First Sagittarius A* Event Horizon Telescope Results. VIII. Physical Interpretation of the Polarized Ring

dc.contributor.authorAkiyama K
dc.contributor.organizationfi=Suomen ESO-keskus|en=Finnish Centre for Astronomy with ESO|
dc.contributor.organizationfi=Tuorlan observatorio|en=Tuorla Observatory|
dc.contributor.organization-code1.2.246.10.2458963.20.54954054844
dc.contributor.organization-code1.2.246.10.2458963.20.90670098848
dc.converis.publication-id387502422
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/387502422
dc.date.accessioned2025-08-28T02:13:05Z
dc.date.available2025-08-28T02:13:05Z
dc.description.abstractIn a companion paper, we present the first spatially resolved polarized image of Sagittarius A* on event horizon scales, captured using the Event Horizon Telescope, a global very long baseline interferometric array operating at a wavelength of 1.3 mm. Here we interpret this image using both simple analytic models and numerical general relativistic magnetohydrodynamic (GRMHD) simulations. The large spatially resolved linear polarization fraction (24%–28%, peaking at ∼40%) is the most stringent constraint on parameter space, disfavoring models that are too Faraday depolarized. Similar to our studies of M87*, polarimetric constraints reinforce a preference for GRMHD models with dynamically important magnetic fields. Although the spiral morphology of the polarization pattern is known to constrain the spin and inclination angle, the time-variable rotation measure (RM) of Sgr A* (equivalent to ≈46° ± 12° rotation at 228 GHz) limits its present utility as a constraint. If we attribute the RM to internal Faraday rotation, then the motion of accreting material is inferred to be counterclockwise, contrary to inferences based on historical polarized flares, and no model satisfies all polarimetric and total intensity constraints. On the other hand, if we attribute the mean RM to an external Faraday screen, then the motion of accreting material is inferred to be clockwise, and one model passes all applied total intensity and polarimetric constraints: a model with strong magnetic fields, a spin parameter of 0.94, and an inclination of 150°. We discuss how future 345 GHz and dynamical imaging will mitigate our present uncertainties and provide additional constraints on the black hole and its accretion flow.
dc.identifier.eissn2041-8213
dc.identifier.jour-issn2041-8205
dc.identifier.olddbid208754
dc.identifier.oldhandle10024/191781
dc.identifier.urihttps://www.utupub.fi/handle/11111/58409
dc.identifier.urlhttps://dx.doi.org/10.3847/2041-8213/ad2df1
dc.identifier.urnURN:NBN:fi-fe2025082788086
dc.language.isoen
dc.okm.affiliatedauthorRamakrishnan, Venkatessh
dc.okm.affiliatedauthorWiik, Kaj
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherInstitute of Physics Publishing
dc.publisher.countryUnited Kingdomen_GB
dc.publisher.countryBritanniafi_FI
dc.publisher.country-codeGB
dc.relation.articlenumberL26
dc.relation.doi10.3847/2041-8213/ad2df1
dc.relation.ispartofjournalAstrophysical Journal Letters
dc.relation.issue2
dc.relation.volume964
dc.source.identifierhttps://www.utupub.fi/handle/10024/191781
dc.titleFirst Sagittarius A* Event Horizon Telescope Results. VIII. Physical Interpretation of the Polarized Ring
dc.year.issued2024

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