the continuing saga of the explosive event(s) in the m87 jet d. e. harris, sao

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The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO collaborators/co-authors C. C. Cheung J. A. Biretta F. Aharonian L. Stawarz E. S. Perlman S. Wagner W. Sparks D. Horn A. S. Wilson K. Mannheim T. Bretz

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The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO. collaborators/co-authors C. C. Cheung J. A. Biretta F. Aharonian L. Stawarz E. S. Perlman S. Wagner W. Sparks D. Horn - PowerPoint PPT Presentation

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Page 1: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

The continuing saga of the explosive event(s) in the M87

jet D. E. Harris, SAO

collaborators/co-authorsC. C. Cheung J. A. Biretta F. Aharonian

L. Stawarz E. S. Perlman S. Wagner

W. Sparks D. Horn

A. S. Wilson K. Mannheim

T. Bretz

H. Krawczynski

R. Mukherjee

V. Vassiliev

J. Carson

Page 2: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Reminder: when viewing radio -

We think we see (distorted) view of emitting volumes containing relativistic electrons and magnetic fields.

• ‘distorted’ shape from projection effects & aberration• ‘distorted’ intensity from relativistic beaming

Page 3: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

When viewing an X-ray image -

In addition to the same attributes as the radio,• We are viewing acceleration regions: I.e. high

energy electrons are being produced throughout the emitting volume.

Page 4: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

outline

UV/HST image, J. Madrid & W. Sparks

Part I: X-ray LC of core, HST-1, knots D & A. - caveats are the instrumental effects.

Part II: Superluminal proper motions of radio components within HST-1.

Part III: The TeV connection.

Page 5: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Photometry

• Straightforward to separate core & HST-1 when there is no pileup - model the PSF w. ChaRT.

• First order recovery of piled events: weight each event w. its energy and sum 0.2-17keV; use evt1 file with no grade filtering (mitigate effects of grade migration)

Page 6: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

keV/s light curves for core, HST1, knots D and A

Page 7: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Bleeding from release of trapped charge at readout time

Page 8: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Instrumental Problems

• Subtract 5% of HST-1 from the core.

• Bleeding from one side of PSF: release of trapped charge (not modeled).

• Other losses include ETN (eat-thy-neighbor), on-board filtering, and bits of piled events which are outside 3x3 pixel region.

Page 9: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Readout Streak Photometry

• Lousy s/n: we get the equivalent of 18s of CC mode from a 5ks observation by measuring ~40 rows. Background is high.

• Apparently, true peak is significantly higher than what we had thought.

Page 10: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

The Radio Side

• Started VLA in 2003• To avoid data gaps

when VLA is in C & D arrays, started VLBA in 2005.

Page 11: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Superluminal Proper Motions

• The inner (vlba) jet is not known to be superluminal.

• HST-1 has ß=v⁄c≈4 for some components.

Page 12: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

HST-1

• 4 epochs shown between 2005.0 and 2006.5 (we have about a dozen; more coming)

• New bits getting resolved and downstream bit moving

Page 13: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Trajectories on the sky

• A (blue) at 2.5c, then decelerates to 1.4c

• B (green) trails A, same velocity, but different PA.

• C (red & magenta) splits into 2 components with c1 (magenta) moving faster, at 4.30.7.

Page 14: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

The TeV connection

HESS group reported a higher gamma ray flux in 2005. They argued that because of rapid variability, the likely origin was the nucleus (close to SMBH) in spite of apparent similarity of X-ray and -ray light curves.

Page 15: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Evidence that the HESS -rays originated in HST-1 rather than from

the nuclear region.• The X-ray LC for HST-1 peaked at the same time as the

-ray high state. • IC is a mandatory process of any relativistic plasma:

both starlight and the synchrotron spectrum are most prominent ≈1014 Hz; TeV emission is expected from =106 electrons, and the expected intensity is approximately what was observed.

• The IC and synchrotron spectral indices have similar values.

• The photon-photon opacity for the alternate location near the SMBH is much greater than 1.

Page 16: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

Short Timescale Variability

As often happens, the data are ambiguous. In principle we could use similarities in light curves to decide the origin of the -rays. In practice, there is not enough overlap.

Page 17: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

To what extent is M87 a Blazar?

Defining characteristics: • Large change of amplitude (“flare”);

• Associated generation of superluminal blobs;

• Associated VHE emission.

Idiosyncrasies:• M87 timescale is longer than typical blazar

Page 18: The continuing saga of the explosive event(s) in the M87 jet D. E. Harris, SAO

Girdwood - 2007 May 21

FIN

Nature has been fairly kind: after we find something unique like the first pulsar, we then find many more and are able to study the class of these objects. In the case of M87, it thus seems either the flare of 2005 is unique and we now have to search for similar events in other jets (nothing like this has so far been detected in the Cen A jet, despite many observations over many years), OR it is just an individual member of a known class (e.g. blazars), albeit with some extreme values.