source: trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex@ 6585

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