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trunk/doc/release.2015/ps1.calibration/calibration.tex
r41181 r41188 1367 1367 fluxes. 1368 1368 1369 The first challenge is to select which measurements to use in 1370 the calculation of the average photometry. For the $3\pi$ Survey 1371 data, asingle object may have anywhere from zero to roughly twenty1369 The first challenge is to select which measurements to use in the 1370 calculation of the average photometry. For the $3\pi$ Survey data, a 1371 single object may have anywhere from zero to roughly twenty 1372 1372 measurements in a given filter. Not all measurements are of equal 1373 1373 value, but we need a process which assigns an average photometry value … … 1377 1377 measurements available in each filter for each object. Once the set 1378 1378 of measurements to be used in the analysis is determined, we use the 1379 Iteratively Reweighted Least Squares (IRLS) technique to determine the 1380 average photometry given the possible presence of non-Gaussian 1381 outliers even within the best subset of measurements. 1382 1383 \note{include a reference to IRLS and describe concept more} 1384 \code{http://users.stat.umn.edu/~sandy/courses/8053/handouts/robust.pdf} 1385 \code{https://arxiv.org/pdf/0807.0575.pdf} 1386 \code{https://www.redalyc.org/pdf/3939/393933924009.pdf} 1387 \code{Street, J. O., Carrol, R. J., \& Ruppert D. 1988, Am. Stat, 42, 152} 1388 \code{Green, P. J., 1984, J. R. Statist. Soc B, 42, 149} 1379 Iteratively Reweighted Least Squares (IRLS) technique \citep[see, 1380 e.g.,][]{Green.1984} to determine the average photometry given the 1381 possible presence of non-Gaussian outliers even within the best subset 1382 of measurements. 1383 1384 %% \note{include a reference to IRLS and describe concept more} 1385 %% \code{http://users.stat.umn.edu/~sandy/courses/8053/handouts/robust.pdf} 1386 %% \code{https://arxiv.org/pdf/0807.0575.pdf} 1387 %% \code{https://www.redalyc.org/pdf/3939/393933924009.pdf} 1388 %% \code{Street, J. O., Carrol, R. J., \& Ruppert D. 1988, Am. Stat, 42, 152} 1389 %% \code{Green, P. J., 1984, J. R. Statist. Soc B, 42, 149} 1390 % https://www.researchgate.net/publication/256800227_Robust_estimation_of_excitation_in_mechanical_systems_under_model_uncertainties 1389 1391 1390 1392 \subsubsection{Selection of Measurements} … … 1498 1500 Pan-STARRS\,1 detections have a relatively high rate of non-Gaussian 1499 1501 outliers, partly because of the wide range of instrumental features 1500 affecting the data (see Paper III). We have used a 1501 technique called Iteratively Reweighted Least Squares (IRLS) fitting 1502 to reduce the sensitivity of the fits to outlier measurements. We 1503 have also used bootstrap resampling to determine confidence limits on 1504 our fits given the observed collection of photometry measurements. In 1505 this case, the analysis is fitting the trivial model that the 1502 affecting the data (see Paper III). \textmod{We have used Iteratively 1503 Reweighted Least Squares (IRLS) fitting to reduce the sensitivity of 1504 the fits to outlier measurements.} 1505 1506 We have also used bootstrap resampling to determine confidence limits 1507 on our fits given the observed collection of photometry measurements. 1508 In this case, the analysis is fitting the trivial model that the 1506 1509 photometry measurements are derived from a population with an 1507 1510 underlying constant value. The discussion below applies to both the … … 1509 1512 photometry fluxes. This technique is used to calculate the average 1510 1513 magnitudes for all three types of photometry stored in the DVO 1511 database: PSF, Kron, and seeing-matched total aperture photometry. 1512 1513 The IRLS analysis starts with an ordinary least squares fit, using the 1514 weights for each measurement as determined from Poisson statistics. 1515 Since our model is a constant flux, this step is equivalent to 1516 calculating a simple weighted average. 1514 database: PSF, Kron, and seeing-matched total aperture photometry. 1515 1516 \textadd{Iteratively-reweighted least-squares fitting describes a 1517 class of parameter estimation techniques in which weights are 1518 modified compared to that derived from the standard error in order 1519 to improve the speed of convergence or the robustness to deviant 1520 measurements. Broad reviews of these techniques can be found in 1521 \cite{Green.1984} and \cite{Street.1988}}. \textmod{In our 1522 implementation, the IRLS analysis} starts with an ordinary least 1523 squares fit, using the weights for each measurement as determined from 1524 Poisson statistics. Since our model is a constant flux, this step is 1525 equivalent to calculating a simple weighted average. 1517 1526 1518 1527 Next, the deviations from the average value for each photometry … … 2980 2989 To further improve the astrometric calibration reliability in this 2981 2990 region, we have generated a new reference catalog combining the PS1 2982 PV3 photometry with astrometry from Gaia DR2 \citep{2018AA...616A...1G}. We are reprocessing all 2983 images from the region North of $+70\mathdegree$ and will provide a 2984 complete Polar Region release using the same data as used for DR2. 2985 This updated release is expected to be available from MAST near the 2986 end of summer 2019. 2991 PV3 photometry with astrometry from Gaia DR2 2992 \citep{2018AA...616A...1G}. We are reprocessing all images from the 2993 region North of $+70\mathdegree$ and will provide a complete Polar 2994 Region release using the same data as used for DR2. This updated 2995 release is expected to be available from MAST near the end of summer 2996 2019. 2987 2997 2988 2998 We consider skycells with more than 10\% bad groups to have been
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