2004
DOI: 10.1086/422093
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A Steady, Radiative‐Shock Method for Computing X‐Ray Emission from Colliding Stellar Winds in Close, Massive‐Star Binaries

Abstract: We present a practical, efficient, semianalytic formalism for computing steady state X-ray emission from radiative shocks between colliding stellar winds in relatively close (orbital period up to order tens of days) massive-star, binary systems. Our simplified approach idealizes the individual wind flows as smooth and steady, ignoring the intrinsic instabilities and associated structure thought to occur in such flows. By also suppressing thin-shell instabilities for wind-collision radiative shocks, our steady … Show more

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Cited by 87 publications
(117 citation statements)
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“…4. For the O+OB binaries with spectral information and defined period, log f X / f BOL ratio from Table 6. inhibition, where the radiation of one component decelerates the wind originating in its companion (Gayley et al 1997;Antokhin et al 2004). It should have more impact on short-period systems than on long-period binaries.…”
Section: Summary and Discussion: The X-ray Properties Of Ob Starsmentioning
confidence: 99%
“…4. For the O+OB binaries with spectral information and defined period, log f X / f BOL ratio from Table 6. inhibition, where the radiation of one component decelerates the wind originating in its companion (Gayley et al 1997;Antokhin et al 2004). It should have more impact on short-period systems than on long-period binaries.…”
Section: Summary and Discussion: The X-ray Properties Of Ob Starsmentioning
confidence: 99%
“…Following the approach of Antokhin et al (2004), we assume that the flow along the WCR is laminar, neglecting any possible effect owing to mixing of the fluid streamlines. We also suppose that the velocity of the fluid at a given position of the WCR is equal to the projected tangential component of the stellar wind velocity.…”
Section: Hydrodynamicsmentioning
confidence: 99%
“…If the wind material is continuously heated and cooled, a time-averaged description of the wind should contain a continuous distribution of plasma temperatures (e.g. Antokhin et al 2004). We therefore mimic such a distribution by using 4 plasma temperature components (T 1+T 2+T 3+T 4) with fixed kT of 0.2, 0.6, 1.0, and 4.0 keV, corresponding loosely to the peak emissivity of dominant spectral features likely to be present in the ACIS-S bandpass (H-like and He-like atoms of Ne, Mg, Si, S, and Fe).…”
Section: Spectral Analysismentioning
confidence: 99%