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dc.contributorDepartment of Physics and Astronomy, University of Delaware, 217 Sharp Lab, Newark, Delaware 19716, USA
dc.contributorDepartment of Physics, Penn State Scranton, Dunmore, PA 18512, USA
dc.contributorNational Centre for Radio Astrophysics, Tata Institute of Fundamental Research, Pune University Campus, Pune 411007, India
dc.contributorNational Research Council of Canada, Herzberg Astronomy and Astrophysics Research Centre, 5071 West Saanich Road, Victoria, BC V9E 2E7, Canada
dc.contributorDepartment of Physics and Astronomy, Howard University, Washington, DC 20059, USA; Center for Research and Exploration in Space Science and Technology, and X-ray Astrophysics Laboratory, NASA/GSFC, Greenbelt, MD 20771, USA
dc.contributorDépartement de Physique et d'Astronomie, Université de Moncton, Moncton, NB E1A 3E9, Canada
dc.contributorDepartment of Physics and Astronomy, Uppsala University, Box 516, Uppsala SE75120, Sweden
dc.contributorArmagh Observatory and Planetarium, College Hill, Armagh BT61 9DG, UK; University of Western Ontario, London, Ontario, N6A 3K7, Canada
dc.contributorINAF - Osservatorio Astrofisico di Catania, Via S. Sofia 78, I-95123 Catania, Italy
dc.contributorLESIA, Paris Observatory, PSL University, CNRS, Sorbonne Université, Université de Paris, 5 place Jules Janssen, 92195 Meudon, France
dc.contributorESO - European Organisation for Astronomical Research in the Southern Hemisphere, Casilla 19001, Santiago 19, Chile
dc.contributorDepartment of Physics and Space Science, Royal Military College of Canada, Kingston, Ontario K7K 7B4, Canada
dc.contributor.authorShultz, M. E.
dc.contributor.authorOwocki, S. P.
dc.contributor.authorud-Doula, A.
dc.contributor.authorBiswas, A.
dc.contributor.authorBohlender, D.
dc.contributor.authorChandra, P.
dc.contributor.authorDas, B.
dc.contributor.authorDavid-Uraz, A.
dc.contributor.authorKhalack, V.
dc.contributor.authorKochukhov, O.
dc.contributor.authorLandstreet, J. D.
dc.contributor.authorLeto, P.
dc.contributor.authorMonin, D.
dc.contributor.authorNeiner, C.
dc.contributor.authorRivinius, Th
dc.contributor.authorWade, G. A.
dc.date.accessioned2024-02-02T13:31:28Z
dc.date.available2024-02-02T13:31:28Z
dc.date.issued2022-06-01T00:00:00Z
dc.identifier.doi10.1093/mnras/stac136
dc.identifier.doi10.48550/arXiv.2201.05512
dc.identifier.other2022arXiv220105512S
dc.identifier.other2022MNRAS.tmp.1099S
dc.identifier.otherastro-ph.SR
dc.identifier.otherastro-ph.HE
dc.identifier.other10.48550/arXiv.2201.05512
dc.identifier.other2022arXiv220105512S
dc.identifier.otherarXiv:2201.05512
dc.identifier.other10.1093/mnras/stac136
dc.identifier.other2022MNRAS.513.1429S
dc.identifier.other2022MNRAS.tmp.1099S
dc.identifier.other-
dc.identifier.other0000-0002-1741-6286
dc.identifier.other0000-0002-0844-6563
dc.identifier.other0000-0003-4062-0776
dc.identifier.other0000-0003-3061-4591
dc.identifier.other0000-0001-8218-8542
dc.identifier.other0000-0003-4864-2806
dc.identifier.other0000-0003-1978-9809
dc.identifier.urihttp://hdl.handle.net/20.500.14302/1575
dc.description.abstractNumerous magnetic hot stars exhibit gyrosynchrotron radio emission. The source electrons were previously thought to be accelerated to relativistic velocities in the current sheet formed in the middle magnetosphere by the wind opening magnetic field lines. However, a lack of dependence of radio luminosity on the wind power, and a strong dependence on rotation, has recently challenged this paradigm. We have collected all radio measurements of magnetic early-type stars available in the literature. When constraints on the magnetic field and/or the rotational period are not available, we have determined these using previously unpublished spectropolarimetric and photometric data. The result is the largest sample of magnetic stars with radio observations that has yet been analysed: 131 stars with rotational and magnetic constraints, of which 50 are radio-bright. We confirm an obvious dependence of gyrosynchrotron radiation on rotation, and furthermore find that accounting for rotation neatly separates stars with and without detected radio emission. There is a close correlation between H α emission strength and radio luminosity. These factors suggest that radio emission may be explained by the same mechanism responsible for H α emission from centrifugal magnetospheres, i.e. centrifugal breakout (CBO), however, while the H α-emitting magnetosphere probes the cool plasma before breakout, radio emission is a consequence of electrons accelerated in centrifugally driven magnetic reconnection.
dc.publisherMonthly Notices of the Royal Astronomical Society
dc.titleMOBSTER - VI. The crucial influence of rotation on the radio magnetospheres of hot stars
dc.typearticle
dc.source.journalMNRAS
dc.source.journalMNRAS.513
dc.source.volume513
refterms.dateFOA2024-02-02T13:31:28Z
dc.identifier.bibcode2022MNRAS.513.1429S


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