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dc.contributorDepartment of Physics and Astronomy, University of Iowa, 52242, Iowa City, IA, USA
dc.contributorArmagh Observatory and Planetarium, College Hill, BT65 9DG, Armagh, Northern Ireland, UK
dc.contributorPenn State Scranton, 120 Ridge View Drive, 18512, Dunmore, PA, USA
dc.contributorDepartment of Physics and Astronomy, Howard University, 20059, Washington, DC, USA; Center for Research and Exploration in Space Science and Technology, and X-ray Astrophysics Laboratory, NASA/GSFC, 20771, Greenbelt, MD, USA; Center for Research and Exploration in Space Science and Technology, and X-ray Astrophysics Laboratory, NASA/GSFC, 20771, Greenbelt, MD, USA
dc.contributorDepartment of Physics & Astronomy, East Tennessee State University, 37614, Johnson City, TN, USA
dc.contributorDepartment of Physics and Astronomy, University College London, Gower Street, WC1E 6BT, London, UK
dc.contributorDépartement de physique, Université de Montréal, Complexe des Sciences, 1375 Avenue Thérèse-Lavoie-Roux, H2V 0B3, Montréal (QC), Canada
dc.contributorDepartment of Astronomy, University of Geneva, Chemin Pegasi 51, 1290, Versoix GE, Switzerland
dc.contributorGAPHE, Univ. of Liège, B5C, Allée du 6 Août 19c, B-4000, Liège, Belgium
dc.contributorAnton Pannekoek Institute for Astronomy and Astrophysics, University of Amsterdam, 1090 GE, Amsterdam, The Netherlands
dc.contributorNASA/GSFC, 20771, Greenbelt, MD, USA
dc.contributorNicolaus Copernicus Astronomical Centre of the Polish Academy of Sciences, Bartycka 18, 00-716, Warsaw, Poland
dc.contributorDepartment of Physics and Astronomy, University of Delaware, 217 Sharp Lab, Newark, DE, USA
dc.contributorInstitute of Astronomy, KU Leuven, Celestijnenlaan 200D/2401, 3001, Leuven, Belgium
dc.contributor.authorGayley, Kenneth G.
dc.contributor.authorVink, Jorick S.
dc.contributor.authorud-Doula, Asif
dc.contributor.authorDavid-Uraz, Alexandre
dc.contributor.authorIgnace, Richard
dc.contributor.authorPrinja, Raman
dc.contributor.authorSt-Louis, Nicole
dc.contributor.authorEkström, Sylvia
dc.contributor.authorNazé, Yaël
dc.contributor.authorShenar, Tomer
dc.contributor.authorScowen, Paul A.
dc.contributor.authorSudnik, Natallia
dc.contributor.authorOwocki, Stan P.
dc.contributor.authorSundqvist, Jon O.
dc.contributor.authorDriessen, Florian A.
dc.contributor.authorHennicker, Levin
dc.date.accessioned2024-02-21T11:02:41Z
dc.date.available2024-02-21T11:02:41Z
dc.date.issued2022-12-01T00:00:00Z
dc.identifier.doi10.1007/s10509-022-04142-6
dc.identifier.doi10.48550/arXiv.2111.11633
dc.identifier.other2021arXiv211111633G
dc.identifier.otherastro-ph.SR
dc.identifier.otherastro-ph.IM
dc.identifier.other2021arXiv211111633G
dc.identifier.other10.1007/s10509-022-04142-6
dc.identifier.other2022Ap&SS.367..123G
dc.identifier.otherarXiv:2111.11633
dc.identifier.other10.48550/arXiv.2111.11633
dc.identifier.other0000-0001-8742-417X
dc.identifier.other-
dc.identifier.urihttp://hdl.handle.net/20.500.14302/1651
dc.description.abstractThe most massive stars are thought to lose a significant fraction of their mass in a steady wind during the main-sequence and blue supergiant phases. This in turn sets the stage for their further evolution and eventual supernova, and preconditions the surrounding medium for all following events, with consequences for ISM energization, chemical enrichment, and dust formation. Understanding these processes requires accurate observational constraints on the mass-loss rates of the most luminous stars, which can also be used to test theories of stellar wind driving. In the past, mass-loss rates have been characterized via collisional emission processes such as optical Hα and free-free radio emission, but these so-called density squared diagnostics require correction in the presence of widespread clumping. Recent observational and theoretical evidence points to the likelihood of a ubiquitously high level of such clumping in hot-star winds, but quantifying its effects requires a deeper understanding of the complex dynamics of radiatively driven winds and their stochastic instabilities. Furthermore, large-scale structures initiating in surface anisotropies and propagating throughout the wind can also affect wind driving and alter mass-loss diagnostics. Time series spectroscopy of high resonance-line opacity in the UV, capable of high resolution and high signal-to-noise, are required to better understand these complex dynamics, and more accurately determine mass-loss rates. The proposed Polstar mission (Scowen et al. 2022, this volume) provides the necessary resolution at the Sobolev (∼10 km s<SUP>−1</SUP>) or sound-speed (∼20 km s<SUP>−1</SUP>) scale, for over three dozen bright galactic massive stars with signal-to noise an order of magnitude above that of the celebrated MEGA campaign (Massa et al. 1995) of the International Ultraviolet Explorer (IUE), via continuous observations that track propagating structures through the winds in real time. Supporting geometric constraints are provided by the polarimetric capabilities present in all the datasets of such a mission.
dc.publisherAstrophysics and Space Science
dc.titleUnderstanding structure in line-driven stellar winds using ultraviolet spectropolarimetry in the time domain
dc.typearticle
dc.source.journalAp&SS
dc.source.journalAp&SS.367
dc.source.volume367
refterms.dateFOA2024-02-21T11:02:41Z
dc.identifier.bibcode2022Ap&SS.367..123G


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