Changeset 6049
- Timestamp:
- Jan 18, 2006, 5:51:41 PM (21 years ago)
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trunk/doc/design/ippSSDD.tex (modified) (3 diffs)
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trunk/doc/design/ippSSDD.tex
r6041 r6049 1 %%% $Id: ippSSDD.tex,v 1. 3 2006-01-19 01:05:28eugene Exp $1 %%% $Id: ippSSDD.tex,v 1.4 2006-01-19 03:51:41 eugene Exp $ 2 2 \documentclass[panstarrs]{panstarrs} 3 3 … … 2750 2750 2751 2751 \subsection{psastro} 2752 Like psphot, psastro may be run as a stand-alone program or as a 2753 library. This 2754 2752 2753 This section discusses the design of psastro in general terms. For 2754 more specific usage information, see the document on psastro. Like 2755 psphot, psastro may be run as a stand-alone program or as a library. 2756 This routine performs astrometric calibration of a collection of 2757 sources from an image or a set of images. As a stand-alone program, 2758 the input to psastro is an image file or set of images files 2759 representing data from single FPA. Like ppImage, the input image or 2760 images may be specified as a single file, a glob, or Nebulous storage 2761 object IDs. The heart of the psastro routine is wrapped with a loop 2762 similar to the one used for ppImage. The primary difference between 2763 the two is that psastro expect a collection of files representing 2764 sources detected in an image, rather than the pixels from an image. 2765 Several standard source file formats, discussed in the psphot 2766 documentation may be read. The sources which are loaded are added to 2767 the FPA heirarchy at the appropriate level, as part of the metadata 2768 collection associated with a given level. As a library function, 2769 psastro is passed an assembled FPA structure with the sources already 2770 placed in the appropriate locations in the metadata containers. 2771 2772 Psastro has three major modes, which are used in each of Phases 1, 2, 2773 and 3. 2774 2775 In the conceptualy most straightforeward mode, each readout contained 2776 in the incoming FPA structure is treated independently. The metadata 2777 describing the approximate astrometry of the readout are used to guess 2778 the coordinates of the sources and to select likely reference sources 2779 from the selected reference catalog. The observed sources are matched 2780 to the reference sources, using either a two-point grid search or 2781 optionally a \tbd{triangle match}. Once an approximate match is 2782 found, a linear fit between detector coordinates an projected 2783 celestial coordinates is attempted. The projected coordinate system 2784 may optionally make use of the default telescope distortion model, if 2785 it is known. The radius of the match between observed and reference 2786 sources is reduced to improve the statistics of the match. This 2787 anaysis mode is used in the Phase 2 processing. 2788 2789 The second type of psastro analysis is used by Phase 3 to improve the 2790 solution determined in Phase 3. In this analysis, psastro expects 2791 detections from a complete mosaic FPA of chips. A complete mosaic 2792 solution is performed in which a single distortion model is used for 2793 the telescope optics and additional linear or higher order terms. 2794 This analysis breaks the degeneracy of the chip position / telescope 2795 distortion by fitting the local gradient of the distortion on chips to 2796 model the telescope distortion. The result of this analysis is a 2797 complete mosaic astrometry model, consisting of (at the moment) 3rd 2798 order polynomials for the telescope distortion and up to 3rd order 2799 polynomials for each of the individual chips. 2800 2801 In the third mode, a collection of detections from across a full 2802 mosaic are used, in conjunction with a model for the chip positions 2803 and the telescope / optical distortion, to determine a single 2804 low-order model for the complete FPA. In this model, only the 2805 boresite coordinates, rotation, and X and Y plate scales are allowed 2806 to vary. This analysis is used for the Phase 1 analysis, in 2807 conjunction with an implementation of psphot. 2808 2809 For any complete mosaic, there are three complementary representations 2810 of the astrometric solution which are used within the IPP. The most 2811 basic description of the astrometry is the collection of header 2812 keywords which define the boresite center coordinates (RA, DEC), the 2813 rotation and platescales 2755 2814 2756 2815 \section{Interfaces} … … 3758 3817 ------ 3759 3818 3760 * top-level routines3819 * poisub / stack 3761 3820 * re-org the Phase 4 stuff to discuss Magic 3762 3821 * astrometry calibration data formats
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