periodic oscillations in the Lense- Thirring precession model Piotr - - PowerPoint PPT Presentation

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periodic oscillations in the Lense- Thirring precession model Piotr - - PowerPoint PPT Presentation

Timing properties of the X-ray quasi- periodic oscillations in the Lense- Thirring precession model Piotr ycki Nicolaus Copernicus Astronomical Center, Warsaw, Poland From the Dolomities to the event horizon: sledging down the black hole


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Timing properties of the X-ray quasi- periodic oscillations in the Lense- Thirring precession model

Piotr Życki

Nicolaus Copernicus Astronomical Center, Warsaw, Poland

„From the Dolomities to the event horizon: sledging down the black hole potential well”, 3rd edition, 16-07-2015

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SLIDE 2

X-ray QPO

Low-f QPO

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SLIDE 3

Observed energy spectra of QPO

Disk emission is not present in the QPO spectra. When time averaged spectra are soft, the QPO spectra are harder than the time averaged spectra.

Sobolewska & Życki 2006

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Lense-Thirring precession model for low-f QPO

Formulated by Stella & Vietri (1998) Recent hydrodynamical simulations suggest that the hot flow behaves (precesses) like a solid body. Inner radius of the flow is determined by properties of the bending waves. It is approximately independent of the spin of the black hole. As a result the maximum precession frequency does not depend on the spin. (C. Done, A. Ingram, C. Fragile)

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The model

+

Connects the „standard” geometry of the transition between the hard-soft state with timing properties

  • Can the torus really precess like a solid body?
  • Unclear trigger of the QPO
  • Does it require a misaligned spin and orbital angular momentum?
  • Requires rotating black hole but does not give a possibility of determining a
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SLIDE 6

Geometry

Two geometrical scenarios:

  • 1. precession axis perp. to the
  • uter disk
  • 2. Precession axis inclined to the
  • uter disk (based on Bardeen-

Peterson effect)

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SLIDE 7

Geometry

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SLIDE 8
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SLIDE 9

coplanar config.

  • prec. axis perp. to the outer disk
  • prec. axis inclined to the outer disk

geometrically thick torus; to be compared with the blue curve

Concept of compactness used here!

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Precesion scenario 2 (precession axis inclined to the outer disk axis) precession axis towards the observer

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SLIDE 11

Precesion scenario 2 (precession axis inclined to the outer disk axis) precession axis away from the observer

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QPO phase lags - observations

GRS 1915+105; RXTE observations Phase difference between 2-5 keV and 13-18 keV QPO; Qu et al., 2010

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Simulations

Half opening angle of the torus – 15 deg Angle between system axis and precession axis – 15 degs Inclination angle: 60 degs

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SLIDE 14

Simulations

Precession axis towards the observer and away from the observer

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SLIDE 15

Lightcurves

Precession axis towards the observer and away from the observer

1 keV and 30 keV light curves

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SLIDE 16

Spectral variability

Precession axis towards the observer and away from the observer

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SLIDE 17

Spectral variability

Precession axis towards the observer and away from the observer

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SLIDE 18

Spectral variability

Precession axis towards the observer and away from the observer

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SLIDE 19

Phase lags

Precession axis towards the observer and away from the observer

3 keV vs 30 keV; signal at fQPO and its first harmonic

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SLIDE 20

Phase lags

Precession axis towards the observer and away from the observer

1 keV vs 30 keV; signal at fQPO and its first harmonic

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SLIDE 21

Phase lags

Precession axis towards the observer and away from the observer

1 keV vs 20 keV; signal at fQPO and its first harmonic

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SLIDE 22

Phase lags

Precession axis at 90 degs angle wrt the observer

1 keV vs 20 keV; signal at fQPO and its first harmonic

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SLIDE 23

Spectral slope vs QPO frequency Gamma Gamma

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SLIDE 24

In summary…

The Monte Carlo approach assumes a simple uniform (density, temperature) configuration. It may be that the radial structure is crucial for explaining the details.