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Variability: from X-ray binaries to AGN

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The remarkable connection between BHXRB and AGN X-ray variability. Caveats and surprises (AGN are different in at least one respect... – PowerPoint PPT presentation

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Title: Variability: from X-ray binaries to AGN


1
Variability from X-ray binaries to AGN
  • Phil Uttley
  • University of Southampton
  • With thanks to Ian McHardy, Patricia Arévalo

2
Overview
  • The remarkable connection between BHXRB and AGN
    X-ray variability
  • Caveats and surprises (AGN are different in at
    least one respect)
  • Interpreting AGN continuum spectral
    variability evidence for multiple variability
    time-scales,

3
X-ray variability in accreting black hole systems
4
Black hole XRB spectral states
(Done Gierlinski 2007)
5
Quantifying variability thepower spectrum
(PSD) of Cyg X-1
Soft state Hard state


6
A gallery of black hole XRB PSDs
Done Gierlinski 2005
7
The origin of the variability
  • Bottom line its fluctuations in the accretion
    flow (disk or ADAF/accreting corona) - please
    drop the flaring solar corona analogy!
  • Very broad range of variability time-scales
  • Neutron-star/BH timing similarities (e.g.
    Klein-Wolt van der Klis 2007)
  • Rms-flux relations/non-linearity (e.g. Uttley et
    al. 2005)
  • Optical/X-ray variability in AGN
  • Flickering is standard outcome of MHD
    simulations
  • Spectral-timing properties

8
Building the PSD one disk-annulus at a time
9
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10
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11
Characteristic time-scales scale with black hole
mass
gt108 M?
106 M?
4?107 M?
12
Characteristic time-scales scale inversely with
accretion rate
Markowitz Uttley 2005
For AGN with the same BH mass, PSD break
time-scale appears to depend on luminosity
13
The BH variability fundamental plane
mass-luminosity-timescale
Now with more detailed fitting Does break
time-scale tB scale with bolometric luminosity
of AGN? Try tB? MBHA/LbolB
McHardy et al., Nature, 2006
AGN
BH XRBs
14
Variability vs. Luminosity
Black squares NLS1, Crosses BL Seyferts (Turner
et al. 1999)
?2rms
Log L2-10 keV
Can use excess-variance to estimate mass e.g.
ONeill et al., Gierlinski et al. 2007, Nikolajuk
(this conf.) but should take accretion rate into
account!
15
Power covers a broad bandwidth soft-state like
fake intermediate
16
Problems caveats
GRO J1655-40 X-ray Flux
  • Is Cyg X-1 unusual, is it really soft state?
    Other soft state BHXRBs show much lower rms (few
    per cent or less), c.f. AGN 20-50 rms
  • Are Seyferts really soft state? Maybe normal
    Seyferts hard state, narrow line Seyfert 1s soft?
    (e.g. Gierlinski et al. 2007)

Hardness
Fractional rms
17
Are soft states variable enough?
Cyg X-1 diskPL energy spectra
mean
Cyg X-1 PSDs 6-13 keV 2-6 keV
rms
The variability is produced primarily by the
power-law, not the disk, which is constant
dilutes variability - dont expect in AGN (disk
in optical/UV, but see later)
18
Are soft states variable enough?
Cyg X-1
GRO J1655-40 (Done et al. 2007)
Variability even more heavily diluted by very
large constant disk in other soft-state sources
19
How typical is the Cyg X-1 soft-state PSD?
20
Are Seyferts in soft states?
NGC 5548 (Gaskell et al. 2008)
Yes, most/all have soft SEDs (mdotgt
1) Low/hard states are LINERs/FR Is?
21
Surprise AGN disks are variable!
Not X-ray reprocessing! Simple energetics
argument Long-term optical fractional
variability amplitude gt X-ray, absolute
luminosity variations even larger! But 1 year
few seconds in BHXRBsnot observed. AGN soft
state disks unstable, BHXRB stable?
(NGC 5548, From Uttley et al. 2003)
22
What about reprocessing?
23
Optical still requires some reprocessing (phew!)
MR 2251-178 (Arévalo et al., submitted) good
X-ray/opt correlation but small lags of
short-term variations require small (lt30)
reprocessed variability component
24
Understanding complex spectral variability in AGN
Example Ark 564 shows complex spectral
variability and time lags (Dewangan 2007)
25
Cyg X-1 hard state spectral-timing behaviour
Basic observations Multiple-Lorentzian Power
spectrum (PSD) Harder X-rays ? more power at
high frequencies (short time-scales) Hard lags
soft, lag is frequency dependent Spectral-timing
shifts between Lorentzians
PSD
26
PSD energy dependence in Ark 564
(McHardy et al. 2007)
PSD is band-limited (unlike soft state). Can be
fitted by two Lorentzians, higher frequency
component stronger at higher energies
27
Complex X-ray lags in Ark 564
(McHardy et al. 2007)
In Ark 564, lags seem to show similar stepped
behaviour to Cyg X-1, this time may be very
high state (also multi-Lorentzians)
28
Mapping the emission region
The lag between two bands is the difference
between emissivity-weighted propagation times
(Arévalo Uttley 2006), which is a function of
radius of origin of the signal and hence the
signal time-scale.
29
Conclusions
  • AGN/BHXRB variability is consistent with being
    the same type of process, scaled by mass and mdot
  • Seyfert variability and SEDs are consistent with
    soft states
  • AGN disks are intrinsically unstable on short
    time-scales, unlike in soft state BHXRBs
  • Many properties of AGN variability may already
    be known from BHXRBs, which will help to decode
    the variability
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