| 1 | \section{Monte Carlo \label{sec:mc}}
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| 2 |
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| 3 | \subsection{Charge Signals with Simulated Noise \label{sec:mc:charge}}
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| 4 |
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| 5 | \begin{figure}[htp]%%[t!]
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| 6 | \centering
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| 7 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_NoNoise_HiGain.eps}
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| 8 | \vspace{\floatsep}
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| 9 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_HiGain.eps}
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| 10 | \vspace{\floatsep}
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| 11 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_NoNoise_LoGain.eps}
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| 12 | \vspace{\floatsep}
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| 13 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_LoGain.eps}
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| 14 | \caption[Charge per Number of photo-electrons Fixed Windows]{Extracted charge per photoelectron versus number of photoelectrons,
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| 15 | for fixed window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 16 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 17 | \label{ChargeDivNphe_FixW}
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| 18 | \end{figure}
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| 19 |
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| 20 | \begin{figure}[htp]
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| 21 | \centering
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| 22 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_HiGain.eps}
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| 23 | \vspace{\floatsep}
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| 24 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_HiGain.eps}
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| 25 | \vspace{\floatsep}
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| 26 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_LoGain.eps}
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| 27 | \vspace{\floatsep}
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| 28 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_LoGain.eps}
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| 29 | \caption[Charge per Number of photo-electrons Sliding Windows]{Extracted charge per photoelectron versus number of photoelectrons,
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| 30 | for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 31 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 32 | \label{ChargeDivNphe_SlidW}
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| 33 | \end{figure}
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| 34 |
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| 35 | \begin{figure}[htp]
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| 36 | \centering
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| 37 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_HiGain.eps}
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| 38 | \vspace{\floatsep}
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| 39 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_HiGain.eps}
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| 40 | \vspace{\floatsep}
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| 41 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_LoGain.eps}
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| 42 | \vspace{\floatsep}
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| 43 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_LoGain.eps}
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| 44 | \caption[Charge per Number of photo-electrons Spline and Digital Filter]{Extracted charge per photoelectron versus number of photoelectrons,
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| 45 | for spline and digital filter extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 46 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 47 | \label{ChargeDivNphe_DFSpline}
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| 48 | \end{figure}
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| 49 |
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| 50 | \begin{figure}[htp]%%[t!]
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| 51 | \centering
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| 52 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_NoNoise_HiGain.eps}
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| 53 | \vspace{\floatsep}
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| 54 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_WithNoise_HiGain.eps}
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| 55 | \vspace{\floatsep}
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| 56 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_NoNoise_LoGain.eps}
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| 57 | \vspace{\floatsep}
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| 58 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_WithNoise_LoGain.eps}
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| 59 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_LoGain.eps}
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| 60 | \caption[Bias Fixed Windows]{The measured bias (extracted charge divided by the conversion factor minus the number of photoelectrons)
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| 61 | versus number of photoelectrons,
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| 62 | for fixed window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 63 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 64 | \label{ConversionvsNphe_FixW}
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| 65 | \end{figure}
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| 66 |
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| 67 | \begin{figure}[htp]
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| 68 | \centering
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| 69 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_NoNoise_HiGain.eps}
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| 70 | \vspace{\floatsep}
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| 71 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_WithNoise_HiGain.eps}
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| 72 | \vspace{\floatsep}
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| 73 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_NoNoise_LoGain.eps}
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| 74 | \vspace{\floatsep}
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| 75 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_WithNoise_LoGain.eps}
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| 76 | \caption[Bias Sliding Windows]{The measured bias (extracted charge divided by the conversion factor minus the number of photoelectrons)
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| 77 | versus number of photoelectrons,
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| 78 | for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 79 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 80 | \label{ConversionvsNphe_SlidW}
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| 81 | \end{figure}
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| 82 |
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| 83 | \begin{figure}[htp]
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| 84 | \centering
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| 85 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_NoNoise_HiGain.eps}
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| 86 | \vspace{\floatsep}
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| 87 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_WithNoise_HiGain.eps}
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| 88 | \vspace{\floatsep}
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| 89 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_NoNoise_LoGain.eps}
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| 90 | \vspace{\floatsep}
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| 91 | \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_WithNoise_LoGain.eps}
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| 92 | \caption[Bias Spline and Digital Filter]{The measured bias (extracted charge divided by the conversion factor minus the number of photoelectrons)
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| 93 | versus number of photoelectrons,
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| 94 | for spline and digital filter extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 95 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 96 | \label{ConversionvsNphe_DFSpline}
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| 97 | \end{figure}
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| 98 |
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| 99 | \begin{figure}[htp]
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| 100 | \centering
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| 101 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_NoNoise_HiGain.eps}
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| 102 | \vspace{\floatsep}
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| 103 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_WithNoise_HiGain.eps}
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| 104 | \vspace{\floatsep}
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| 105 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_NoNoise_LoGain.eps}
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| 106 | \vspace{\floatsep}
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| 107 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_WithNoise_LoGain.eps}
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| 108 | \caption[Charge Resolution Fixed Windows]{The measured resolution (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons,
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| 109 | for fixed window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 110 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 111 | \label{ChargeRes_FixW}
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| 112 | \end{figure}
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| 113 |
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| 114 | \begin{figure}[htp]
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| 115 | \centering
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| 116 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_NoNoise_HiGain.eps}
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| 117 | \vspace{\floatsep}
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| 118 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_WithNoise_HiGain.eps}
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| 119 | \vspace{\floatsep}
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| 120 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_NoNoise_LoGain.eps}
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| 121 | \vspace{\floatsep}
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| 122 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_WithNoise_LoGain.eps}
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| 123 | \caption[Charge Resolution Sliding Windows]{The measured resolution (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons,
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| 124 | for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 125 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 126 | \label{ChargeRes_SlidW}
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| 127 | \end{figure}
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| 128 |
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| 129 | \begin{figure}[htp]
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| 130 | \centering
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| 131 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_NoNoise_HiGain.eps}
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| 132 | \vspace{\floatsep}
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| 133 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_WithNoise_HiGain.eps}
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| 134 | \vspace{\floatsep}
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| 135 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_NoNoise_LoGain.eps}
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| 136 | \vspace{\floatsep}
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| 137 | \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_WithNoise_LoGain.eps}
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| 138 | \caption[Charge Resolution Spline and Digital Filter]{The measured resolution
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| 139 | (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons,
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| 140 | for spline and digital filter extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 141 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 142 | \label{ChargeRes_DFSpline}
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| 143 | \end{figure}
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| 144 |
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| 145 | \clearpage
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| 146 |
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| 147 | \subsection{Charge Signals with and without Simulated Noise \label{sec:mc:chargenoise}}
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| 148 |
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| 149 | \begin{figure}[htp]
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| 150 | \centering
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| 151 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_HiGain.eps}
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| 152 | \vspace{\floatsep}
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| 153 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_HiGain.eps}
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| 154 | \vspace{\floatsep}
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| 155 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_DFSpline_HiGain.eps}
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| 156 | \caption[Bias due to noise high-gain]{Bias due to noise: Difference of extracted charge of same events, with and without simulated noise,
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| 157 | for different extractor methods in the high-gain region.}
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| 158 | \label{Bias_HiGain}
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| 159 | \end{figure}
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| 160 |
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| 161 | \begin{figure}[htp]
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| 162 | \centering
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| 163 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_LoGain.eps}
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| 164 | \vspace{\floatsep}
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| 165 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_LoGain.eps}
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| 166 | \vspace{\floatsep}
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| 167 | \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_DFSpline_LoGain.eps}
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| 168 | \caption[Bias due to noise low-gain]{Bias due to noise: Difference of extracted charge of same events, with and without simulated noise,
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| 169 | for different extractor methods in the low-gain region.}
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| 170 | \label{Bias_LoGain}
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| 171 | \end{figure}
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| 172 |
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| 173 | \clearpage
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| 174 |
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| 175 | \subsection{Arrival Times \label{sec:mc:times}}
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| 176 |
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| 177 | \begin{figure}[htp]%%[t!]
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| 178 | \centering
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| 179 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_NoNoise_HiGain.eps}
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| 180 | \vspace{\floatsep}
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| 181 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_WithNoise_HiGain.eps}
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| 182 | \vspace{\floatsep}
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| 183 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_NoNoise_LoGain.eps}
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| 184 | \vspace{\floatsep}
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| 185 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_WithNoise_LoGain.eps}
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| 186 | \caption[Time Resolution Sliding Windows]{The measured time resolution (RMS of extracted time minus simulated time)
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| 187 | versus number of photoelectrons,
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| 188 | for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 189 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 190 | \label{TimeRes_SlidW}
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| 191 | \end{figure}
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| 192 |
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| 193 | \begin{figure}[htp]
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| 194 | \centering
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| 195 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_NoNoise_HiGain.eps}
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| 196 | \vspace{\floatsep}
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| 197 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_WithNoise_HiGain.eps}
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| 198 | \vspace{\floatsep}
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| 199 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_NoNoise_LoGain.eps}
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| 200 | \vspace{\floatsep}
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| 201 | \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_WithNoise_LoGain.eps}
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| 202 | \caption[Time Resolution Spline and Digital Filter]{The measured time resolution (RMS of extracted time minus simulated time)
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| 203 | versus number of photoelectrons,
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| 204 | for spline and digital filter window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the
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| 205 | low-gain regions. Left: without noise, right: with simulated noise.}
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| 206 | \label{TimeRes_DFSpline}
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| 207 | \end{figure}
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| 208 |
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| 209 |
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| 210 | %%% Local Variables:
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| 211 | %%% mode: latex
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| 212 | %%% TeX-master: "MAGIC_signal_reco"
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| 213 | %%% End:
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