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Changeset 41188 for trunk


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Timestamp:
Dec 2, 2019, 9:16:59 AM (7 years ago)
Author:
eugene
Message:

more referee comments

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1 edited

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  • trunk/doc/release.2015/ps1.calibration/calibration.tex

    r41181 r41188  
    13671367fluxes.
    13681368
    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, a single object may have anywhere from zero to roughly twenty
     1369The first challenge is to select which measurements to use in the
     1370calculation of the average photometry.  For the $3\pi$ Survey data, a
     1371single object may have anywhere from zero to roughly twenty
    13721372measurements in a given filter.  Not all measurements are of equal
    13731373value, but we need a process which assigns an average photometry value
     
    13771377measurements available in each filter for each object.  Once the set
    13781378of 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}
     1379Iteratively Reweighted Least Squares (IRLS) technique \citep[see,
     1380  e.g.,][]{Green.1984} to determine the average photometry given the
     1381possible presence of non-Gaussian outliers even within the best subset
     1382of 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
    13891391
    13901392\subsubsection{Selection of Measurements}
     
    14981500Pan-STARRS\,1 detections have a relatively high rate of non-Gaussian
    14991501outliers, 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
     1502affecting 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
     1506We have also used bootstrap resampling to determine confidence limits
     1507on our fits given the observed collection of photometry measurements.
     1508In this case, the analysis is fitting the trivial model that the
    15061509photometry measurements are derived from a population with an
    15071510underlying constant value.  The discussion below applies to both the
     
    15091512photometry fluxes.  This technique is used to calculate the average
    15101513magnitudes 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. 
     1514database: 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
     1523squares fit, using the weights for each measurement as determined from
     1524Poisson statistics.  Since our model is a constant flux, this step is
     1525equivalent to calculating a simple weighted average.
    15171526
    15181527Next, the deviations from the average value for each photometry
     
    29802989To further improve the astrometric calibration reliability in this
    29812990region, 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.
     2991PV3 photometry with astrometry from Gaia DR2
     2992\citep{2018AA...616A...1G}.  We are reprocessing all images from the
     2993region North of $+70\mathdegree$ and will provide a complete Polar
     2994Region release using the same data as used for DR2.  This updated
     2995release is expected to be available from MAST near the end of summer
     29962019.
    29872997
    29882998We consider skycells with more than 10\% bad groups to have been
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