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Multi-Wavelength Time Variability of Active Galactic Nuclei Ritaban Chatterjee Advisor: Prof. Alan P. Marscher Collaborators: Svetlana Jorstad (B.U.),

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Presentation on theme: "Multi-Wavelength Time Variability of Active Galactic Nuclei Ritaban Chatterjee Advisor: Prof. Alan P. Marscher Collaborators: Svetlana Jorstad (B.U.),"β€” Presentation transcript:

1 Multi-Wavelength Time Variability of Active Galactic Nuclei Ritaban Chatterjee Advisor: Prof. Alan P. Marscher Collaborators: Svetlana Jorstad (B.U.), Phil Uttley (U. Southampton, UK).

2 β€œAn active galactic nucleus (AGN) is a compact region at the centre of a galaxy which has a much higher than normal luminosity over some or all of the electromagnetic spectrum. The radiation from AGN is believed to be a result of accretion on to a super-massive black hole at the centre of the host galaxy.” -Wikipedia

3 Image courtesy of NRAO/AUI Jets of AGN: kpc and pc scale

4 AGN : Schematic Model Cartoon courtesy: Prof. Alan Marscher

5 Why Time Variability?

6 3C 279 Z=0.536 1 mas = 6.3 pc 3C 279

7 Steps of Time Variability Studies Long-term monitoring in multiple wavelengths and VLBA Power spectral density (PSD) Comparison of flux at different wavelengths : Correlation and light curve decomposition Simulation of time variable non-thermal radiation

8 X-RAY OPTICAL RADIO

9 Steps of Time Variability Studies Long-term monitoring in multiple wavelengths and VLBA Power spectral density (PSD) Comparison of flux at different wavelengths : Correlation and light curve decomposition Simulation of time variable non-thermal radiation

10 Variability in Different Timescales 2000 Days : Years Maximum/Average ~ 2.5 70 Days : Months Maximum/Average ~ 1.5 10 Days : Weeks Maximum/Average ~ 1.3

11 First PSD of nonthermal radiation from AGN jets

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13 PSD Analysis There is higher amplitude variability at longer timescales than at shorter timescales Simulation of artificial light curves for comparison X-ray PSDs of accretion disk systems show characteristic time scale

14 Simulation of Light Curves Using PSD

15 Long-term monitoring in multiple wavelengths and VLBA Power spectral density (PSD) Comparison of flux at different wavelengths : Correlation analysis and light curve decomposition Simulation of time variable non-thermal radiation Steps of Time Variability Studies

16 3C 279 : X-ray-optical Cross-Correlation Optical leads X-ray by ~ 19 Days Chatterjee et al. 2008 (ApJ, 489, 79)

17 Correlation Time Window

18 X-RAY OPTICAL RADIO

19 Long-term monitoring in multiple wavelengths and VLBA Power spectral density (PSD) Comparison of flux at different wavelengths : Correlation analysis and light curve decomposition Simulation of time variable non-thermal radiation Steps of Time Variability Studies

20 Decomposition into flares X-ray light curve : 10-day Gaussian smoothing applied

21 X-ray light curve : Sum of model flares & real data Chatterjee et al. 2008 (ApJ, in press)

22 Optical light curve : Sum of model flares & real data Chatterjee et al. 2008 (ApJ, in press)

23 X-ray and Optical : Superposed 1.Time lag between peaks 2.Power of flares : Area under the curve

24 Time Delay (Days) X/Op Ratio 1.270.4 2.240.62 3.490.67 4.150.44 5.221.4 6.160.18 7.250.38 8.270.3 9.30.95 10.80.98 11.30.87 12.60.88 Larger time delay, Smaller ratio Smaller time delay, Ratio ~1

25 6 out of 12 optical flares have more power than the related X-ray flare. Optical => Synchrotron X-ray=> Synchrotron self-Compton (SSC) => SSC/Synch Puzzling! When x/op ~1, time delay is very small. Summary of correlation and flare decomposition

26 Long-term monitoring in multiple wavelengths and VLBA Power spectral density (PSD) Comparison of flux at different wavelengths : Correlation analysis and light curve decomposition Simulation of time variable non-thermal radiation Modeling of synchrotron (optical) and synchrotron self- Compton (X-ray) flares B ~r -b, N 0 ~r -n, R ~r Steps of Time Variability Studies

27 Real and Simulated Light Curves Red: Optical (Synchrotron), Green: X-ray (SSC)

28 Real and Simulated Light Curves SIMULATEDREAL Red: Optical (Synchrotron), Green: X-ray (SSC)

29 Downstream SSC (Green) maybe smaller than Synchrotron (Red) UPSTREAMDOWNSTREAM

30 Sketch of emission region upstream and downstream x/op~1 x/op<1 UpstreamDownstream

31 Sketch of emission region upstream and downstream βˆ† t smaller x/op~1 βˆ† t larger x/op<1 UpstreamDownstream

32 Time Delay (Days) X/Op Ratio 1.270.4 2.240.62 3.490.67 4.150.44 5.221.4 6.160.18 7.250.38 8.270.3 9.30.95 10.80.98 11.30.87 12.60.88 Larger time delay, Smaller ratio Smaller time delay, Ratio ~1

33 CONCLUSIONS: LOCATION AND MECHANISM OF EMISSION There is higher amplitude variability at longer timescales than at shorter timescales X-ray and optical variations are highly correlated. X-ray/optical correlation changes over time. Contemporaneous X-ray and optical flares: X/OP β‰ˆ 1 => closer to the base of the jet X/OP farther from the base of the jet

34 THE END

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38 Multi-wavelength Light Curves of 3C 120 between 2002 and 2007

39 PSD of Cygnus X-1 : Break Frequency Credit : Uttley et al. (2004)

40 3C 120 PSD with break

41 AGN : Unified Picture


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