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dc.contributor.authorHarris, Daniel E.
dc.contributor.authorCheung, Chi C.
dc.contributor.authorStawarz, Łukasz
dc.contributor.authorBiretta, J. A.
dc.contributor.authorPerlman, Eric S.
dc.date.accessioned2014-12-01T19:41:23Z
dc.date.available2014-12-01T19:41:23Z
dc.date.issued2009-06-11
dc.identifier.citationBiretta, J.A., Cheung, C.C., Harris, D.E., Perlman, E.S., & Stawarz, Ł. (2009) Variability timescales in the M87 jet: signatures of E^2 losses, discovery of a quasi period in HST-1, and the site of TeV flaring. The Astrophysical Journal, 699(1), 305.en_US
dc.identifier.urihttp://hdl.handle.net/11141/446
dc.description.abstractWe investigate the variability timescales in the jet of M87 with two goals. The first is to use the rise times and decay times in the radio, ultraviolet, and X-ray light curves of HST-1 to constrain the source size and the energy loss mechanisms affecting the relativistic electron distributions. HST-1 is the first jet knot clearly resolved from the nuclear emission by Chandra and is the site of the huge flare of 2005. We find clear evidence for a frequency-dependent decrease in the synchrotron flux being consistent with E 2 energy losses. Assuming that this behavior is predominantly caused by synchrotron cooling, we estimate a value of 0.6 mG for the average magnetic field strength of the HST-1 emission region, a value consistent with previous estimates of the equipartition field. In the process of analyzing the first derivative of the X-ray light curve of HST-1, we discovered a quasi-periodic oscillation which was most obvious in 2003 and 2004 prior to the major flare in 2005. The four cycles observed have a period of order six months. The second goal is to search for evidence of differences between the X-ray variability timescales of HST-1 and the unresolved nuclear region (diameter <0farcs6). These features, separated by more than 60 pc, are the two chief contenders for the origin of the TeV variable emissions observed by H.E.S.S. in 2005 and by MAGIC and VERITAS in 2008. The X-ray variability of the nucleus appears to be at least twice as rapid as that of the HST-1 knot. However, the shortest nuclear variability timescale we can measure from the Chandra data (≤20 days) is still significantly longer than the shortest TeV variability of M87 reported by the H.E.S.S. and MAGIC telescopes (1-2 days).en_US
dc.language.isoen_USen_US
dc.rightsThis published article is available in accordance with the publisher's policy. It may be subject to U.S. Copyright Law.en_US
dc.rights.urihttp://aas.org/publications/aas-copyright-policyen_US
dc.titleVariability timescales in the M87 jet: signatures of E^2 losses, discovery of a quasi period in HST-1, and the site of TeV flaringen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/0004-637X/699/1/305


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