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Relative Timing of Variability of Blazars at X‐Ray and Lower Frequencies

dc.contributor.authorMarscher, Alan P.en_US
dc.contributor.authorJorstad, Svetlana G.en_US
dc.contributor.authorAller, Margo F.en_US
dc.contributor.authorMcHardy, Ian M.en_US
dc.contributor.authorBalonek, Thomas J.en_US
dc.contributor.authorTeräsranta, Harrien_US
dc.contributor.authorTosti, Ginoen_US
dc.date.accessioned2011-11-15T16:10:18Z
dc.date.available2011-11-15T16:10:18Z
dc.date.issued2004-07-05en_US
dc.identifier.citationMarscher, Alan P.; Jorstad, Svetlana G.; Aller, Margo F.; McHardy, Ian; Balonek, Thomas J.; Teräsranta, Harri; Tosti, Gino (2004). "Relative Timing of Variability of Blazars at X‐Ray and Lower Frequencies." AIP Conference Proceedings 714(1): 167-173. <http://hdl.handle.net/2027.42/87866>en_US
dc.identifier.otherAPCPCS-714-1en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/87866
dc.description.abstractThe rich X‐ray light curves of blazars obtained with RXTE allow meaningful correlation analyses with longer wavelengths. This reveals strong connections of variations across the electromagnetic spectrum. In 3C 279, PKS 1510‐089, and BL Lac, the characteristics of the X‐ray variability change along with the projected direction of the compact jet. Outbursts in the radio, IR, or optical often precede flares at high energies. A period of pronounced variability in BL Lac in late 2000 occurs at both optical and X‐ray frequencies, with the X‐ray spectral index steepening. A superluminal radio knot is ejected during this event. The implication of our monitoring results is that the IR to X‐ray (as well as γ‐ray) emission is cospatial with the compact radio jet, most likely occurring in the superluminal knots. In the radio galaxy 3C 120, in which the X‐rays probably come mainly from a hot accretion‐disk corona, the appearance of superluminal radio knots follows (by 4 weeks) dips in the X‐ray emission, as in microquasars but on longer timescales. The delay implies that the core of the radio jet, as seen in mm‐wave VLBA images, lies at least 0.4 pc from the central engine, consistent with models in which the jet flow accelerates far from the black hole. The quasar 3C 273 may be an interesting hybrid case in which contributions to the X‐ray emission may come from both the jet and corona. The power spectral density has a low‐frequency break that, in analogy with black‐hole binary systems, implies a mass of the central black hole of 3 – 6 × 108 M☉, similar to that obtained by reverberation mapping of emission‐line variability. © 2004 American Institute of Physicsen_US
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleRelative Timing of Variability of Blazars at X‐Ray and Lower Frequenciesen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/87866/2/167_1.pdf
dc.identifier.doi10.1063/1.1781021en_US
dc.identifier.sourceX-RAY TIMING 2003: Rossie and Beyonden_US
dc.owningcollnamePhysics, Department of


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