Book contents
- Frontmatter
- Contents
- Index of Participants
- Preface
- I Evidence and Implications of Anisotropy in AGN
- II Luminosity Functions and Continuum Energy Distributions
- III The Broad Line Region: Variability and Structure
- IV X-rays and Accretion Disks
- V Beams, Jets and Blazars
- Magnetic Propulsion of Jets in AGN
- MHD Accretion-Ejection Model: X- and γ-rays and Formation of Relativistic Pair Beams
- Relativistic Electron Beams in AGN: Construction of Transonic Solutions
- Properties of Relativistic Jets
- A Massive Binary Black Hole in 1928+738?
- Gamma-Rays from Blazars: a Comparison of 3C 279, PKS 0537-441 and Mrk 421
- Microquasars in the Galactic Centre Region
- A Comparison of the Ultra-violet Continuum Variability Properties of Blazars and Seyfert 1s
- Simultaneous Optical and IR Monitoring of the Seyfert Nucleus NGC 7469
- Broad-Band Spectra and Polarization Properties of Variable Flat-Spectrum Radio Sources
- The Radio to Optical Variability of the BL Lac Object ON 231
- January 1992 Microvariability Campaign of OJ 287
- Blazar Microvariability: a Case Study of AO 0235+164
- Timescales of the Optical Variability of the BL Lacertae Galaxy PKS 2201+044
- Dynamics of Quasar Variability
- The Variability of a Large Sample of Quasars
- The Fate of Central Black Holes in Merging Galaxies
- Polarimetric Searching for Goldstone Bosons from AGNs
- VI Concluding Talk
Dynamics of Quasar Variability
from V - Beams, Jets and Blazars
Published online by Cambridge University Press: 04 August 2010
- Frontmatter
- Contents
- Index of Participants
- Preface
- I Evidence and Implications of Anisotropy in AGN
- II Luminosity Functions and Continuum Energy Distributions
- III The Broad Line Region: Variability and Structure
- IV X-rays and Accretion Disks
- V Beams, Jets and Blazars
- Magnetic Propulsion of Jets in AGN
- MHD Accretion-Ejection Model: X- and γ-rays and Formation of Relativistic Pair Beams
- Relativistic Electron Beams in AGN: Construction of Transonic Solutions
- Properties of Relativistic Jets
- A Massive Binary Black Hole in 1928+738?
- Gamma-Rays from Blazars: a Comparison of 3C 279, PKS 0537-441 and Mrk 421
- Microquasars in the Galactic Centre Region
- A Comparison of the Ultra-violet Continuum Variability Properties of Blazars and Seyfert 1s
- Simultaneous Optical and IR Monitoring of the Seyfert Nucleus NGC 7469
- Broad-Band Spectra and Polarization Properties of Variable Flat-Spectrum Radio Sources
- The Radio to Optical Variability of the BL Lac Object ON 231
- January 1992 Microvariability Campaign of OJ 287
- Blazar Microvariability: a Case Study of AO 0235+164
- Timescales of the Optical Variability of the BL Lacertae Galaxy PKS 2201+044
- Dynamics of Quasar Variability
- The Variability of a Large Sample of Quasars
- The Fate of Central Black Holes in Merging Galaxies
- Polarimetric Searching for Goldstone Bosons from AGNs
- VI Concluding Talk
Summary
Introduction
We have heard many times during this conference that variability is a powerful tool to investigate the nature of AGN. The goal of this talk is to demonstrate that the clues derived from variability studies may be partial, disappointing and even misleading, if some characteristics of variability are overlooked and the proper statistical tools are not adopted. To convince you that such a caveat, although obvious, is important and productive, we should like to focus on a few issues, particularly important from our point of view.
The stochastic nature of the light curves
First of all, let's draw your attention to the fact that light curves of quasars have generally random behaviour, i.e., that the knowledge of the value of a time series at a given instant does not allow (in a broad sense) one to forecast the future evolution of the light curve. What does it mean from a physical point of view? It means that quasars are dynamical systems of high dimensionality, systems whose temporal evolution is described by an extremely large set of differential equations (or by partial differential equations). In other words, quasars are dynamical systems whose evolution is determined by a large number of external factors. To understand this point let us consider an example close to common sense: a pendulum. As is well known, the temporal evolution of such a system is described by a second order ordinary differential equation.
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- The Nature of Compact Objects in Active Galactic NucleiProceedings of the 33rd Herstmonceux Conference, held in Cambridge, July 6-22, 1992, pp. 412 - 415Publisher: Cambridge University PressPrint publication year: 1994