Magnetic field at a jet base: extreme Faraday rotation in 3C 273 revealed by ALMA

dc.contributor.authorT. Hovatta
dc.contributor.authorS. O'Sullivan
dc.contributor.authorI. Martí-Vidal
dc.contributor.authorT. Savolainen
dc.contributor.authorA. Tchekhovskoy
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-id39807455
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/39807455
dc.date.accessioned2025-08-27T23:46:54Z
dc.date.available2025-08-27T23:46:54Z
dc.description.abstractAims. We studied the polarization behavior of the quasar 3C 273 over the 1 mm wavelength band at ALMA with a total bandwidth of 7.5 GHz across 223-243 GHz at 0.8 '' resolution, corresponding to 2.1 kpc at the distance of 3C 273. With these observations we were able to probe the optically thin polarized emission close to the jet base, and constrain the magnetic field structure.Methods. We computed the Faraday rotation measure using simple linear fitting and Faraday rotation measure synthesis. In addition, we modeled the broadband behavior of the fractional Stokes Q and U parameters (qu-fitting). The systematic uncertainties in the polarization observations at ALMA were assessed through Monte Carlo simulations.Results. We find the unresolved core of 3C 273 to be 1.8% linearly polarized. We detect a very high rotation measure (RM) of (5.0 +/- 0.3) x 10(5) rad m(-2) over the 1 mm band when assuming a single polarized component and an external RM screen. This results in a rotation of >40 degrees of the intrinsic electric vector position angle, which is significantly higher than typically assumed for millimeter wavelengths. The polarization fraction increases as a function of wavelength, which according to our qu-fitting could be due to multiple polarized components of different Faraday depth within our beam or to internal Faraday rotation. With our limited wavelength coverage we cannot distinguish between the cases, and additional multi-frequency and high angular resolution observations are needed to determine the location and structure of the magnetic field of the Faraday active region. Comparing our RM estimate with values obtained at lower frequencies, the RM increases as a function of observing frequency, following a power law with an index of 2.0 +/- 0.2, consistent with a sheath surrounding a conically expanding jet. We also detect similar to 0.2% circular polarization, although further observations are needed to confirm this result.
dc.identifier.eissn1432-0746
dc.identifier.jour-issn0004-6361
dc.identifier.olddbid204601
dc.identifier.oldhandle10024/187628
dc.identifier.urihttps://www.utupub.fi/handle/11111/53100
dc.identifier.urnURN:NBN:fi-fe2021042825428
dc.language.isoen
dc.okm.affiliatedauthorHovatta, Talvikki
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.publisherEDP SCIENCES S A
dc.publisher.countryFranceen_GB
dc.publisher.countryRanskafi_FI
dc.publisher.country-codeFR
dc.relation.articlenumberARTN A111
dc.relation.doi10.1051/0004-6361/201832587
dc.relation.ispartofjournalAstronomy and Astrophysics
dc.relation.volume623
dc.source.identifierhttps://www.utupub.fi/handle/10024/187628
dc.titleMagnetic field at a jet base: extreme Faraday rotation in 3C 273 revealed by ALMA
dc.year.issued2019

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