Changeset 41206 for trunk/doc/release.2015/ps1.datasystem/response.v1.txt
- Timestamp:
- Dec 16, 2019, 3:52:41 PM (7 years ago)
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trunk/doc/release.2015/ps1.datasystem/response.v1.txt
r41205 r41206 12 12 the bottom and added a line to show where the distribution and 13 13 publication mechanisms interface to these customers. 14 15 ## Section 3.1 16 17 This is by no means necessary, but I'm curious to see a table or 18 discussion 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 20 pipelines 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 27 Running "Registration" only once for each exposure would seem to 28 prohibit re-running "burntool" after updating the algorithm for that - 29 and I'm guessing you didn't get that fully stabilized until after you 30 had already processed some images and learned from thr experience. How 31 did 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 39 Why a 3rd-order polynomial from chip to focal plane? Wouldn't an 40 affine transform have been sufficient (and more than that degenerate 41 with 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 59 What makes the masks generated in this step "dynamic"? Are they 60 generated wholly from the reference catalog (i.e. predicting where a 61 ghost will appear based on the position of a bright star)? It seems 62 like the CAMERA step does not utilize any of the pixel data (just the 63 pixel-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 72 Is the selection of which warped images go into a stack driven by 73 human operators, or are there automated systems to launch these jobs, 74 too? 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 82 How much of the PSF-convolved galaxy models do you re-fit in forced 83 photometry? If you're fitting more than just the amplitude at that 84 stage, and considering each exposure as independent, you're 85 potentially throwing away a lot of S/N (at least in the many-exposure 86 limit), even if you average later. If you're just fitting the 87 amplitude, the structural parameters are still going to be the ones 88 affected by poor PSFs in the stack. 89 90 **
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