3.3.3 Mirror Scatter


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3.3.3 Mirror Scatter

   

The scattering wings of the SXT PSF begin to dominate the narrow core at about 20 arcsec from the center-at a level about 5 or 6 orders of magnitude down from the peak (see Fig. 4 in the Tsuneta, et al. (1991 `Red Book'). The scattering wings may be characterized from over-exposed flares observed in FFI mode such as 6-Sep-92 18:48. Hara (to be published) has derived the following expression which describes the shape of the PSF wing for a flare of K, through the thin filters

per full resolution SXT pixel and per unit intensity in the flare, with r specified in arcsec. The scattering properties of the mirror are wavelength dependent. This introduces a dependence upon input spectrum in correcting for the PSF scattering wings in data analysis. Hara represents this dependence in terms of a ratio of the mean wavelength of the flare and the mean wavelength of the reference ( K) spectrum and gives the following expression for the PSF wing for other source temperatures.

where is the average wavelength recorded by SXT through either the Al.1 or AlMg filters at temperature .

Scattering wing corrections have not yet been derived for the thicker filters and programs for use of the preliminary algorithms derived by Hara have not yet been released for general use because of concerns of their applicability away from sun center.


next up previous contents
Next: 3.3.4 Vignetting Correction Up: 3.3 The MirrorLens Previous: 3.3.2 Point Spread Function


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