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Changeset 41324


Ignore:
Timestamp:
Apr 3, 2020, 1:33:57 PM (6 years ago)
Author:
eugene
Message:

updates in response to referee; new figure versions

Location:
trunk/doc/release.2015/ps1.analysis
Files:
4 added
7 edited

Legend:

Unmodified
Added
Removed
  • trunk/doc/release.2015/ps1.analysis/Makefile

    r41307 r41324  
    2424PDFPICS = \
    2525pics/peaks.pdf \
    26 pics/FWHM.smooth.trend.ps1.pdf \
     26pics/galplanecut.pdf \
     27pics/FWHM.smooth.trend.v1.ps1.pdf \
    2728pics/radial.profiles.pdf \
    2829pics/moment.class.pdf \
  • trunk/doc/release.2015/ps1.analysis/analysis.tex

    r41316 r41324  
    595595  Footprints                 & Y & Y & N & Y     & \ref{sec:footprints}             & All detections \\
    596596  Moments                    & Y & Y & Y & Y     & \ref{sec:moments}                & All detections \\
    597   PSF Model                  & Y & Y & Y & N$^2$ & \ref{sec:PSF.Model}              & Uses bright, unsat. stars \\
     597  PSF Model                  & Y & Y & Y & N$^2$ & \ref{sec:PSF.Model}              & Selected bright stars \\
    598598  Bright Star Profile        & Y & Y & N & Y     & \ref{sec:very.bright.star}       & Saturated Stars \\
    599599  Radial Profiles v1         & Y & Y & N & Y     & \ref{sec:radial.profile}         & All detections \\
     
    615615\hline
    616616\multicolumn{5}{l}{$^1$ Background subtraction is performed by {\tt ppSub} before calling {\tt psphot}} \\
    617 \multicolumn{5}{l}{$^2$ PSF modeling is perform by {\tt ppSub} on the input warps before calling {\tt psphot}} \\
     617\multicolumn{5}{l}{$^2$ PSF modeling is performed by {\tt ppSub} on the input warps before calling {\tt psphot}} \\
    618618\end{tabular}
    619619\end{center}
     
    961961
    962962\subsection{Initial Source Detection}
     963\label{sec:source.detection}
    963964
    964965\subsubsection{Peak Detection}
     
    11361137  \caption{\label{fig:moments.window} Example of the biases
    11371138    encountered when measuring the second moments.  A simulated image
    1138     was generated using the PS1 PSF profile.  Each panel corresponds
    1139     to a different value of $\sigma_w$, corresponding to the window
    1140     FWHM values as marked.  The solid red line is the true FWHM of the
    1141     PSF used to generate the stars (1.4 arcsec in all cases).  The
    1142     blue solid line is the FWHM of the window function.  The gray dots
    1143     are the FWHM derived from the measured second moments for stars in
    1144     the image.  The median of this distribution (mag $< -10$) is
    1145     listed as ``obs''.  The ratio of the median FWHM to the FWHM of
    1146     the window function is listed as ``ratio'', while the ratio of the
    1147     median FWHM to the true stellar FWHM is listed as ``bias''.  The
    1148     dotted blue line is the target (65\% of the window function).  In
    1149     this example, we would choose $\sigma_w$ between 0.5 and 0.8
    1150     arcseconds so the dotted blue line would match the bright end of
    1151     the gray dots.   See discussion in the text for the choice of
    1152     target window.
    1153 }
     1139    was generated using the PS1 PSF profile.  Panels (a) - (e)
     1140    corresponds to a different value of $\sigma_w$, corresponding to
     1141    the window FWHM values as marked.  The solid red line is the true
     1142    FWHM of the PSF used to generate the stars (1.4 arcsec in all
     1143    cases).  The blue solid line is the FWHM of the window function.
     1144    The gray dots are the FWHM derived from the measured second
     1145    moments for stars in the image.  The median of this distribution
     1146    (mag $< -10$) is listed as ``obs''.  The ratio of the median FWHM
     1147    to the FWHM of the window function is listed as ``ratio'', while
     1148    the ratio of the median FWHM to the true stellar FWHM is listed as
     1149    ``bias''.  The dotted blue line is the target (65\% of the window
     1150    function).  In this example, we would choose $\sigma_w$ between
     1151    0.5 and 0.8 arcseconds (FWHM between 2.64 and 3.52 arcseconds), so
     1152    the dotted blue line would match the bright end of the gray dots.
     1153    See discussion in the text for the choice of target window.  }
    11541154  \end{center}
    11551155\end{figure}
     
    14581458    arcsec (blue).  The red and blue points are individual pixel
    14591459    values.  The black line shows the PSF model with radial trend of
    1460     the form $(1 + \kappa r^2 + r^{3.33})^{-1}$.}
    1461 
     1460    the form $(1 + \kappa r^2 + r^{3.33})^{-1}$.  The models use a 1D
     1461    average of the 2D analytical portion of the PSF models fitted
     1462    to these specific stars in their standard analysis.  }
    14621463  \end{center}
    14631464\end{figure}
     
    15561557  \includegraphics[width=\hsize]{{\picdir/moment.class}.\plotext}
    15571558  \caption{\label{fig:moment.class} Illustration of PSF star selection
    1558     using the second moments in $X_{\rm ccd}$ and $Y_{\rm ccd}$
    1559     directions.  The dominant clump is located in this diagram.
    1560     Galaxies tend to have a range of sizes and thus spread out above
    1561     the stars.  Cosmic rays also have a range of sizes, with one
    1562     dimension smaller than the PSF.  The red circle represents the PSF
    1563     star candidates. }
     1559    using the second moments. \textadd{Each point represents the
     1560      second moments in the $X_{\rm ccd}$ and $Y_{\rm ccd}$ directions
     1561      for sources measured in one chip (XY32) from a particular PS\,1
     1562      exposure (o6065g0428o)}.  The dominant clump is located in this
     1563    diagram \textadd{to identify the stars.}  Galaxies tend to have a range of
     1564    sizes and thus spread out above the stars.  Cosmic rays also have
     1565    a range of sizes, with one dimension smaller than the PSF.  The
     1566    red circle represents the PSF star candidates. }
    15641567  \end{center}
    15651568\end{figure}
     
    18941897sky radius.  These values are saved in the \textmod{output FITS catalog files}, but
    18951898not sent to the PSPS.  The sky radius value is used below in the
    1896 calculation of the Kron magnitude.
     1899calculation of the Kron magnitude. \note{used in both versions?}
     1900\note{calculated for the second pass?}
    18971901
    18981902\subsubsection{Kron Magnitudes}
     
    22372241After a first pass through the image, in which the brighter sources
    22382242above a high threshold level have been detected, measured, and
    2239 subtracted, \ippprog{psphot} optionally begins a second pass at the image.  In
    2240 this stage, the new peaks are detected on the image with the bright
    2241 sources subtracted.  In this pass, the peak detection process uses the
    2242 variance image to test the validity of the individual peaks.  All peaks
    2243 with a significance greater than a user-defined minimum threshold are
    2244 accepted as sources of potential interest. 
    2245 
    2246 The sources which are measured in this faint-source stage are clearly
    2247 low significance detections.  The PV3 threshold for the bright source
    2248 analysis is a signal-to-noise of 20.  The flag bit
    2249 \code{PM_SOURCE_MODE2_PASS1_SRC} is raised for sources detected in
    2250 this initial analysis stage.  The lower limit cutoff for the faint
    2251 source analysis in PV3 is a signal-to-noise of 5.0.  Sources detected
    2252 in the faint source stage are fitted with the PSF model using the
    2253 linear, ensemble fitting process.
     2243subtracted, \ippprog{psphot} optionally begins a second pass at the
     2244image.  \textadd{Some of the steps described in the previous sections
     2245  are repeated in this analysis, though with some modifications as
     2246  discussed below.}
     2247
     2248\textadd{The source detection steps described in
     2249  Section~\ref{sec:source.detection} are repeated.  To start, the
     2250  sources detected in the previous steps are subtracted from the
     2251  image, and the variance enhanced by adding the variance predicted by
     2252  the model to the variance image, doubling the effective variance at
     2253  the location of previously detected sources.  As in
     2254  Section~\ref{sec:peaks}, the image is smoothed, but in this pass it
     2255  is convolved with the PSF determined above, not a place-holder
     2256  Gaussian.  The new peaks are detected on the smoothed image. The
     2257  peak detection process again uses the variance image to test the
     2258  significance of the individual peaks.  All peaks with a significance
     2259  greater than a user-defined minimum threshold are accepted as
     2260  sources of potential interest.  Footprints are again generated as in
     2261  Section~\ref{sec:footprints}.}
     2262
     2263\textadd{Next, moments are measured as in Section~\ref{sec:moments}.
     2264  In this pass, however, the size of the window function applied for
     2265  the measurement of the moments is fixed at the value determined from
     2266  the bright source analysis.  All sources, including those measured
     2267  in the bright-source analysis (which are re-added to the image and
     2268  their variance reset), are then simultaneously fit for their flux
     2269  normalizations as in Section~\ref{sec:ensemble.fitting}.  In this
     2270  step, the `best' model is used for each source, either a PSF model
     2271  or the unconvolved extended source model determined in
     2272  Section~\ref{sec:nonlinear.galaxy.model}.  For the newly detected
     2273  sources, the PSF model is used, with the position set by the
     2274  centroids.}
     2275
     2276\textadd{After the flux-normalization is calculated, the moments
     2277  are used to calculate the preliminary Kron radius and flux (see
     2278  Section~\ref{sec:kron.mags}).  These are in turn used to assess the
     2279  source sizes as in Section~\ref{sec:source.size}.  However, the
     2280  non-linear fitting steps for the PSF model fits
     2281  (Section~\ref{sec:nonlinear.psf.model}) and the extended source
     2282  model fits (Section~\ref{sec:nonlinear.galaxy.model}) are not
     2283  performed for these faint sources.  These steps are skipped for two
     2284  reasons: First, the non-linear fitting steps are costly in terms of
     2285  computation time and the faint sources usually far out-number the
     2286  brighter sources.  Second, since these are faint sources they do not
     2287  have the signal-to-noise to constrain models with many additional
     2288  parameters.  In addition, the positions (for PSF sources) are not
     2289  much improved using the non-linear fitting compared with the
     2290  non-parametric centroid measurement for these faint sources.
     2291  \note{show with a model}.}
     2292
     2293The PV3 threshold for the bright source analysis is a signal-to-noise
     2294of 20.  The flag bit \code{PM_SOURCE_MODE2_PASS1_SRC} is raised for
     2295sources detected in this initial analysis stage.  The lower limit
     2296cutoff for the faint source analysis in PV3 is a signal-to-noise of
     22975.0.
    22542298
    22552299In the \ippprog{psphotStack} version of the code, the 5 filter images
     
    23332377    pointing compared to the next 17 images, after correction for a
    23342378    relative zero point, as a function of the instrumental magnitudes
    2335     above the detection threshold.  Black dots are from stars for
    2336     which both measurements have {\tt PSF\_QF} $> 0.95$, while grey
     2379    above the detection threshold.  Gray dots are from stars for
     2380    which both measurements have {\tt PSF\_QF} $> 0.95$, while light red
    23372381    dots have lower {\tt PSF\_QF} values.  The top three panels (a) -
    23382382    (c) show histograms in three magnitude ranges for the magnitude
     
    30663110 \includegraphics[width=\hsize,clip]{\picdir/{galaxy.exp.complete}.\plotext}
    30673111 \includegraphics[width=\hsize,clip]{\picdir/{galaxy.dev.complete}.\plotext}
    3068   \caption{\label{fig:galaxy.complete} Top: Completeness curves for
    3069     simulated galaxies with Exponential profiles.  Bottom:
    3070     Completeness curves for simulated galaxies with DeVaucouleur
    3071     profiles.  The curves are shown as a function of the difference
    3072     between the injected instrumental magnitude of the galaxy and the
    3073     magnitude corresponding to the $5\sigma$ detection threshold for a
    3074     PSF-like source.  The black curves shows the compleness for all
    3075     galaxies.  The three colored curves show the completeness for
    3076     three major axis ranges. Compact galaxies are more likely to be
    3077     detected since peaks are detected after convolution with the
    3078     PSF. }
     3112  \caption{\label{fig:galaxy.complete} {\bf Panel (a):} Completeness
     3113    curves for simulated galaxies with Exponential profiles.  {\bf
     3114      Panel (b):} Completeness curves for simulated galaxies with
     3115    DeVaucouleur profiles.  The curves are shown as a function of the
     3116    difference between the injected instrumental magnitude of the
     3117    galaxy and the magnitude corresponding to the $5\sigma$ detection
     3118    threshold for a PSF-like source.  The black curves shows the
     3119    compleness for all galaxies.  The three colored curves show the
     3120    completeness for three major axis ranges. Compact galaxies are
     3121    more likely to be detected since peaks are detected after
     3122    convolution with the PSF. \textadd{The simulated images have seeing of
     3123    1\arcsec, equal to pixels.}}
    30793124  \end{center}
    30803125\end{figure}
     
    30843129the Exponential and DeVaucouleur models, respectively. 
    30853130Both figures show the reliability of the measured magnitudes, major
    3086 and minor axis sizes, and ellipticities.  For all recovered
     3131and minor axis sizes, and \textadd{ellipticities, which we represent as
     3132$\frac{R_{\rm Major} - R_{\rm Minor}}{R_{\rm Major} + R_{\rm
     3133    Minor}}$. Galaxies are grouped in 0.1 magnitude bins based
     3134on their injected magnitudes. 
     3135For all recovered
    30873136parameters, the standard deviation of the difference between the
    3088 measured parameter and the truth value is shown for all galaxies as a
    3089 function of magnitude, as well as for subsets in major-axis ranges.
     3137measured parameter and the truth value is shown for all galaxies in
     3138each magnitude bin, as well as for subsets in major-axis ranges.}
    30903139The mean of the difference, illustrating any biases, is also given
    30913140for all galaxies.  The comparison for the major and minor axis sizes
     
    31063155  \begin{center}
    31073156 \includegraphics[width=\hsize,clip]{\picdir/{galaxy.exp.params}.\plotext}
     3157
    31083158  \caption{\label{fig:exp.params} Parameter recovery for simulated
    3109     galaxies with Exponential profiles.  }
     3159    galaxies with Exponential profiles.  In each panel, we show
     3160    several statistics for the difference between the truth parameter
     3161    and the measured value for galaxies in a series of brightness
     3162    bins, ranging from 5 magnitudes to 0.5 magnitudes brighter than
     3163    the PSF $5-\sigma$ detection threshold.  Statistics, as shown in
     3164    the legend, include the average difference, the standard deviation
     3165    for all galaxies in the bin, and the standard deviations for 3
     3166    major axis ranges.  Panel (a) through (d) show in order the
     3167    recovered magnitudes, ellipticity, major axis size; minor axis
     3168    size.  Panels (e) and (f) show statistics for the major and minor
     3169    axis difference as a fraction of the truth value.  The average
     3170    magnitude difference is plotted so that positive numbers mean the
     3171    fitted flux is brighter than the injected flux.  }
    31103172  \end{center}
    31113173\end{figure*}
     
    31163178 \includegraphics[width=\hsize,clip]{\picdir/{galaxy.dev.params}.\plotext}
    31173179  \caption{\label{fig:dev.params} Parameter recovery for simulated
    3118     galaxies with DeVaucouleur profiles.  }
     3180    galaxies with DeVaucouleur profiles.  See
     3181    Figure~\ref{fig:exp.params} for complete explanation.}
    31193182  \end{center}
    31203183\end{figure*}
  • trunk/doc/release.2015/ps1.analysis/response.txt

    r41317 r41324  
    7777state the same for galaxy astrometry, fluxes and colors.
    7878
    79 ****
     79**** TBD
    8080
    8181A detail of the code is presented (variable names, etc) that imply
     
    9696that the photometric goals are achieved
    9797
    98 **** see note section Forced PSF Phot
     98**** TBD see note section Forced PSF Phot
    9999
    100100- Sec 7, where the image differencing detections and photometry is used
     
    437437range.
    438438
    439 **** TDB: was the turned on for PV3?
     439**** TBD: was the turned on for PV3?
    440440
    441441Sec 4.7:
     
    719719each of the sub-panels (a), (b), etc, and describe in the caption.
    720720
    721 **** TBD: fixed for Figures 2, 5, 6 TBD: 8, 9, 10
     721** fixed for Figures 2, 5, 6, 8, 9, 10
    722722
    723723Figure 2:
     
    746746particular stars
    747747
    748 **** TBD: NEED to examine how figure was created
     748** the lines are a 1D average of the PSF models fitted to these stars (added to caption)
    749749
    750750Figure 4:
     
    752752denoted by a point.
    753753
    754 **** TBD
     754** updated the caption
    755755
    756756Figures 5 and 6:
     
    766766- Caption should specify the seeing of these images (not in the text either).
    767767
    768 **** TBD
     768** added to caption and text
    769769
    770770Figures 8 and 9:
     
    774774in the text. The other 4 panels could refer to the explanation in Sec 5.5.
    775775
    776 **** TBD
     776** captions update to be more informative.
    777777
    778778References:
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