- Timestamp:
- Dec 6, 2016, 6:32:52 AM (10 years ago)
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trunk/doc/release.2015/ps1.calibration/calibration.tex
r39835 r39836 436 436 * result is a collection of zero points for photometric images 437 437 * discuss stats on the zero points and the airmass terms 438 * does eddie still use per exposure or per star airmass terms? 438 439 \end{verbatim} 439 440 440 441 \subsection{Relphot Analysis} 442 443 The ubercal analysis above results in a table of zero points for all 444 exposures considered to be photometric, along with a set of 445 low-resolution flat-field corrections. It is now necessary to use this 446 information to determine zero points for the remaining exposures and 447 to improve the resolution of the flat-field correction. This analysis 448 is done within the IPP DVO database system. 449 450 The ubercal zero points and the flat-field correction data are loaded 451 into the PV3 DVO database using the program \code{setphot}. This 452 program converts the reported zero point and flat field values to the DVO internal representation 453 in which the zero point of each image is split into three main 454 components: 455 \[ 456 zp_{\rm total} = zp_{\rm nominal} + M_{cal} + K_{rm \lambda}(sec \zeta - 1) 457 \] 458 where $zp_{\rm nominal}$ is a static value for each filter, $K_{rm 459 \lambda}$ is the static slope of the trend with respect to the 460 airmass trend ($\zeta$) for each filter, $M_{cal}$ is the offset 461 needed by each exposure to match the ubercal value, or to bring the 462 given image into agreement with the rest of the exposures, as 463 discussed below. The flat-field information is encoded in a table of 464 flat-field offsets as a function of time, filter, and camera position. 465 466 \note{measurement values are modified $M_{cal}, M_{flat}$, flags} 467 468 When the ubercal values are ingested into the database, 469 441 470 \begin{verbatim} 442 471 * ingest the ubercal zero points (setphot)
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