Chandra X-Ray Spectroscopy of the Focused Wind in the Cygnus X-1 System III. Dipping in the Low/Hard State

We present an analysis of three Chandra High Energy Transmission Gratings observations of the black hole binary CygX-1/HDE 226868 at different orbital phases. The stellar wind that is powering the accretion in this system is characterized by temperature and density in homogeneities including structu...

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Published inAstronomy and astrophysics (Berlin) Vol. 626; p. A64
Main Authors Hirsch, Maria, Hell, Natalie, Grinberg, Victoria, Ballhausen, Ralf, Nowak, Michael A., Pottschmidt, Katja, Schulz, Norbert S., Dauser, Thomas, Hanke, Manfred, Kallman, Timothy R., Brown, Gregory V., Wilms, Jörn
Format Journal Article
LanguageEnglish
Published Goddard Space Flight Center EDP Sciences 13.06.2019
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Summary:We present an analysis of three Chandra High Energy Transmission Gratings observations of the black hole binary CygX-1/HDE 226868 at different orbital phases. The stellar wind that is powering the accretion in this system is characterized by temperature and density in homogeneities including structures, or “clumps”, of colder, more dense material embedded in the photoionized gas. As these clumps pass our line of sight, absorption dips appear in the light curve. We characterize the properties of the clumps through spectral changes during various dip stages. Comparing the silicon and sulfur absorption line regions (1.6–2.7 keV Ξ 7.7–4.6 Å) in four levels of varying column depth reveals the presence of lower ionization stages, i.e., colder or denser material, in the deeper dip phases. The Doppler velocities of the lines are roughly consistent within each observation, varying with the respective orbital phase. This is consistent with the picture of a structure that consists of differently ionized material, in which shells of material facing the black hole shield the inner and back shells from the ionizing radiation. The variation of the Doppler velocities compared to a toy model of the stellar wind, however, does not allow us to pin down an exact location of the clump region in the system. This result, as well as the asymmetric shape of the observed lines, point at a picture of a complex wind structure.
Bibliography:GSFC-E-DAA-TN70477
GSFC
Goddard Space Flight Center
AC52-07NA27344
USDOE National Nuclear Security Administration (NNSA)
LLNL-JRNL-761005
ISSN:0004-6361
1432-0746
DOI:10.1051/0004-6361/201935074