorReaves, David Earlpt_BR
dc.contributor.authorVon Hippel, Theodore A.pt_BR
dc.contributor.authorMullally, Fergalpt_BR
dc.contributor.authorShipman, Harry L.pt_BR
dc.contributor.authorThompson, S. E.pt_BR
dc.contributor.authorSilvestri, Nicole M.pt_BR
dc.contributor.authorHynes, R. I.pt_BR
dc.date.accessioned2015-01-20T02:15:22Zpt_BR
dc.date.issued2013pt_BR
dc.identifier.issn0004-637Xpt_BR
dc.identifier.urihttp://hdl.handle.net/10183/109069pt_BR
dc.description.abstractWe have finally measured the evolutionary rate of cooling of the pulsating hydrogen atmosphere (DA) white dwarf ZZ Ceti (Ross 548), as reflected by the drift rate of the 213.13260694 s period. Using 41 yr of time-series photometry from 1970 November to 2012 January, we determine the rate of change of this period with time to be dP/dt = (5.2 ± 1.4) ×10−15 s s-ˡ employing the O−C method and (5.45 ± 0.79) ×10−15 s s-ˡ using a direct nonlinear least squares fit to the entire lightcurve. We adopt the dP/dt obtained from the nonlinear least squares program as our final determination, but augment the corresponding uncertainty to a more realistic value, ultimately arriving at the measurement of dP/dt = (5.5 ± 1.0) ×10−15 s s-ˡ. After correcting for proper motion, the evolutionary rate of cooling of ZZ Ceti is computed to be (3.3 ± 1.1) ×10−15 s s-ˡ. This value is consistent within uncertainties with the measurement of (4.19±0.73)×10−15 s s-ˡ for another similar pulsating DA white dwarf, G 117-B15A.Measuring the cooling rate of ZZ Ceti helps us refine our stellar structure and evolutionary models, as cooling depends mainly on the core composition and stellar mass. Calibrating white dwarf cooling curves with this measurement will reduce the theoretical uncertainties involved in white dwarf cosmochronometry. Should the 213.13 s period be trapped in the hydrogen envelope, then our determination of its drift rate compared to the expected evolutionary rate suggests an additional source of stellar cooling. Attributing the excess cooling to the emission of axions imposes a constraint on the mass of the hypothetical axion particle.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofThe astrophysical journal. Bristol. Vol. 771, no. 1 (July 2013), 17, 11 p.pt_BR
dc.rightsOpen Accessen
dc.subjectRadiação estelarpt_BR
dc.subjectStars: evolutionen
dc.subjectStars: individual (ZZ Ceti, R548)en
dc.subjectMassa estelarpt_BR
dc.subjectStars: oscillations (including pulsations)en
dc.subjectAnãs brancaspt_BR
dc.subjectEvolucao estelarpt_BR
dc.subjectStars: variables: generalen
dc.subjectSéries temporaispt_BR
dc.subjectWwhite dwarfsen
dc.subjectProcessos internos estelarespt_BR
dc.subjectFotometria estelarpt_BR
dc.titleMeasuring the evolutionay rate of cooling of ZZ Cetipt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000900674pt_BR
dc.type.originEstrangeiropt_BR


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