in collaboration with julien malzac renaud belmont bo ena
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In collaboration with: Julien Malzac, Renaud Belmont, Bo ena Czerny, - PowerPoint PPT Presentation

In collaboration with: Julien Malzac, Renaud Belmont, Bo ena Czerny, Pierre-Olivier Petrucci Agata R a ska 27.01.2015, University of Bamberg NuSTAR observation of Solar corona ~1 keV In collaboration with: Julien Malzac, Renaud


  1. In collaboration with: Julien Malzac, Renaud Belmont, Bo ż ena Czerny, Pierre-Olivier Petrucci Agata Ró ż a ń ska 27.01.2015, University of Bamberg

  2. NuSTAR observation of Solar corona ~1 keV In collaboration with: Julien Malzac, Renaud Belmont, Bo ż ena Czerny, Pierre-Olivier Petrucci Agata Ró ż a ń ska 16.07.2015, Sesto-Sexten

  3. ~10 6-7 K, optically thick corona Black hole cold accretion disk In collaboration with: Julien Malzac, Renaud Belmont, Bo ż ena Czerny, Pierre-Olivier Petrucci Agata Ró ż a ń ska 16.07.2015, Sesto-Sexten

  4. International conference organised by Andrzej Zdziarski in 1996 in Koninki, Poland

  5. International conference organised by Andrzej Zdziarski in 1996 in Koninki, Poland

  6. International conference organised by Andrzej Zdziarski in 1996 in Koninki, Poland

  7. Hot corona 10 9 K, cooled by Comptonization was optically thin, as shown by Haardt & Maraschi in 1993

  8. Continuum energy distribution in radio-quiet AGN:

  9. Continuum energy distribution in radio-quiet AGN:

  10. Janiuk et al. 2001 PG1211+143

  11. Janiuk et al. 2001 PG1211+143 large optical depth

  12. Gierli ń ski & Done 2004

  13. Gierli ń ski & Done 2004

  14. Jin, Ward, Done, Gelbord 2012

  15. Jin, Ward, Done, Gelbord 2012

  16. Jin, Ward, Done, Gelbord 2012

  17. Done, Davis, Blaes, Ward 2012

  18. Done, Davis, Blaes, Ward 2012

  19. Petrucci et al. 2013 , Mrk 509

  20. Petrucci et al. 2013, Mrk 509

  21. Petrucci et al. 2013 , Mrk 509

  22. Warm , dissipated corona, optically thick , cooled purely by Compton scattering, grey ~10 6-7 K, optically thick corona cold accretion disk

  23. Warm , dissipated corona, optically thick , cooled purely by Compton scattering, grey ~10 6-7 K, optically thick corona cold accretion disk purely scattered, dissipated corona 1) S=J+Q

  24. Warm , dissipated corona, optically thick , cooled purely by Compton scattering, grey ~10 6-7 K, optically thick corona cold accretion disk purely scattered, dissipated corona 1) S=J+Q 2)

  25. Corona is cooled by Compton scattering 1)

  26. Corona is cooled by Compton scattering 1) 2)

  27. Corona is cooled by Compton scattering

  28. Corona in hydrostatic equilibrium with cold disc 1)

  29. Corona in hydrostatic equilibrium with cold disc 1) 2) 3)

  30. Corona in hydrostatic equilibrium with cold disc 1) 2) 3) 4)

  31. Corona in hydrostatic equilibrium with cold disc 1) 2)

  32. Corona in hydrostatic equilibrium with cold disc 1) 2) 3) 4)

  33. Corona in hydrostatic equilibrium with cold disc 1) 2) 3) 4)

  34. Corona is Compton dominated 1)

  35. Corona is Compton dominated 1) 2) at the base of the corona 3)

  36. The optical depth of the base of dissipated corona

  37. Conclusions

  38. Conclusions 1) Dissipative corona purely cooled by Compton scattering heats up to ~ 1 keV on the base of radiative transfer. 2) Maximum optical depth of such corona: optical depth in hydr. eq. ~ 5 3) The optical depth of soft corona is increasing when gas pressure is reduced for instance when magnetic pressure is increasing. 4) For optical depth ~ 20 , but maybe there is another mechanism to low down the gas pressure ????

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