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Changes between Version 9 and Version 10 of IPP_Progress_Report_20100816


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Timestamp:
Aug 23, 2010, 9:44:00 PM (16 years ago)
Author:
watersc1
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  • IPP_Progress_Report_20100816

    v9 v10  
    77 * IPP Code Updates
    88
    9 We are in the process of switching the operational IPP code to a new
    10 software release.   The new tag is ipp-20100823.
     9We are in the process of switching the operational IPP code to a new software release.   The new tag is ipp-20100823.
    1110
    12 This update includes a number of features and fixes to issues which
    13 have been in progress for some time.  Here is a summary list of the
    14 main salient points:
     11This update includes a number of features and fixes to issues which have been in progress for some time.  Here is a summary list of the main salient points:
    1512
    16 1) a new "staticsky" distribution component : this is the method by
    17 which we will be distributing the results from the full photometry
    18 analysis of the static sky images.
     13 1. a new "staticsky" distribution component : this is the method by which we will be distributing the results from the full photometry analysis of the static sky images.
     14 1. Full extended source analysis!  psphot is now able to produce acceptable measurements of all of the extended source parameters on our list.
     15   a. for all sources, we are now including Kron parameters (Kron flux and error in an aperture 2.5 times the first radial moment (R1), plus the flux within 1 times R and 4 times R1, as well as the value of R1.
     16   a. in the static sky analysis, for all sources we now report the radial aperture measurements (this was available in the earlier MD04 example set).
     17   a. Petrosian and elliptical surface brightness profiles for a subset of extended sources (S/N above some cut off to be defined, probably based on galactic latitude)
     18   a. PSF-convolved model fits for a subset of extended sources for Exponential, DeVaucouleur, and Sersic models.
     19 1. fixed the forced photometry non-negative flux bug
     20 1.  added some other new stats:
     21  a. for PSF fits, we now have "psfWeightNotPoor" and "psfWeightNotBad" : the first gives the fraction of psf-weighted unmasked pixels considering any mask bits (except the internal 'mark' bit), while the former considers only 'bad' mask bits -- these are written to QF_PSF and QF_PSF_PERFECT in the CMF / SMF files.  This may help to exclude false sources in subtracted burn regions (SUSPECT mask bit) or sources too close to a mask edge (CONV.POOR mask bit).
     22  a. raw aperture magnitudes (in addition to the curve-of-growth corrected version) for PSF measurements.
     23  a. in diff images, we now have several additional statistics related to the proximity of a diff detection to an input image source: DIFF_R_P, SN_P : distance and S/N of nearest bright source in the plus image, DIFF_R_M,SN_M : same for the minus image.
     24  a. for PSF sources, we have added several higher order moments: MOMENTS_M3C,S (third moments cos & sin theta), and same for 4th moments.
     25 1. somewhat better CR / EXT tests, including use of Kron magnitude as test for source size (CR vs EXT) instead of PSF-based aperture. (though these are not yet reported as a probability).
     26 1. save the radial profile aperture sizes in the headers
     27 1. swap read order in dvomerge to loop over the available input tables and merge them with existing output tables
     28 1. allow dvomerge to operate on only a region of the sky
     29 1. update to dvomerge to allow different average photcodes in the inputs and the output database.
     30 1. some important issues in ppSub that were resulting is somewhat poor matches when the IQ difference between the two images was large:
     31  a. ensure masked pixels are NANed in output diff image
     32  b. define separate penalties for each image (based on their fwhm values)
     33  c. define separate apertures for each image for flux normalization
     34  d. choose aperture based on curve-of-growth (was based on fixed fraction of full aperture flux, and thus noisy)
     35  e. some fine tuning of the penalty factor (this still seems arbitrary, and results are somewhat sensitive to the right value)
    1936
    20 2) Full extended source analysis!  psphot is now able to produce
    21 acceptable measurements of all of the extended source parameters on
    22 our list.
    23   a) for all sources, we are now including Kron parameters (Kron flux
    24 and error in an aperture 2.5 times the first radial moment (R1), plus
    25 the flux within 1 times R and 4 times R1, as well as the value of R1.
    26   b) in the static sky analysis, for all sources we now report the
    27 radial aperture measurements (this was available in the earlier MD04
    28 example set).
    29   c) Petrosian and elliptical surface brightness profiles for a subset
    30 of extended sources (S/N above some cut off to be defined, probably
    31 based on galactic latitude)
    32   d) PSF-convolved model fits for a subset of extended sources for
    33 Exponential, DeVaucouleur, and Sersic models.
     37Note that there are three new output formats that are needed to make all of these features part of the standard products:
    3438
    35 3) fixed the forced photometry non-negative flux bug
     39  * for chip-image processing: PS1_V3
     40  * for staticsky processing: PS1_SV1
     41  * for diff processing: PS1_DV2
    3642
    37 4) added some other new stats:
    38  a) for PSF fits, we now have "psfWeightNotPoor" and "psfWeightNotBad"
    39 : the first gives the fraction of psf-weighted unmasked pixels
    40 considering any mask bits (except the internal 'mark' bit), while the
    41 former considers only 'bad' mask bits -- these are written to QF_PSF
    42 and QF_PSF_PERFECT in the CMF / SMF files.  This may help to exclude
    43 false sources in subtracted burn regions (SUSPECT mask bit) or sources
    44 too close to a mask edge (CONV.POOR mask bit).
    45  b) raw aperture magnitudes (in addition to the curve-of-growth
    46 corrected version) for PSF measurements.
    47  c) in diff images, we now have several additional statistics related
    48 to the proximity of a diff detection to an input image source:
    49 DIFF_R_P, SN_P : distance and S/N of nearest bright source in the plus
    50 image, DIFF_R_M,SN_M : same for the minus image.
    51  d) for PSF sources, we have added several higher order moments:
    52 MOMENTS_M3C,S (third moments cos & sin theta), and same for 4th
    53 moments.
    54 
    55 5) somewhat better CR / EXT tests, including use of Kron magnitude as
    56 test for source size (CR vs EXT) instead of PSF-based aperture.
    57 (though these are not yet reported as a probability).
    58 
    59 6) save the radial profile aperture sizes in the headers
    60 
    61 7) swap read order in dvomerge to loop over the available input tables
    62 and merge them with existing output tables
    63 
    64 8) allow dvomerge to operate on only a region of the sky
    65 
    66 9) update to dvomerge to allow different average photcodes in the
    67 inputs and the output database.
    68 
    69 10) some important issues in ppSub that were resulting is somewhat
    70 poor matches when the IQ difference between the two images was large:
    71   a) ensure masked pixels are NANed in output diff image
    72   b) define separate penalties for each image (based on their fwhm values)
    73   c) define separate apertures for each image for flux normalization
    74   d) choose aperture based on curve-of-growth (was based on fixed
    75 fraction of full aperture flux, and thus noisy)
    76   e) some fine tuning of the penalty factor (this still seems
    77 arbitrary, and results are somewhat sensitive to the right value)
    78 
    79 Note that there are three new output formats that are needed to make
    80 all of these features part of the standard products:
    81 
    82 for chip-image processing: PS1_V3
    83 for staticsky processing: PS1_SV1
    84 for diff processing: PS1_DV2
    85 
    86 I would like to run with the old versions for a few days to check that
    87 there are no problems, and to give people a bit of a warning.  we need
    88 to be particularly careful that the MOPS folks do not get torqued by
    89 the diff output changes.
     43I would like to run with the old versions for a few days to check that there are no problems, and to give people a bit of a warning.  we need to be particularly careful that the MOPS folks do not get torqued by the diff output changes.
    9044
    9145 * Data Samples:
    9246
    93 I am placing two example data set (simulated images) that illustrate
    94 the extended source analysis and the difference image analysis
     47I am placing two example data set (simulated images) that illustrate the extended source analysis and the difference image analysis
    9548
    96 rsync://pikake.ifa.hawaii.edu/psphot.extended.simtest  :  this
    97 directory contains a set of images with fake galaxies (a range of
    98 sersic parameters, convolved with a Gaussian seeing kernel) and psphot
    99 fits to those same images. (inputs are image.fake.NN.fits, outputs are
    100 image.fake.pcm.x2.*)
     49rsync://pikake.ifa.hawaii.edu/psphot.extended.simtest  :  this directory contains a set of images with fake galaxies (a range of sersic parameters, convolved with a Gaussian seeing kernel) and psphot fits to those same images. (inputs are image.fake.NN.fits, outputs are image.fake.pcm.x2.*)
    10150
    102 rsync://pikake.ifa.hawaii.edu/ppsub.samples.simtest : this directory
    103 contains an extensive set of images with different PSFs all
    104 differenced against each other with the newly-updated psphot.  There
    105 are two classes of images: those with .fg in the name have Gaussian
    106 PSFs (range of sizes, axis ratios, and angles), while those with .fp
    107 use the PS1_V1 model (a wingier PSF meant to mimic PS1).
     51rsync://pikake.ifa.hawaii.edu/ppsub.samples.simtest : this directory contains an extensive set of images with different PSFs all differenced against each other with the newly-updated psphot.  There are two classes of images: those with .fg in the name have Gaussian PSFs (range of sizes, axis ratios, and angles), while those with .fp use the PS1_V1 model (a wingier PSF meant to mimic PS1).
    10852
    109 rsync://pikake.ifa.hawaii.edu/ppsub.samples.simtest.oldcode : the same
    110 set of input image pairs diff'ed using the previous version of ppSub.
     53rsync://pikake.ifa.hawaii.edu/ppsub.samples.simtest.oldcode : the same set of input image pairs diff'ed using the previous version of ppSub.
    11154
    112 We will attempt to run MD04 with the static sky analysis tomorrow for
    113 people to play with.
     55We will attempt to run MD04 with the static sky analysis tomorrow for people to play with.
    11456
    11557 * MD04 Photometry
    11658
    117 I have done some investigation of the high systematic photometry
    118 errors in the MD04 stacks as reported by Nigel M.  Some of the plots
    119 related to this study can be found here:
    120 https://svn.pan-starrs.ifa.hawaii.edu/trac/ipp/wiki/MD04_Stack_Photometry_20100819
     59I have done some investigation of the high systematic photometry errors in the MD04 stacks as reported by Nigel M.  Some of the plots related to this study can be found here: https://svn.pan-starrs.ifa.hawaii.edu/trac/ipp/wiki/MD04_Stack_Photometry_20100819
    12160
    122 I first checked that the PSFs of the stars had a consistent shape by
    123 overlaying the normalized PSFs, and confirmed that they are indeed
    124 consistent.
     61I first checked that the PSFs of the stars had a consistent shape by overlaying the normalized PSFs, and confirmed that they are indeed consistent.
    12562
    126 I next examined the impact of different PSF models, to check the
    127 impact of the choice of model shape (ie, is the photometry more
    128 consistent the more accurately the PSF is modelled).  This did not
    129 have a huge impact on the photometry (the bright-end sag was still
    130 apparent), but the bright end photometric scatter is less in my
    131 analysis (PSF - AP) than in Nigel's (PS1 - SDSS).
     63I next examined the impact of different PSF models, to check the impact of the choice of model shape (ie, is the photometry more consistent the more accurately the PSF is modelled).  This did not have a huge impact on the photometry (the bright-end sag was still apparent), but the bright end photometric scatter is less in my analysis (PSF - AP) than in Nigel's (PS1 - SDSS).
    13264
    133 I then ran the same tests using non-poisson weights.  This addresses
    134 the bright end sag, and perhaps tightens the photometry a bit.
     65I then ran the same tests using non-poisson weights.  This addresses the bright end sag, and perhaps tightens the photometry a bit.
    13566
    13667=== Serge Chastel ===