Changeset 40614 for trunk/doc/release.2015/ps1.analysis/analysis.tex
- Timestamp:
- Jan 26, 2019, 2:24:50 PM (7 years ago)
- File:
-
- 1 edited
-
trunk/doc/release.2015/ps1.analysis/analysis.tex (modified) (13 diffs)
Legend:
- Unmodified
- Added
- Removed
-
trunk/doc/release.2015/ps1.analysis/analysis.tex
r40610 r40614 1 %\documentclass[iop,floatfix]{emulateapj}2 \documentclass[10pt,preprint]{aastex}1 \documentclass[iop,floatfix]{emulateapj} 2 % \documentclass[10pt,preprint]{aastex} 3 3 % \pdfoutput=1 4 4 … … 162 162 contained only average information resulting from the many individual 163 163 images obtained by the $3\pi$ Survey observations. A second data 164 release, DR2, was made available \note{20 January 2019}. DR2 provides164 release, DR2, was made available 28 January 2019. DR2 provides 165 165 measurements from all of the individual exposures, and include an 166 166 improved calibration of the PV3 processing of that dataset. … … 466 466 467 467 \begin{table*} 468 \caption{\label{tab:measurements} \nocode{psphot} measurements performed} % \vspace{-0.5cm} 468 469 \begin{center} 469 470 \footnotesize 470 \caption{\label{tab:measurements} \nocode{psphot} measurements performed} % \vspace{-0.5cm}471 471 \begin{tabular}{lccccll} 472 472 \hline … … 531 531 532 532 \begin{table*} 533 \caption{\label{tab:det_flag_values} \nocode{psphot} Detection Flag Values \#1} % \vspace{-0.5cm} 533 534 \begin{center} 534 535 \footnotesize 535 \caption{\label{tab:det_flag_values} \nocode{psphot} Detection Flag Values \#1} % \vspace{-0.5cm}536 536 \begin{tabular}{lrl} 537 537 \hline … … 578 578 579 579 \begin{table*} 580 \caption{\label{tab:det_flag2_values} \nocode{psphot} Detection Flag Values \#2} % \vspace{-0.5cm} 580 581 \begin{center} 581 582 \footnotesize 582 \caption{\label{tab:det_flag2_values} \nocode{psphot} Detection Flag Values \#2} % \vspace{-0.5cm}583 583 \begin{tabular}{lrl} 584 584 \hline … … 672 672 673 673 \begin{table*} 674 \caption{\label{tab:mask_values} \nocode{psphot} / GPC1 Mask Image Pixel Values} % \vspace{-0.5cm} 674 675 \begin{center} 675 676 \footnotesize 676 \caption{\label{tab:mask_values} \nocode{psphot} / GPC1 Mask Image Pixel Values} % \vspace{-0.5cm}677 677 \begin{tabular}{lcccl} 678 678 \hline … … 1252 1252 a linear model: 1253 1253 \[ 1254 R[(x_{\rm mod},y_{\rm mod})][(x_{\rm ccd},y_{\rm ccd})] = R_o[(x_{\rm 1255 mod},y_{\rm mod})] + R_x[(x_{\rm 1256 mod},y_{\rm mod})] x_{\rm ccd} + R_y[(x_{\rm 1257 mod},y_{\rm mod})] y_{\rm ccd} 1254 \begin{array}{lll} 1255 R[(x_{\rm mod},y_{\rm mod})][(x_{\rm ccd},y_{\rm ccd})] & = & R_o[(x_{\rm mod},y_{\rm mod})] \\ 1256 & + & R_x[(x_{\rm mod},y_{\rm mod})] x_{\rm ccd} \\ 1257 & + & R_y[(x_{\rm mod},y_{\rm mod})] y_{\rm ccd} \\ 1258 \end{array} 1258 1259 \] 1259 1260 where $R[(x_{\rm mod},y_{\rm mod})][(x_{\rm ccd},y_{\rm ccd})]$ is the … … 1367 1368 for a given order of the PSF 2D variations.} % \vspace{-0.5cm} 1368 1369 \begin{center} 1369 \begin{tabular}{lll l}1370 \begin{tabular}{lll} 1370 1371 \hline 1371 1372 \hline 1372 {\bf Minimum Number of Stars} & {\bf Order} & {\bf Number of Grid Cells} \\ 1373 {\bf Minimum Number} & {\bf Order} & {\bf Number of} \\ 1374 {\bf of Stars} & & {\bf Grid Cells} \\ 1373 1375 \hline 1374 16 & 1 & 4 & 4\\1375 54 & 2 & 9 & 6\\1376 128 & 3 & 16 & 8\\1377 300 & 4 & 25 & 12\\1378 576 & 5 & 36 & 16\\1376 16 & 1 & 4 \\ 1377 54 & 2 & 9 \\ 1378 128 & 3 & 16 \\ 1379 300 & 4 & 25 \\ 1380 576 & 5 & 36 \\ 1379 1381 \hline 1380 1382 \end{tabular} … … 2305 2307 2306 2308 % Graham & Driver : Graham A. W., Driver S. P. 2005, PASA 22, 118 2307 a% DOI: https://doi.org/10.1071/AS050012309 % DOI: https://doi.org/10.1071/AS05001 2308 2310 2309 2311 The central pixel of the S\'ersic, DeVaucouleur, and Exponential 2310 models require special handling. When comparing an analytical model2312 models requires special handling. When comparing an analytical model 2311 2313 to the pixelized image recorded by a CCD, one normally treats the 2312 2314 value in a pixel as equivalent to the value of the model at the center … … 2798 2800 image. 2799 2801 2800 \section{Examples and Tests}2801 2802 \note{to be added}2802 % \section{Examples and Tests} 2803 2804 % \section{Conclusions} 2803 2805 2804 2806 \acknowledgments … … 2821 2823 2822 2824 \bibliographystyle{apj} 2823 \bibliography{lib}{}2824 %\input{analysis.bbl}2825 %\bibliography{lib}{} 2826 \input{analysis.bbl} 2825 2827 2826 2828 \end{document} … … 2851 2853 * plots showing the quality of the data? 2852 2854 2853 Tables needed:2854 2855 * table of models?2856 2857 Work still needed:2858 2859 * section 3.5.3 Model applied to detected sources needs to be reviewed2860 2861 * background model description (see waters)2862 2863 % alternative version:2864 % @book{madsen2004methods,2865 % title={Methods for Non-linear Least Squares Problems},2866 % author={Madsen, K. and Nielsen, H.B. and Tingleff, O. and Danmarks tekniske universitet. Informatik og Matematisk Modellering},2867 % url={https://books.google.com/books?id=mhj4MgEACAAJ},2868 % year={2004},2869 % publisher={Informatics and Mathematical Modelling, Technical University of Denmark}2870 % }2871 2872 2855 % programs mentioned in this text: 2873 2856 % psphot … … 2877 2860 % ppSub 2878 2861 2879 2880 kukui: foreach f (`grep PM_SOURCE ~/src/kukui/panstarrs/ipp-trunk/psModules/src/objects/pmSourceMasks.h | grep -v "^#" | prcol 1`)2881 foreach? echo --- $f ---2882 foreach? grep $f */*.tex2883 foreach? end2884 --- PM_SOURCE_MODE_DEFAULT ---2885 --- PM_SOURCE_MODE_PSFMODEL ---2886 --- PM_SOURCE_MODE_EXTMODEL ---2887 --- PM_SOURCE_MODE_FITTED ---2888 --- PM_SOURCE_MODE_FAIL ---2889 ps1.analysis/analysis.tex:flags the object with the bad bit \code{PM_SOURCE_MODE_FAIL}. It is2890 ps1.analysis/analysis.tex:non-linear PSF fit (\code{PM_SOURCE_MODE_FAIL}).2891 --- PM_SOURCE_MODE_POOR ---2892 ps1.analysis/analysis.tex:the flag bit (\code{PM_SOURCE_MODE_POOR}).2893 --- PM_SOURCE_MODE_PAIR ---2894 --- PM_SOURCE_MODE_PSFSTAR ---2895 --- PM_SOURCE_MODE_SATSTAR ---2896 ps1.analysis/analysis.tex:non-linear PSF model fit (\code{PM_SOURCE_MODE_SATSTAR}). Among these2897 ps1.analysis/analysis.tex:saturated stars (\code{PM_SOURCE_MODE_SATSTAR}). These model fits2898 --- PM_SOURCE_MODE_BLEND ---2899 --- PM_SOURCE_MODE_EXTERNAL ---2900 --- PM_SOURCE_MODE_BADPSF ---2901 --- PM_SOURCE_MODE_DEFECT ---2902 --- PM_SOURCE_MODE_SATURATED ---2903 --- PM_SOURCE_MODE_CR_LIMIT ---2904 --- PM_SOURCE_MODE_EXT_LIMIT ---2905 --- PM_SOURCE_MODE_MOMENTS_FAILURE ---2906 --- PM_SOURCE_MODE_SKY_FAILURE ---2907 --- PM_SOURCE_MODE_SKYVAR_FAILURE ---2908 --- PM_SOURCE_MODE_BELOW_MOMENTS_SN ---2909 --- PM_SOURCE_MODE_BIG_RADIUS ---2910 --- PM_SOURCE_MODE_AP_MAGS ---2911 --- PM_SOURCE_MODE_BLEND_FIT ---2912 --- PM_SOURCE_MODE_EXTENDED_FIT ---2913 --- PM_SOURCE_MODE_EXTENDED_STATS ---2914 --- PM_SOURCE_MODE_LINEAR_FIT ---2915 --- PM_SOURCE_MODE_NONLINEAR_FIT ---2916 --- PM_SOURCE_MODE_RADIAL_FLUX ---2917 --- PM_SOURCE_MODE_SIZE_SKIPPED ---2918 --- PM_SOURCE_MODE_ON_SPIKE ---2919 --- PM_SOURCE_MODE_ON_GHOST ---2920 --- PM_SOURCE_MODE_OFF_CHIP ---2921 --- PM_SOURCE_MODE2_DEFAULT ---2922 --- PM_SOURCE_MODE2_DIFF_WITH_SINGLE ---2923 ps1.analysis/analysis.tex:\code{PM_SOURCE_MODE2_DIFF_WITH_SINGLE = 0x00000001} is raised, while2924 --- PM_SOURCE_MODE2_DIFF_WITH_DOUBLE ---2925 ps1.analysis/analysis.tex:\code{PM_SOURCE_MODE2_DIFF_WITH_DOUBLE = 0x00000002} raised.2926 --- PM_SOURCE_MODE2_MATCHED ---2927 --- PM_SOURCE_MODE2_ON_SPIKE ---2928 --- PM_SOURCE_MODE2_ON_STARCORE ---2929 --- PM_SOURCE_MODE2_ON_BURNTOOL ---2930 --- PM_SOURCE_MODE2_ON_CONVPOOR ---2931 --- PM_SOURCE_MODE2_PASS1_SRC ---2932 --- PM_SOURCE_MODE2_HAS_BRIGHTER_NEIGHBOR ---2933 --- PM_SOURCE_MODE2_BRIGHT_NEIGHBOR_1 ---2934 --- PM_SOURCE_MODE2_BRIGHT_NEIGHBOR_10 ---2935 --- PM_SOURCE_MODE2_DIFF_SELF_MATCH ---2936 ps1.analysis/analysis.tex:$\sigma$, then the bit \code{PM_SOURCE_MODE2_DIFF_SELF_MATCH =2937 --- PM_SOURCE_MODE2_SATSTAR_PROFILE ---2938 --- PM_SOURCE_MODE2_ECONTOUR_FEW_PTS ---2939 --- PM_SOURCE_MODE2_RADBIN_NAN_CENTER ---2940 --- PM_SOURCE_MODE2_PETRO_NAN_CENTER ---2941 --- PM_SOURCE_MODE2_PETRO_NO_PROFILE ---2942 --- PM_SOURCE_MODE2_PETRO_INSIG_RATIO ---2943 --- PM_SOURCE_MODE2_PETRO_RATIO_ZEROBIN ---2944 --- PM_SOURCE_MODE2_EXT_FITS_RUN ---2945 --- PM_SOURCE_MODE2_EXT_FITS_FAIL ---2946 --- PM_SOURCE_MODE2_EXT_FITS_RETRY ---2947 --- PM_SOURCE_MODE2_EXT_FITS_NONE ---
Note:
See TracChangeset
for help on using the changeset viewer.
