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Changeset 6049


Ignore:
Timestamp:
Jan 18, 2006, 5:51:41 PM (21 years ago)
Author:
eugene
Message:

updates to psastro

File:
1 edited

Legend:

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Added
Removed
  • trunk/doc/design/ippSSDD.tex

    r6041 r6049  
    1 %%% $Id: ippSSDD.tex,v 1.3 2006-01-19 01:05:28 eugene Exp $
     1%%% $Id: ippSSDD.tex,v 1.4 2006-01-19 03:51:41 eugene Exp $
    22\documentclass[panstarrs]{panstarrs}
    33
     
    27502750
    27512751\subsection{psastro}
    2752 Like psphot, psastro may be run as a stand-alone program or as a
    2753 library.  This
    2754 
     2752
     2753This section discusses the design of psastro in general terms.  For
     2754more specific usage information, see the document on psastro.  Like
     2755psphot, psastro may be run as a stand-alone program or as a library.
     2756This routine performs astrometric calibration of a collection of
     2757sources from an image or a set of images.  As a stand-alone program,
     2758the input to psastro is an image file or set of images files
     2759representing data from single FPA.  Like ppImage, the input image or
     2760images may be specified as a single file, a glob, or Nebulous storage
     2761object IDs.  The heart of the psastro routine is wrapped with a loop
     2762similar to the one used for ppImage.  The primary difference between
     2763the two is that psastro expect a collection of files representing
     2764sources detected in an image, rather than the pixels from an image.
     2765Several standard source file formats, discussed in the psphot
     2766documentation may be read.  The sources which are loaded are added to
     2767the FPA heirarchy at the appropriate level, as part of the metadata
     2768collection associated with a given level.  As a library function,
     2769psastro is passed an assembled FPA structure with the sources already
     2770placed in the appropriate locations in the metadata containers.
     2771
     2772Psastro has three major modes, which are used in each of Phases 1, 2,
     2773and 3.
     2774
     2775In the conceptualy most straightforeward mode, each readout contained
     2776in the incoming FPA structure is treated independently.  The metadata
     2777describing the approximate astrometry of the readout are used to guess
     2778the coordinates of the sources and to select likely reference sources
     2779from the selected reference catalog.  The observed sources are matched
     2780to the reference sources, using either a two-point grid search or
     2781optionally a \tbd{triangle match}.  Once an approximate match is
     2782found, a linear fit between detector coordinates an projected
     2783celestial coordinates is attempted.  The projected coordinate system
     2784may optionally make use of the default telescope distortion model, if
     2785it is known.  The radius of the match between observed and reference
     2786sources is reduced to improve the statistics of the match.  This
     2787anaysis mode is used in the Phase 2 processing.
     2788
     2789The second type of psastro analysis is used by Phase 3 to improve the
     2790solution determined in Phase 3.  In this analysis, psastro expects
     2791detections from a complete mosaic FPA of chips.  A complete mosaic
     2792solution is performed in which a single distortion model is used for
     2793the telescope optics and additional linear or higher order terms.
     2794This analysis breaks the degeneracy of the chip position / telescope
     2795distortion by fitting the local gradient of the distortion on chips to
     2796model the telescope distortion.  The result of this analysis is a
     2797complete mosaic astrometry model, consisting of (at the moment) 3rd
     2798order polynomials for the telescope distortion and up to 3rd order
     2799polynomials for each of the individual chips.
     2800
     2801In the third mode, a collection of detections from across a full
     2802mosaic are used, in conjunction with a model for the chip positions
     2803and the telescope / optical distortion, to determine a single
     2804low-order model for the complete FPA.  In this model, only the
     2805boresite coordinates, rotation, and X and Y plate scales are allowed
     2806to vary.  This analysis is used for the Phase 1 analysis, in
     2807conjunction with an implementation of psphot.
     2808
     2809For any complete mosaic, there are three complementary representations
     2810of the astrometric solution which are used within the IPP.  The most
     2811basic description of the astrometry is the collection of header
     2812keywords which define the boresite center coordinates (RA, DEC), the
     2813rotation and platescales
    27552814
    27562815\section{Interfaces}
     
    37583817------
    37593818
    3760 * top-level routines
     3819* poisub / stack
    37613820* re-org the Phase 4 stuff to discuss Magic
    37623821* astrometry calibration data formats
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