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trunk/doc/release.2015/ps1.analysis/analysis.tex
r40614 r40689 2676 2676 models for each galaxy model measured for the stack image. 2677 2677 2678 \subsection{Galaxy Lensing Parameters} 2679 2680 \begin{verbatim} 2681 * background : KSB, related (mention Deacon et al here or at the end?) 2682 * second moments are discussed above (same values, including window function as given) 2683 * write out the KSB formalism 2684 * stellar parameters using PSF stars 2685 * output parameters 2686 * this is only done on warp -- move to ForceWarp section? 2687 \end {verbatim} 2688 2689 Weak-lensing studies frequently use non-parametric measurements of the 2690 ellipticities of galaxies to quantify the strength of gravitational 2691 lensing, and thus directly measure mass distributions in the Universe. 2692 The classic approach was originally described by 2693 \cite{1995ApJ...449..460K} and applied to a set of deep HST 2694 observations. The details of the technique were further refined by 2695 \cite{1998ApJ...504..636H}; in the discussion below we primarily use 2696 their notation, though we explicitly cast their integrals as sums over 2697 discrete pixels. 2698 2699 The KSB-style analysis of object ellipticities has also been used by 2700 several authors to search for margially-resolved binary stars 2701 in wide-field imaging data. The use of the lensing statistics for 2702 this application was described by \cite{2005ApJ...626.1070H} in the 2703 context of vetting planet transit events in data from the Optical 2704 Gravitational Lensing Experiment (OGLE). \cite{2013ApJS..206...18T} 2705 applied the techinique to PTF data to search for binary stars and 2706 \cite{2017MNRAS.468.3499D} used the same technique to search for 2707 binary companions to known ultracool dwarfs using Pan-STARRS $\3pi$ 2708 data. The work by \cite{2017MNRAS.468.3499D} used images and their 2709 own analysis of the pixels with the program Sextractor 2710 \citep{Bertin.ref}. 2711 2712 For the Pan-STARRS $\3pi$ PV3 analysis, we have measured the full set 2713 of KSB lensing parameters for \note{which subset?} of the data to 2714 enable both lensing studies and binary / multiple star searches. Here 2715 we describe the measurements as performed within \ippprog{psphot}, 2716 reviewing the mathematical framework as described by 2717 \cite{1995ApJ...449..460K} and \cite{1998ApJ...504..636H}. 2718 2719 The goal of the KSB technique is to measure the intrinsic ellipticity 2720 of objects (i.e., galaxies, in the case of weak lensing studies) as 2721 would be observed sky on the without instrumental effects. The 2722 analysis starts with the observed ellipticity of the object as 2723 represented by the two polarization components derived from the second 2724 moments (see Section~\ref{sec:moments}): 2725 \begin{eqnarray} 2726 e_1 = \frac{M_{xx} - M_{yy}}{M_{xx} + M_{yy}} \\ 2727 e_2 = \frac{2 M_{xy}}{M_{xx} + M_{yy}}. \\ 2728 \end{eqnarray} 2729 These two quantities have values which range from -1 to +1, with a 2730 circularly-symmetric object having $(e_1,e_2) = 0.0,0.0$. The two 2731 polarization components vary sinusoidally with twice the position 2732 angle of the object: an elongated object aligned with the $x$-pixel 2733 axis will have positive values of $e_1$ and $e_2$ values near zero, 2734 while the same object aligned with the $y$-pixel axis will negative 2735 $e_1$ values. An object with a position angle on the 45\degree\ lines 2736 between the pixel axes will have large positive or negative values of 2737 $e_2$ and low absoluate values of $e_1$. 2738 2739 \note{need for the window function}. 2740 2741 The observed ellipticity of an object observed in a real instrument 2742 will be affected by the instrumental signature of the instrument. To 2743 first order, the effect on the polarization components can be 2744 described as a combination of ``smear'', in which the observed shape 2745 is more circularized (driving $e_1,e_2$ to low absolute values) and 2746 ``shear'', in which the observed shape is stretched in one direction 2747 relative to the others (driving $e_1,e_2$ to larger absolute values). 2748 With sufficient understanding of the image PSF, both shear and smear 2749 terms can be corrected. 2750 2751 2752 2753 @ARTICLE{2017MNRAS.468.3499D, 2754 author = {{Deacon}, N.~R. and {Magnier}, E.~A. and {Best}, W.~M.~J. and 2755 {Liu}, M.~C. and {Dupuy}, T.~J. and {Chambers}, K.~C. and {Draper}, P.~W. and 2756 {Flewelling}, H. and {Metcalfe}, N. and {Tonry}, J.~L. and {Wainscoat}, R.~J. and 2757 {Waters}, C.}, 2758 title = "{Identification of partially resolved binaries in Pan-STARRS 1 data}", 2759 journal = {\mnras}, 2760 archivePrefix = "arXiv", 2761 eprint = {1702.05491}, 2762 primaryClass = "astro-ph.SR", 2763 keywords = {binaries: visual, brown dwarfs}, 2764 year = 2017, 2765 month = jul, 2766 volume = 468, 2767 pages = {3499-3515}, 2768 doi = {10.1093/mnras/stx440}, 2769 adsurl = {http://adsabs.harvard.edu/abs/2017MNRAS.468.3499D}, 2770 adsnote = {Provided by the SAO/NASA Astrophysics Data System} 2771 } 2772 2773 @ARTICLE{1995ApJ...449..460K, 2774 author = {{Kaiser}, N. and {Squires}, G. and {Broadhurst}, T.}, 2775 title = "{A Method for Weak Lensing Observations}", 2776 journal = {\apj}, 2777 eprint = {astro-ph/9411005}, 2778 keywords = {COSMOLOGY: OBSERVATIONS, COSMOLOGY: DARK MATTER, GALAXIES: FORMATION, COSMOLOGY: GRAVITATIONAL LENSING, COSMOLOGY: LARGE-SCALE STRUCTURE OF UNIVERSE}, 2779 year = 1995, 2780 month = aug, 2781 volume = 449, 2782 pages = {460}, 2783 doi = {10.1086/176071}, 2784 adsurl = {http://adsabs.harvard.edu/abs/1995ApJ...449..460K}, 2785 adsnote = {Provided by the SAO/NASA Astrophysics Data System} 2786 } 2787 @ARTICLE{1998ApJ...504..636H, 2788 author = {{Hoekstra}, H. and {Franx}, M. and {Kuijken}, K. and {Squires}, G. 2789 }, 2790 title = "{Weak Lensing Analysis of CL 1358+62 Using Hubble Space Telescope Observations}", 2791 journal = {\apj}, 2792 keywords = {GALAXIES: CLUSTERS: INDIVIDUAL ALPHANUMERIC: CL 1358+62, GALAXIES: FUNDAMENTAL PARAMETERS, COSMOLOGY: GRAVITATIONAL LENSING, galaxies: clusters: individual (Cl 1358 + 62), Galaxies: Fundamental Parameters, Cosmology: Gravitational Lensing}, 2793 year = 1998, 2794 month = sep, 2795 volume = 504, 2796 pages = {636-660}, 2797 doi = {10.1086/306102}, 2798 adsurl = {http://adsabs.harvard.edu/abs/1998ApJ...504..636H}, 2799 adsnote = {Provided by the SAO/NASA Astrophysics Data System} 2800 } 2801 @ARTICLE{2005ApJ...626.1070H, 2802 author = {{Hoekstra}, H. and {Wu}, Y. and {Udalski}, A.}, 2803 title = "{An Algorithm to Detect Blends with Eclipsing Binaries in Planet Transit Searches}", 2804 journal = {\apj}, 2805 eprint = {astro-ph/0501353}, 2806 keywords = {Stars: Binaries: Eclipsing, Stars: Planetary Systems}, 2807 year = 2005, 2808 month = jun, 2809 volume = 626, 2810 pages = {1070-1078}, 2811 doi = {10.1086/430299}, 2812 adsurl = {http://adsabs.harvard.edu/abs/2005ApJ...626.1070H}, 2813 adsnote = {Provided by the SAO/NASA Astrophysics Data System} 2814 } 2815 @ARTICLE{2013ApJS..206...18T, 2816 author = {{Terziev}, E. and {Law}, N.~M. and {Arcavi}, I. and {Baranec}, C. and 2817 {Bloom}, J.~S. and {Bui}, K. and {Burse}, M.~P. and {Chorida}, P. and 2818 {Das}, H.~K. and {Dekany}, R.~G. and {Kraus}, A.~L. and {Kulkarni}, S.~R. and 2819 {Nugent}, P. and {Ofek}, E.~O. and {Punnadi}, S. and {Ramaprakash}, A.~N. and 2820 {Riddle}, R. and {Sullivan}, M. and {Tendulkar}, S.~P.}, 2821 title = "{Millions of Multiples: Detecting and Characterizing Close-separation Binary Systems in Synoptic Sky Surveys}", 2822 journal = {\apjs}, 2823 archivePrefix = "arXiv", 2824 eprint = {1210.4550}, 2825 primaryClass = "astro-ph.SR", 2826 keywords = {binaries: close, methods: data analysis, stars: statistics, surveys, techniques: image processing }, 2827 year = 2013, 2828 month = jun, 2829 volume = 206, 2830 eid = {18}, 2831 pages = {18}, 2832 doi = {10.1088/0067-0049/206/2/18}, 2833 adsurl = {http://adsabs.harvard.edu/abs/2013ApJS..206...18T}, 2834 adsnote = {Provided by the SAO/NASA Astrophysics Data System} 2835 } 2836 2678 2837 \section{Difference Image Photometry} 2679 2838
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