1997
DOI: 10.1023/a:1004208323283
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Cited by 23 publications
(2 citation statements)
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“…Instead the absorption can be described as a continuous range of columns through which the source is seen, as expected for the pre-shock material. While the ionization structure of the column is outside of the scope of this paper (see Rainger et al 1997), the data are clearly consistent with a power law column-covering fraction distribution of neutral material, so we use this model in all the following fits. The continuum is also significantly better described by a multi-temperature α = 1 cooling shock model than by a single temperature plasma, so we use this to describe the plasma emission in all the following fits.…”
Section: Asca Datamentioning
confidence: 93%
“…Instead the absorption can be described as a continuous range of columns through which the source is seen, as expected for the pre-shock material. While the ionization structure of the column is outside of the scope of this paper (see Rainger et al 1997), the data are clearly consistent with a power law column-covering fraction distribution of neutral material, so we use this model in all the following fits. The continuum is also significantly better described by a multi-temperature α = 1 cooling shock model than by a single temperature plasma, so we use this to describe the plasma emission in all the following fits.…”
Section: Asca Datamentioning
confidence: 93%
“…Modelling including all these are being developed [9], but here we use a phenomenological description of this complex absorption in terms of a continuous (power law) distribution of neutral absorping column and covering fraction (C f ∝ N β H , see also [10]).…”
Section: Spectral Complexitymentioning
confidence: 99%