| 1 | \documentclass[12pt]{article}
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| 2 | \usepackage{magic-tdas}
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| 3 |
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| 4 |
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| 5 | \usepackage[latin1]{inputenc}
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| 6 |
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| 7 | \usepackage{amsmath}
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| 8 | \usepackage{amssymb}
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| 9 |
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| 10 | \usepackage{amsthm}
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| 11 | \usepackage{color}
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| 12 |
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| 13 | \usepackage{graphicx}
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| 14 | \usepackage{caption2}
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| 15 |
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| 16 | %\usepackage{citesort}
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| 17 | \usepackage{url}
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| 18 | \usepackage{mdwlist}
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| 19 | \usepackage{lscape}
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| 20 |
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| 21 | \setlength{\parindent}{0cm}
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| 22 |
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| 23 | \sloppy
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| 24 |
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| 25 | \renewcommand{\captionfont}{\small\slshape}
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| 26 | \renewcommand{\baselinestretch}{1.0}
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| 27 | \renewcommand{\arraystretch}{1.0}
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| 28 |
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| 29 | \begin{document}
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| 30 |
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| 31 |
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| 32 |
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| 33 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 34 | %% Please, for the formatting just include here the standard
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| 35 | %% elements: title, author, date, plus TDAScode
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| 36 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 37 | \title{Comparison of Signal Reconstruction Algorithms for the MAGIC Telescope}
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| 38 | \author{H. Bartko, M. Gaug, F. Goebel, A. Moralejo,\\
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| 39 | Th. Schweizer, M. Shayduk, N. Sidro, W. Wittek}
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| 40 | \date{February 21$^{\mathrm{st}}$, 2005\\}
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| 41 | \TDAScode{MAGIC-TDAS 05-xx\\ 050221}
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| 42 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 43 |
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| 44 | %% title %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 45 | \maketitle
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| 46 |
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| 47 | %% abstract %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 48 | \begin{abstract}
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| 49 | Presently, the MAGIC telescope uses a 300~MHz FADC system to sample the transmitted and shaped signals from
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| 50 | the captured Cherenkov light of air showers.
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| 51 | In this note. different algorithms to reconstruct the signal from the read out samples
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| 52 | are described and compared. Criteria for comparison are defined and used to judge the
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| 53 | different extractors applied to calibration signals, cosmics and pedestals. At the end,
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| 54 | extractors are recommended for the most conservative and the most advanced and demanding analyses.
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| 55 | It is shown that the digital filter
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| 56 | can be used to extract and fit single photo-electron pulses from the night sky background.
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| 57 | The achievable time resolution has been derived as a function of the incident number of
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| 58 | photo-electrons.
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| 59 | %\begin{equation}
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| 60 | %\Delta T_{\mathrm{cosmics}} \approx \sqrt{\frac{(2\,\mathrm{ns})^2}{<Q>/{\mathrm{phe}}}
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| 61 | %+ \frac{(4.5\,\mathrm{ns})^2}{<Q>^2/{\mathrm{phe^2}}} + (0.2\,\mathrm{ns})^2} . \nonumber
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| 62 | %\label{eq:time:fitprediction}
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| 63 | %\end{equation}
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| 64 | For galactic backgrounds an image cleaning threshold as low as 5~photo-electrons can be achieved
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| 65 | without using the timing information and for rejecting 99.7\% of noise.
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| 66 | \end{abstract}
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| 67 |
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| 68 | %% contents %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 69 | \newpage
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| 70 | \tableofcontents
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| 71 |
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| 72 | %% body %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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| 73 | %\include{pedplots}
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| 74 | \include{Introduction}
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| 75 | \include{Reconstruction}
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| 76 | \include{Algorithms}
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| 77 | \include{Criteria}
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| 78 | \include{Pedestal}
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| 79 | \include{Calibration}
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| 80 | \include{Pulpo}
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| 81 | \include{MonteCarlo}
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| 82 | \include{Speed}
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| 83 | \include{Results}
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| 84 | \include{Conclusions}
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| 85 | %\include{pheplots}
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| 86 |
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| 87 | \bibliography{bibfile}
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| 88 | \bibliographystyle{bibstyle}
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| 89 |
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| 90 | \end{document}
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| 91 |
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| 92 |
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| 93 |
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