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dc.contributorNew Mexico State University, MSC 3DA, Las Cruces, NM 88003, USA; Picture Rocks Observatory, 1025 S. Solano Dr. Suite D., Las Cruces, NM 88001, USA
dc.contributorFinnish Centre for Astronomy with ESO, Quantum, Vesilinnantie 5, FI-20014, University of Turku, Finland
dc.contributorMullard Space Science Laboratory, University College London, Holmbury St. Mary, Surrey RH5 6NT, UK
dc.contributorDepartment of Physics, The George Washington University, Washington, DC 20052, USA
dc.contributorCentre for Extragalactic Astronomy, Department of Physics, Durham University, South Road, Durham DH1 3LE, UK; Astronomical Observatory, University of Warsaw, Al. Ujazdowskie 4, 00-478 Warsaw, Poland
dc.contributorBay Area Environmental Research Institute, Moffett Field, CA 94035, USA
dc.contributorPicture Rocks Observatory, 1025 S. Solano Dr. Suite D., Las Cruces, NM 88001, USA
dc.contributorInstituto Nacional de Pesquisas Espaciais, Av. dos Astronautas 1758, São José dos Campos, SP 12227-010, Brazil
dc.contributorDepartment of Physics, University of Notre Dame, Notre Dame, IN 46556, USA
dc.contributorDepartment of Astronomy, University of Washington, Seattle, WA 98195, USA
dc.contributorArmagh Observatory and Planetarium, College Hill, Armagh, UK
dc.contributorArmagh Observatory and Planetarium, College Hill, Armagh, UK; Department of Physics, University of Warwick, Gibbet Hill Road, Coventry CV4 7AL, UK
dc.contributorCentre for Extragalactic Astronomy, Department of Physics, Durham University, South Road, Durham DH1 3LE, UK
dc.contributor.authorMason, Paul A.
dc.contributor.authorHakala, Pasi
dc.contributor.authorWu, Kinwah
dc.contributor.authorBarrett, Paul E.
dc.contributor.authorIłkiewicz, Krystian
dc.contributor.authorLittlefield, Colin
dc.contributor.authorMonroy, Lorena C.
dc.contributor.authorSezer, Hasan C.
dc.contributor.authorJablonski, Francisco
dc.contributor.authorGarnavich, Peter
dc.contributor.authorSzkody, Paula
dc.contributor.authorRamsay, Gavin
dc.contributor.authorDuffy, Christopher
dc.contributor.authorScaringi, Simone
dc.date.accessioned2024-05-08T15:37:50Z
dc.date.available2024-05-08T15:37:50Z
dc.date.issued2024-04-01T00:00:00Z
dc.identifier.doi10.3847/1538-4357/ad27d7
dc.identifier.other2024ApJ...965...96M
dc.identifier.other10.3847/1538-4357/ad27d7
dc.identifier.other0000-0002-5897-3038
dc.identifier.other-
dc.identifier.other0000-0002-7568-8765
dc.identifier.other0000-0002-8456-1424
dc.identifier.other0000-0002-4005-5095
dc.identifier.other0000-0001-7746-5795
dc.identifier.other0000-0002-0386-2306
dc.identifier.other0000-0003-4069-2817
dc.identifier.other0000-0003-4373-7777
dc.identifier.other0000-0001-8722-9710
dc.identifier.other0000-0001-6662-0200
dc.identifier.other0000-0001-5387-7189
dc.identifier.urihttp://hdl.handle.net/20.500.14302/2042
dc.description.abstractTransiting Exoplanet Survey Satellite (TESS) photometry of the polars AM Herculis (AM Her) and AR Ursae Majoris (AR UMa) is presented, along with high-speed photometry. AM Her shows a variety of high states with frequent transitions between them. TESS photometry of AR UMa in the low state reveals no evidence of accretion, while the McDonald 2.1 m telescope caught AR UMa in its high accretion state. Roche-lobe overflow is shut off during low states of AR UMa, while accretion often still takes place during low states of AM Her. We derive inclinations of 50° and 70° for AM Her and AR UMa respectively. To model the high-state light curves of AM Her, we employ a self-organized map light-curve classification scheme to establish common accretion configurations. The cyclotron radiation properties then allow the production of emission region maps on the surface of the white dwarf. The accretion geometry of AM Her is most consistent with a multipolar field structure. The high-state photometry of AR UMa has stochastic accretion flaring, which we attribute to magnetically buffeted mass transfer through the inner Lagrangian point L1. To consider this possibility, we examine the magnetism of both stars and argue that the local magnetic field near L1 can initiate short-lived accretion events and affect transitions between high and low accretion states in both AM Her and AR UMa. In particular, AR UMa has the low state as its default, while AM Her and most other active polars are in the high state by default.
dc.publisherThe Astrophysical Journal
dc.titleTESS Photometry of AM Her and AR UMa: Binary Parameters, Cyclotron Emission Modeling, and Mass Transfer Duty Cycles
dc.typearticle
dc.source.journalApJ
dc.source.journalApJ...965
dc.source.volume965
dc.identifier.bibcode2024ApJ...965...96M


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