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Timestamp:
Dec 16, 2019, 3:52:41 PM (7 years ago)
Author:
eugene
Message:

updates with referee responses

File:
1 edited

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  • trunk/doc/release.2015/ps1.datasystem/response.v1.txt

    r41205 r41206  
    1212   the bottom and added a line to show where the distribution and
    1313   publication mechanisms interface to these customers.
     14
     15## Section 3.1
     16
     17This is by no means necessary, but I'm curious to see a table or
     18discussion of what fraction of jobs of various types failed with bad
     19"quality". In other words, how much data could you not get through the
     20pipelines at all, and what was the most sensitive step?
     21
     22** We liked this suggestion and added a subsection 3.12 and a new
     23   table (2) to discuss the failure rates.
     24
     25## Section 3.3
     26
     27Running "Registration" only once for each exposure would seem to
     28prohibit re-running "burntool" after updating the algorithm for that -
     29and I'm guessing you didn't get that fully stabilized until after you
     30had already processed some images and learned from thr experience. How
     31did that work?
     32
     33** We added a couple of sentences to explain that we used a
     34   semi-manual task to re-run just the burntool analysis during
     35   development and if the code ever needs to be changed.
     36
     37## Section 3.5
     38
     39Why a 3rd-order polynomial from chip to focal plane? Wouldn't an
     40affine transform have been sufficient (and more than that degenerate
     41with the focal plane to sky transform)?
     42
     43** We use the higher-order transformation for each chip to capture the
     44   small-scale astrometric signal present in the data.  One could use
     45   an afine transformation for chip-to-focal plane and capture the
     46   same signal in a much higher-order model for focal-plane to sky,
     47   but that was not our development path.  These would be equivalent
     48   solutions.  (Note that degeneracies exist in both cases).   We
     49   avoid the degeneracy of the chip positions in the focal plane
     50   solution by fitting the local gradient to get the initial
     51   distortion solution (and there are certain terms which are held
     52   fixed for the focal plane.)  We then limit the impact of the
     53   degeneracy by fitting the two levels independently and fixing the
     54   focal-plane solution after a few iterations.
     55
     56   We have added some words to explain some of this, but leave the
     57   details to Paper IV.
     58
     59What makes the masks generated in this step "dynamic"? Are they
     60generated wholly from the reference catalog (i.e.  predicting where a
     61ghost will appear based on the position of a bright star)? It seems
     62like the CAMERA step does not utilize any of the pixel data (just the
     63pixel-level masks from CHIP). Is that correct?
     64
     65  ** correct: the dynamic masks are generated from the reference
     66     catalog and do not go back to the original pixels.  We added a
     67     paragraph to clarify.
     68
     69
     70## Section 3.8
     71
     72Is the selection of which warped images go into a stack driven by
     73human operators, or are there automated systems to launch these jobs,
     74too?
     75
     76  ** section 5.2 discusses how both the nightly stacks and
     77     large-scale reprocessing campaign stacks are automatically
     78     defined.  We added some words to refer to this section in 3.8.
     79
     80## Section 3.10
     81
     82How much of the PSF-convolved galaxy models do you re-fit in forced
     83photometry? If you're fitting more than just the amplitude at that
     84stage, and considering each exposure as independent, you're
     85potentially throwing away a lot of S/N (at least in the many-exposure
     86limit), even if you average later. If you're just fitting the
     87amplitude, the structural parameters are still going to be the ones
     88affected by poor PSFs in the stack.
     89
     90  **
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