Index: trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex
===================================================================
--- trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex	(revision 6568)
+++ trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex	(revision 6574)
@@ -1,15 +1,181 @@
 \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.
 
 \begin{figure}[htp]%%[t!]
 \centering
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_NoNoise_HiGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_WithNoise_HiGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_NoNoise_LoGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_WithNoise_LoGain.eps}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_LoGain.eps}
+\caption[Charge per Number of photo-electrons Fixed Windows]{Extracted charge per photoelectron 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.}
+\label{ChargeDivNphe_FixW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_LoGain.eps}
+\caption[Charge per Number of photo-electrons Sliding Windows]{Extracted charge per photoelectron 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{ChargeDivNphe_SlidW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_LoGain.eps}
+\caption[Charge per Number of photo-electrons Spline and Digital Filter]{Extracted charge per photoelectron 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 
+low-gain regions. Left: without noise, right: with simulated noise.}
+\label{ChargeDivNphe_DFSpline}
+\end{figure}
+
+\begin{figure}[htp]%%[t!]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_FixW_WithNoise_LoGain.eps}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeDivNphevsNphe_FixW_WithNoise_LoGain.eps}
+\caption[Bias Fixed Windows]{The measured bias (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.}
+\label{ConversionvsNphe_FixW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_SlidW_WithNoise_LoGain.eps}
+\caption[Bias Sliding Windows]{The measured bias (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.}
+\label{ConversionvsNphe_SlidW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ConversionvsNphe_DFSpline_WithNoise_LoGain.eps}
+\caption[Bias Spline and Digital Filter]{The measured bias (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 
+low-gain regions. Left: without noise, right: with simulated noise.}
+\label{ConversionvsNphe_DFSpline}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_FixW_NoNoise_LoGain.eps}
+  \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, 
+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.}
+\label{ChargeRes_FixW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_SlidW_NoNoise_LoGain.eps}
+  \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, 
+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{ChargeRes_SlidW}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_NoNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_WithNoise_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_NoNoise_LoGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_ChargeRes_DFSpline_WithNoise_LoGain.eps}
+\caption[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 
+low-gain regions. Left: without noise, right: with simulated noise.}
+\label{ChargeRes_DFSpline}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_HiGain.eps}
+  \vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_HiGain.eps}
+  \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.}
+\label{Bias_HiGain}
+\end{figure}
+
+\begin{figure}[htp]
+\centering
+  \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_LoGain.eps}
+  \vspace{\floatsep}
+  \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.}
+\label{Bias_LoGain}
+\end{figure}
+
+\begin{figure}[htp]%%[t!]
+\centering
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_NoNoise_HiGain.eps}
+\vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_WithNoise_HiGain.eps}
+\vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_SlidW_NoNoise_LoGain.eps}
+\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.}
@@ -19,171 +185,14 @@
 \begin{figure}[htp]
 \centering
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_DFSpline_NoNoise_HiGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_DFSpline_WithNoise_HiGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_DFSpline_NoNoise_LoGain.eps}
-\vspace{\floatsep}
-  \includegraphics[width=0.38\linewidth]{TimeAndChargePlots/TDAS_TimeRes_DFSpline_WithNoise_LoGain.eps}
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_NoNoise_HiGain.eps}
+\vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_WithNoise_HiGain.eps}
+\vspace{\floatsep}
+  \includegraphics[width=0.49\linewidth]{TDAS_TimeRes_DFSpline_NoNoise_LoGain.eps}
+\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.}
 \label{TimeRes_DFSpline}
-\end{figure}
-
-\begin{figure}[htp]%%[t!]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_FixW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_FixW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_FixW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_FixW_WithNoise_LoGain.eps}
-\caption{ Charge divided by number of photoelectrons versus the number of photoelectrons, for fixed window extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ChargeDivNphe_FixW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_SlidW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_SlidW_WithNoise_LoGain.eps}
-\caption{ Charge divided by number of photoelectrons versus the number of photoelectrons, for sliding window extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ChargeDivNphe_SlidW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_DFSpline_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeDivNphevsNphe_DFSpline_WithNoise_LoGain.eps}
-\caption{ Charge divided by number of photoelectrons versus the number of photoelectrons, for spline and 
-digital filter extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ChargeDivNphe_DFSpline}
-\end{figure}
-
-\begin{figure}[htp]%%[t!]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_FixW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_FixW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_FixW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_FixW_WithNoise_LoGain.eps}
-\caption{ Charge divided by the conversion factor minus the number of photoelectrons 
-versus the number of photoelectrons, for fixed window extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ConversionvsNphe_FixW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_SlidW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_SlidW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_SlidW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_SlidW_WithNoise_LoGain.eps}
-\caption{ Charge divided by the conversion factor minus the number of photoelectrons  
-versus the number of photoelectrons, for sliding window extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ConversionvsNphe_SlidW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_DFSpline_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_DFSpline_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_DFSpline_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ConversionvsNphe_DFSpline_WithNoise_LoGain.eps}
-\caption{ Charge divided by the conversion factor minus the number of photoelectrons 
-versus the number of photoelectrons, for spline and 
-digital filter extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ConversionvsNphe_DFSpline}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_FixW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_FixW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_FixW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_FixW_WithNoise_LoGain.eps}
-\caption{ Charge resolution versus the number of photoelectrons, for fixed window and spline extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ChargeRes_FixW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_SlidW_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_SlidW_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_SlidW_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_SlidW_WithNoise_LoGain.eps}
-\caption{ Charge resolution versus the number of photoelectrons, for sliding extractors 
-in different window sizes for low (down) and high (upper) gain contribution, with (right) and with out (left) noise.}
-\label{ChargeRes_SlidW}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_DFSpline_NoNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_DFSpline_WithNoise_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_DFSpline_NoNoise_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_ChargeRes_DFSpline_WithNoise_LoGain.eps}
-\caption{ Charge resolution versus the number of photoelectrons, for spline and 
-digital filter extractors in different window sizes for low (down) and high (upper) 
-gain contribution, with (right) and with out (left) noise.}
-\label{ChargeRes_DFSpline}
-\end{figure}
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_HiGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\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.}
-\label{Bias_HiGain}
-\end{figure}
-
-
-\begin{figure}[htp]
-\centering
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_Bias_SlidW_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\linewidth]{TimeAndChargePlots/TDAS_Bias_FixW_LoGain.eps}
-  \vspace{\floatsep}
-  \includegraphics[width=0.4\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.}
-\label{Bias_LoGain}
 \end{figure}