Show simple item record

dc.contributor.authorJ. Wilkes, Belinda
dc.contributor.authorV. Lal, Dharam
dc.contributor.authorWorrall, D. M.
dc.contributor.authorBirkinshaw, Mark
dc.contributor.authorHaas, Martin
dc.contributor.authorWillner, S. P.
dc.contributor.authorAntonucci, Robert
dc.contributor.authorAshby, M. L. N.
dc.contributor.authorAvara, Mark
dc.contributor.authorBarthel, Peter
dc.contributor.authorChini, Rolf
dc.contributor.authorFazio, G.
dc.contributor.authorHardcastle, M.J.
dc.contributor.authorLawrence, Charles
dc.contributor.authorLeipski, Christian
dc.contributor.authorOgle, Patrick
dc.contributor.authorSchulz, Bernhard
dc.date.accessioned2012-03-27T13:00:34Z
dc.date.available2012-03-27T13:00:34Z
dc.date.issued2012-01-20
dc.identifier.citationJ. Wilkes , B , V. Lal , D , Worrall , D M , Birkinshaw , M , Haas , M , Willner , S P , Antonucci , R , Ashby , M L N , Avara , M , Barthel , P , Chini , R , Fazio , G , Hardcastle , M J , Lawrence , C , Leipski , C , Ogle , P & Schulz , B 2012 , ' Chandra X-ray Observations of the redshift 1.53, radio-loud quasar 3C 270.1 ' , The Astrophysical Journal , vol. 745 , no. 1 , 84 . https://doi.org/10.1088/0004-637X/745/1/84
dc.identifier.issn0004-637X
dc.identifier.otherArXiv: http://arxiv.org/abs/1109.4395v2
dc.identifier.otherORCID: /0000-0003-4223-1117/work/30391008
dc.identifier.urihttp://hdl.handle.net/2299/8061
dc.description20 pages, 7 figures, accepted by ApJ
dc.description.abstractChandra X-ray observations of the high redshift (z =1.532) radio-loud quasar 3C270.1 in 2008 February show the nucleus to have a power-law spectrum, Gamma = 1.66 +/- 0.08, typical of a radio-loud quasar, and a marginally-detected Fe Kalpha emission line. The data also reveal extended X-ray emission, about half of which is associated with the radio emission from this source. The southern emission is co-spatial with the radio lobe and peaks at the position of the double radio hotspot. Modeling this hotspot including Spitzer upper limits rules out synchrotron emission from a single power-law population of electrons, favoring inverse-Compton emission with a field of ~11nT, roughly a third of the equipartition value. The northern emission is concentrated close to the location of a 40 deg. bend where the radio jet is presumed to encounter external material. It can be explained by inverse Compton emission involving Cosmic Microwave Background photons with a field of ~3nT, roughly a factor of nine below the equipartition value. The remaining, more diffuse X-ray emission is harder (HR=-0.09 +/- 0.22). With only 22.8+/-5.6 counts, the spectral form cannot be constrained. Assuming thermal emission with a temperature of 4 keV yields an estimate for the luminosity of 1.8E44 erg/s, consistent with the luminosity-temperature relation of lower-redshift clusters. However deeper Chandra X-ray observations are required to delineate the spatial distribution, and better constrain the spectrum of the diffuse emission to verify that we have detected X-ray emission from a high-redshift cluster.en
dc.format.extent1182133
dc.language.isoeng
dc.relation.ispartofThe Astrophysical Journal
dc.subjectastro-ph.HE
dc.subjectastro-ph.CO
dc.titleChandra X-ray Observations of the redshift 1.53, radio-loud quasar 3C 270.1en
dc.contributor.institutionSchool of Physics, Astronomy and Mathematics
dc.contributor.institutionCentre for Astrophysics Research
dc.description.statusPeer reviewed
rioxxterms.versionofrecord10.1088/0004-637X/745/1/84
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record