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Quasar Jet Surveys with Chandra Herman L. Marshall (MIT) D. - PowerPoint PPT Presentation

Quasar Jet Surveys with Chandra Herman L. Marshall (MIT) D. Schwartz, D. WorralL, M. Birkinshaw (SAO) M. Lister, B. Hogan, P. Kharb (Purdue) & J. Gelbord, E. Perlman, L. Godfrey, J. Lovell, etc. Schwartz et al. 2000 CXC Marshall et al.


  1. Quasar Jet Surveys with Chandra Herman L. Marshall (MIT) D. Schwartz, D. WorralL, M. Birkinshaw (SAO) M. Lister, B. Hogan, P. Kharb (Purdue) & J. Gelbord, E. Perlman, L. Godfrey, J. Lovell, etc. Schwartz et al. 2000 CXC Marshall et al. 2001

  2. Overview • History of FR II jet surveys using Chandra • Results from 2 recent surveys • Individual studies • see also poster by Leith Godfrey HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 2

  3. Overview • History of FR II jet surveys using Chandra • Results from 2 recent surveys • Individual studies • see also poster by Leith Godfrey HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 2

  4. First Chandra Jet • Observed for focussing Schwartz et al. 2000 Contours: Radio Color: X-ray • Jet flux is 7% of core flux • 3C 273: 0.5% in jet • Optical jet emission is weak Contours: Radio Color: Optical • Rules out simple synchrotron • Rules out SSC l e d o m • Inverse Compton of CMB n o r t o r h c n • Jet is 10° to line of sight B y M S C f f o C I • Bulk Γ ~ 15 C S S • Γ , θ like pc scale VLBI HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 3

  5. First Chandra Jet • Observed for focussing Schwartz et al. 2000 Contours: Radio Color: X-ray • Jet flux is 7% of core flux • 3C 273: 0.5% in jet • Optical jet emission is weak Contours: Radio Color: Optical • Rules out simple synchrotron • Rules out SSC l e d o m • Inverse Compton of CMB n o r t o r h c n • Jet is 10° to line of sight B y M S C f f o C I • Bulk Γ ~ 15 C S S • Γ , θ like pc scale VLBI HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 3

  6. First Chandra Jet • Observed for focussing Schwartz et al. 2000 Contours: Radio Color: X-ray • Jet flux is 7% of core flux • 3C 273: 0.5% in jet • Optical jet emission is weak Contours: Radio Color: Optical • Rules out simple synchrotron • Rules out SSC l e d o m • Inverse Compton of CMB n o r t o r h c n • Jet is 10° to line of sight B y M S C f f o C I • Bulk Γ ~ 15 C S S • Γ , θ like pc scale VLBI HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 3

  7. IC-CMB Method • See Tavecchio+ ’00, Celotti+ ’01, Dermer ’95 • Based on blazar core modeling • superluminal motion --> high Γ , small θ • Doppler factor is large δ = 1 / (Γ[1 − β cos θ ]) • Estimate B’ me in jet frame • based on B me in observed frame B ′ me = B me /δ • B me depends (weakly) on L r , V of a jet knot • Assume L x is iC from CMB: u B = B 2 L S = ν r S r = u B 8 π = a [(1 + z ) T ] 4 Γ 2 L S ≅ aT 4 (1 + z ) 4 δ 2 ν r S r L IC ν x S x u ν L IC ν x S x • Match B to B’ me , giving δ from observables HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 4

  8. Jet Surveys • Selected from VLA, ATCA maps of FSRQs • Sambruna+ 2004 • 17 objects, 10 detected in 10 ks snapshots • Marshall+ 2005, 2011, & in prep. • 56 sources, 5 ks snapshots • 32/51 detected, some overlap with Sambuna+ • Hogan+ 2011 — selected from MOJAVE • 21/27 detected, some overlap with M+ • Cheung+ 2007, Saez+ 2011 — 3 at z > 4 • Total: 48/78 = 61.5% (z<2.5), HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 5

  9. Survey Examples HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 6

  10. Jet Survey Results I • S x /S r distribution is broad • <S x /S r > depends weakly on z • IC-CMB: <S x /S r > ∝ (1+z) α +3 , but not found HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 7

  11. Jet Survey Results I • S x /S r distribution is broad • <S x /S r > depends weakly on z • IC-CMB: <S x /S r > ∝ (1+z) α +3 , but not found HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 7

  12. Mojave Survey Hogan+ 2011 • Sample from MOJAVE list • VLBI: pc-scale jet motion • Chandra survey: IC-CMB model constraints • Jets likely bend by few degrees from pc to kpc • Deceleration is most likely HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 8

  13. Deeper Imaging I • Deep X-ray imaging: more X-rays between knots • PKS1136: decelerating by entrainment (Tavecchio 05) Sambruna et al. 2006 Sambruna et al. 2006 HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 9

  14. Deeper Imaging II • Radio-OIR fits simple synchrotron • X-ray peak fit by IC- Godfrey+ ’11 CMB after bend • knot is elongated along jet • total power --> e+/e- • Γ = 6 HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 10

  15. Deepest Imaging Jester+ ’06 3C 273 Siemiginowska+ ’07 PKS 1127-145 Harris + ’11 4C 19.44 Schwartz+ ’06 Q1055+201 HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 11

  16. 3C 273 Jet 2nd part • Width changes along jet • A1, B1: point-like • Rest is broad channel • Spectral indices differ • Spine-sheath structure? Marshall et al. 2006 Jester et al. 2006 HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 12 Jester et al. 2006

  17. Bonus: Pictor A • New radio map, HST images • Galactic tidal tail, long offset 1.6 µ knot in jet HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 13

  18. Bonus: Pictor A • New radio map, HST images • Galactic tidal tail, long offset 1.6 µ knot in jet HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 13

  19. Summary • Chandra surveys: jets in 60% of FSRQs (z<2.5) • Distribution of S x /S r is broad • Dependence on z is not obvious • Angles to line of sight larger than on pc scale • Some jets are relativistic on Mpc scales • Follow-ups provide details • IC-CMB fits for many knots --> gives B, Γ • Deceleration, entrainment likely • Radio/X-ray offsets, α x are problematic • Need large survey with z>2.5, z>4 • Need UV, X-ray polarization HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 14

  20. Barcelona HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15 15

  21. Barcelona 15 Montserrat HEPRO 3 — June 30, 2011 Marshall — Quasar Jets /15

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