|
par1 | minimum angle (degrees) between source photons incident on the slab
and the slab normal
|
par2 | maximum angle (degrees) between source photons incident on the slab
and the slab normal
|
par3 | Angle (degrees) between the observer's line of sight and the slab normal. |
par4 | Iron abundance relative to Solar |
par5 | Iron K-edge energy |
par6 | Fraction of the direct flux seen by the observer |
par7 | Normalization of the reflected continuum |
par8 | redshift |
Suppose the incident photon spectrum is N(E) photons cms
keV
and
that the incident continuum is steady in time, and suppose further that the
reflected continuum from the slab is R(E). When you multiply the incident
spectrum with hrefl, what you actually get is the following:
Thus, the actual physical situation described above corresponds to
par6 = 1.0
par7 = 1.0
You may decide to float par6 and/or par7. In that case, you must decide what the best-fitting values of these parameters mean physically for your case. It may imply time-lags between the direct and reflected components, different source and/or disk geometries to those assumed, or something else.
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Last modified: Friday, 23-Aug-2024 13:20:40 EDT