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dc.contributor.authorTadhunter, Cliveen_US
dc.contributor.authorSparks, Williamen_US
dc.contributor.authorAxon, Daviden_US
dc.contributor.authorBergeron, Louisen_US
dc.contributor.authorJackson, Nealen_US
dc.contributor.authorPackham, Christopheren_US
dc.contributor.authorHough, Jamesen_US
dc.contributor.authorRobinson, Andrewen_US
dc.contributor.authorYoung, Stuarten_US
dc.date.accessioned2006-05-31T13:25:29Zen_US
dc.date.available2006-05-31T13:25:29Zen_US
dc.date.issued2000-04en_US
dc.identifier.citationMonthly Notices of the Royal Astronomical Society 313 (2000) L52-L56en_US
dc.identifier.issn1365-2966en_US
dc.identifier.urihttp://hdl.handle.net/1850/1897en_US
dc.descriptionRIT community members may access full-text via RIT Libraries licensed databases: http://library.rit.edu/databases/
dc.description.abstractWe present near-IR imaging polarimetry observations of the nucleus of Cygnus A, taken with the NICMOS camera of the HST at a wavelength of 2.0µm. These maps reveal a highly collimated region of polarized emission straddling the nucleus and extending to a radius of 1.2 arcseconds. Remarkably, this feature coincides with one, but only one, limb of the edge-brightened bicone structure seen in the total intensity image. The high degree (Pk 25%) and orientation of the extended polarization feature are consistent with a scattering origin. Most plausibly, the detection of polarization along only one limb of the bicone is a consequence of intrinsic anisotropy of the near-IR continuum within the radiation cones, with the direction of maximum intensity of the near-IR radiation field significantly displaced from the direction of the radio axis. The unresolved nuclear core source is also highly polarized (Pk > 28%), with a position angle close to the perpendicular to the radio axis. Given that this high degree of nuclear polarization can only be explained in terms of dichroic extinction if the dichroic mechanism is unusually efficient in Cygnus A, it is more likely that the nuclear polarization is due to the scattering of nuclear light in an unresolved scattering region close to the AGN. In this case, the flux of the core source in the K-band is dominated by scattered rather than transmitted quasar light, and previous extinction estimates based on K-band photometry of the core substantially underestimate the true nuclear extinction. (Refer to PDF file for exact formulas).en_US
dc.description.sponsorshipBased on Observations made with the ESA/NASA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5- 26555. We thank the referee — Stuart Lumsden — for useful comments. A. Robinson acknowledges support from the Royal Society.en_US
dc.format.extent131347 bytesen_US
dc.format.mimetypeapplication/pdfen_US
dc.language.isoen_USen_US
dc.publisherBlackwell Publishing: Monthly Notices of the Royal Astronomical Societyen_US
dc.relation.ispartofseriesvol. 313en_US
dc.relation.ispartofseriesissue 4en_US
dc.relation.ispartofseriespps. L52-L56en_US
dc.subjectGalaxies-infrareden_US
dc.subjectPolarizationen_US
dc.titleHighly polarized structures in the near-nuclear regions of Cygnus A: Intrinsic anisotropy within the cones?en_US
dc.typeArticleen_US
dc.identifier.urlhttp://dx.doi.org/10.1046/j.1365-8711.2000.03442.x


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