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Super-orbital variability

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Presentation on theme: "Super-orbital variability"— Presentation transcript:

1 Super-orbital variability
in Cygnus X-1 ISSI, Bern, Switzerland March 3-7, 2008 J. Poutanen, A. Zdziarski, A. Ibragimov MNRAS, submitted

2 Accretion via Roche lobe and focused wind
Stream trajectory and disk formation for the case of equal masses. Coriolis force shifts the stream from the line connecting the stars.

3 Superorbital variability
Radio X-rays

4 Dips distribution

5 Orbital profiles as a function of superorbital phase

6 (c) A view from the top bulge  b disc supergiant  =0.5  =0

7 i    =0.5  =0 observer (a) A view along the orbital plane,  =0
bulge supergiant black hole disc  =0.5  =0

8  =0.5  =0 observer (b) A view along the orbital plane,  =0.5 disc
supergiant black hole bulge  =0.5  =0

9 Model Wind Parameters: inclination i=40 deg Precession angle  Bulge
Optical depths: bulge b,0 , wind w,0 Bulge azimuth b

10 Model Emissivity profile of the accretion disk For the jet/ outflow

11 Orbital profiles as a function of superorbital phase

12 Results

13 PDS of the model flux

14 Conclusions Discovery of orbital modulation strength on superorbital phase of Cyg X-1 Effect can be explained by the bulge displaced from the line connecting the stars by 25 deg. Distribution of dips is consistent with the model Beat-frequencies should be observed, with the stronger lower one.

15 Log-normal flux distribution


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