\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=0.49\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.}
\label{TimeRes_SlidW}
\end{figure}

\begin{figure}[htp]
\centering
  \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}



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