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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).
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βAn 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.β -Wikipedia
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Image courtesy of NRAO/AUI Jets of AGN: kpc and pc scale
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AGN : Schematic Model Cartoon courtesy: Prof. Alan Marscher
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Why Time Variability?
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3C 279 Z=0.536 1 mas = 6.3 pc 3C 279
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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
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X-RAY OPTICAL RADIO
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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
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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
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First PSD of nonthermal radiation from AGN jets
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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
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Simulation of Light Curves Using PSD
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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
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3C 279 : X-ray-optical Cross-Correlation Optical leads X-ray by ~ 19 Days Chatterjee et al. 2008 (ApJ, 489, 79)
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Correlation Time Window
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X-RAY OPTICAL RADIO
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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
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Decomposition into flares X-ray light curve : 10-day Gaussian smoothing applied
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X-ray light curve : Sum of model flares & real data Chatterjee et al. 2008 (ApJ, in press)
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Optical light curve : Sum of model flares & real data Chatterjee et al. 2008 (ApJ, in press)
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X-ray and Optical : Superposed 1.Time lag between peaks 2.Power of flares : Area under the curve
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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
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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
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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
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Real and Simulated Light Curves Red: Optical (Synchrotron), Green: X-ray (SSC)
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Real and Simulated Light Curves SIMULATEDREAL Red: Optical (Synchrotron), Green: X-ray (SSC)
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Downstream SSC (Green) maybe smaller than Synchrotron (Red) UPSTREAMDOWNSTREAM
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Sketch of emission region upstream and downstream x/op~1 x/op<1 UpstreamDownstream
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Sketch of emission region upstream and downstream β t smaller x/op~1 β t larger x/op<1 UpstreamDownstream
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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
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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 1 => closer to the base of the jet X/OP farther from the base of the jet
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THE END
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Multi-wavelength Light Curves of 3C 120 between 2002 and 2007
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PSD of Cygnus X-1 : Break Frequency Credit : Uttley et al. (2004)
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3C 120 PSD with break
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AGN : Unified Picture
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