Probing the Inner Jet of the Quasar PKS 1510  089 with Multi-waveband Monitoring Alan Marscher Boston University Research Web Page: www.bu.edu/blazars.

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Presentation transcript:

Probing the Inner Jet of the Quasar PKS 1510  089 with Multi-waveband Monitoring Alan Marscher Boston University Research Web Page:

Main Collaborators in the Study Svetlana Jorstad (Boston University) Valery Larionov (St. Petersburg State U., Russia) Ivan Agudo (IAA, Spain) Margo Aller (U. Michigan) Paul Smith (Steward Obs.) Anne Lähteenmäki (Metsähovi Radio Obs.) Funded by NASA (Fermi & ADP grants) & NSF Svetlana Jorstad (Boston University) Valery Larionov (St. Petersburg State U., Russia) Ivan Agudo (IAA, Spain) Margo Aller (U. Michigan) Paul Smith (Steward Obs.) Anne Lähteenmäki (Metsähovi Radio Obs.) Funded by NASA (Fermi & ADP grants) & NSF

Long-term connection between X-ray & radio Optical flux not so well correlated with radio, X-ray Marscher et al. (2009, Astrophysical Journal, submitted) X-rays Radio waves 5000 The Quasar PKS (z=0.361) Conclusion: X-rays are mainly external Compton by low-E electrons - supports Madejski et al. & Kataoka et al.

Two bright superluminal blobs emerged during the outbursts in brightness during the 2nd half of 2008 & the 1st half of GHz VLBA Images of PKS Marscher et al. (2009, Astrophysical Journal, submitted) Contours: intensity Colors: polarization V app = 23c

Simultaneous  -ray & optical flares but relative amplitudes & lags vary Marscher et al. (2009, Astrophysical Journal, submitted)  -ray Blazar PKS Flux JD Superluminal knot passed through core during largest optical flare (day 4962)

Rotation of Optical Polarization in PKS Time when blob passed through core Direction of optical polarization Very sharp, high-amplitude, strongly polarized optical (+  -ray) flare at end of rotation as new superluminal blob passed through core Rotation by ~ 720° during spring 2009 outburst

BL Lac: pol. rotation, blob first seen upstream of core X-rayOptical polarization angle rotated smoothly during 1st flare, then became same as that of blob TeV  -ray data: Albert et al. (2007, ApJL, 666, L17 Marscher et al. (2008, Nature, 452, 966) X-rays  -rays Visible Light Radio waves VLBA 43 GHz Late 2005: Double optical/X-ray flare, detection at TeV  -ray energies

BL Lac: Physical Picture Moving blob/shock follows spiral streamline through toroidal magnetic field in zone where the flow of the jet accelerates + becomes focused Physical Picture of BL Lac: As Predicted* *Vlahakis (2006, in Variability of Blazars: Entering the GLAST Era) Site of flare 1 Site of flare 2 Marscher et al. (2008, Nature, 452, 966) Polarization direction rotates as blob passes through different magnetic field orientations Blob enters standing shock wave in core, causing flare 2

BL Lac: Physical Picture Feature covers much of jet cross-section, but not all Centroid is off-center  Net B rotates as feature moves down jet, P perpendicular to B Emission feature following spiral path down jet P vector B net

Rotation of Optical Polarization in PKS Rotation starts when major optical activity begins Rotation ends when major optical activity ends + superluminal blob passes through core Direction of optical polarization Time when blob passed through core Flux Polarization Optical Curve: emission feature following a spiral path in an accelerating flow  increases from 8 to 24,  from 15 to 38 Core = 17 pc from central engine Blob moves 0.3 pc/day as it approaches core - Timing argues against rotation resulting from random walk caused by turbulence -Also, polarization rotation from days 4990 to 5000 similar to end of earlier rotation, as expected if caused by geometry of B as a weak blob approaches core

Sharp flare on day 4962 probably SSC (1st + 2nd order) as blob is compressed by standing shock wave inside core Flares with high  :opt ratios occur as blob passes location of *local* source of external seed photons, L ext ~ 3x10 43 erg/s  1st flare: BLR?  Later: synchrotron in slower sheath of jet? B ~ 1 G at start, G at core (from timescale of flare decay) Flares during 1st Half of 2009 in PKS Interpretation: All flares in 2009 caused by a single superluminal blob moving down jet  -ray to optical flux ratios vary greatly from flare to flare - from ~70 on day 4847 to <10 on days 4928 & 4962

Conclusions  -ray and X-ray flares in jets are caused by superluminal knots (“blobs”) that move down the jet & are seen in VLBA images - See also poster by Svetlana Jorstad today Relativistic jets of AGN are connected to black hole & accretion disk - Disturbances creating superluminal knots + outbursts in brightness start in the central engine near the supermassive black hole Rotations of polarization & timing of flares agree with magnetic- launching models of jets High-E photon emission in the jet occurs by both SSC & EC in multiple zones, sometimes because electrons are energized & radiate more, other times because electrons in jet encounter extra light from local sources (probably sheath) & knock it up to high energies Combination of VLBA imaging + multi-waveband flux & polarization monitoring is a powerful probe of inner jets of blazars

PKS : Flare in Aug-Sep 2008 Time delays of peaks: Optical first  -ray 1 week later X-ray & radio 10 days after  -ray Superluminal knot (red arrow) passed through core before this flare AGILE detection early in 2008 during optical flaring activity, at start of X- ray/radio rise Marscher et al. (2009, Astrophysical Journal, submitted) Flux