Changeset 6575 for trunk/MagicSoft/TDAS-Extractor

Timestamp:

02/17/05 19:22:24 (20 years ago)

Author:

gaug

Message:

*** empty log message ***

File:

• trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex (modified) (9 diffs)

trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex

@@ -1 +1 @@
 \section{Monte Carlo \label{sec:mc}}
 
-\subsection{Charge Signals \label{sec:mc:charge}}
-
-Comparing MC signal with and w/o noise for high and low gain pulses.
+\subsection{Charge Signals with Simulated Noise \label{sec:mc:charge}}
 
 \begin{figure}[htp]%%[t!]
@@ -108 +106 @@
   \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_WithNoise_LoGain.eps}
-\caption[Resolution Fixed Windows]{The measured resolution (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons, 
+\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, 
 for fixed window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the 
 low-gain regions. Left: without noise, right: with simulated noise.}
@@ -123 +121 @@
   \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_WithNoise_LoGain.eps}
-\caption[Resolution Sliding Windows]{The measured resolution (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons, 
+\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, 
 for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the 
 low-gain regions. Left: without noise, right: with simulated noise.}
@@ -138 +136 @@
   \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_WithNoise_LoGain.eps}
-\caption[Resolution Spline and Digital Filter]{The measured resolution 
+\caption[Charge Resolution Spline and Digital Filter]{The measured resolution 
 (RMS of extracted charge divided by the conversion factor minus the number of photoelectrons) versus number of photoelectrons, 
 for spline and digital filter extractors in different window sizes. The top plots show the high-gain and the bottom ones show the 
@@ -145 +143 @@
 \end{figure}
 
+\subsection{Charge Signals with and without Simulated Noise \label{sec:mc:chargenoise}}
+
 \begin{figure}[htp]
 \centering
@@ -152 +152 @@
   \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_DFSpline_HiGain.eps}
-\caption{ Charge bias: comparation bwtween MC files with and without noise, for 
-different extractor methods in high gain region.}
+\caption[Bias due to noise high-gain]{Bias due to noise: Difference of extracted charge of same events, with and without simulated noise, 
+for different extractor methods in the high-gain region.}
 \label{Bias_HiGain}
 \end{figure}
@@ -163 +163 @@
   \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_LoGain.eps}
   \vspace{\floatsep}
-  \includegraphics[width=0.49Q\linewidth]{TimeAndChargePlots/TDAS_Bias_DFSpline_LoGain.eps}
-\caption{ Charge bias: comparation bwtween MC files with and without noise, for 
-different extractor methods in low gain region.}
+  \includegraphics[width=0.49Q\linewidth]{TimeAndChargePlots/TDAS_Bias_DFSpline_LoGain.eps} 
+\caption[Bias due to noise low-gain]{Bias due to noise: Difference of extracted charge of same events, with and without simulated noise, 
+for different extractor methods in the low-gain region.}
 \label{Bias_LoGain}
 \end{figure}
 
+\subsection{Arrival Times \label{sec:mc:times}}
+
 \begin{figure}[htp]%%[t!]
 \centering
@@ -178 +180 @@
 \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_WithNoise_LoGain.eps}
-\caption{Time Resolution for Sliding extractors in deifferent window sizes for low (down) and high (upper) 
-gain contribution, with (right) and with out (left) noise.}
+\caption[Time Resolution Sliding Windows]{The measured time resolution (RMS of extracted time minus simulated time) 
+versus number of photoelectrons, 
+for sliding window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the 
+low-gain regions. Left: without noise, right: with simulated noise.}
 \label{TimeRes_SlidW}
 \end{figure}
@@ -192 +196 @@
 \vspace{\floatsep}
   \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_WithNoise_LoGain.eps}
-\caption{Time Resolution for Splines and Digital Filter extractors for low (down) and high (upper)  
-gain contribution, with (right) and with out (left) noise.}
+\caption[Time Resolution Spline and Digital Filter]{The measured time resolution (RMS of extracted time minus simulated time) 
+versus number of photoelectrons, 
+for spline and digital filter window extractors in different window sizes. The top plots show the high-gain and the bottom ones show the 
+low-gain regions. Left: without noise, right: with simulated noise.}
 \label{TimeRes_DFSpline}
 \end{figure}