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diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.nav b/Kstmumu/Face2Face_meeting/Comparison/Comparison.nav
index 4ff133c..995e372 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.nav
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.nav
@@ -8,132 +8,28 @@
 \headcommand {\sectionentry {1}{Introduction}{4}{Introduction}{0}}
 \headcommand {\beamer@sectionpages {1}{3}}
 \headcommand {\beamer@subsectionpages {1}{3}}
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.out b/Kstmumu/Face2Face_meeting/Comparison/Comparison.out
index 9b0da9b..e8ad7e5 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.out
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.out
@@ -1,5 +1 @@
 \BOOKMARK [2][]{Outline0.1}{Introduction}{}
-\BOOKMARK [2][]{Outline0.2}{Method of Moments - Theory}{}
-\BOOKMARK [2][]{Outline0.3}{Moments of Ss}{}
-\BOOKMARK [2][]{Outline0.4}{Toy MC study}{}
-\BOOKMARK [2][]{Outline0.5}{S-wave}{}
diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.pdf b/Kstmumu/Face2Face_meeting/Comparison/Comparison.pdf
index cb262eb..3eab7ae 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.pdf
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.pdf
Binary files differ
diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.synctex.gz b/Kstmumu/Face2Face_meeting/Comparison/Comparison.synctex.gz
index 753bb0a..014b11e 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.synctex.gz
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.synctex.gz
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.tex b/Kstmumu/Face2Face_meeting/Comparison/Comparison.tex
index 8183995..f220aa0 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.tex
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.tex
@@ -10,6 +10,8 @@
 \newcommand\abs[1]{\left|#1\right|}
 \usepackage{hepnicenames}
 \usepackage{hepunits}
+\usepackage{color}
+
 
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5
@@ -44,1029 +46,436 @@
 
 
 \section{Introduction}
-\begin{frame}\frametitle{Introduction}
-Why method of moments:
-\begin{enumerate}
-\item Complementary approach to LL fits.
-\item Allows to extract info measuring quantities in event basis depending on the angular distribution.
-\item Used in $\PB \to \rho \Plepton \nu$(SLAC-386 UC-414),\\ $\PJpsi \to \PK \PK \gamma$(PRD 71, 032005 (2005) ), etc.
-\end{enumerate}
-
-
-\end{frame}
-\section{Method of Moments - Theory}
-\begin{frame}\frametitle{Method of moments}
-{~}
-Let's assume we have our pdf with $k$ unknown parameters:~$PDF(x_i, \alpha)$, $dim(\alpha)=k$. One can calculate $k$ moments, which are the functions of $\alpha_i$:
-\begin{equation}
-\mu_i=f(\alpha_1,..., \alpha_k) = E[W_i]
-\end{equation}
-For $n$ events, we can estimate:
-\begin{equation}
-\widehat{\mu}_i=\dfrac{1}{n}\sum_{j=0}^{j=n-1} w_j
-\end{equation}
-, where $w_j=g(x_i)$
-
-\end{frame}
-
-\begin{frame}\frametitle{Trivial example}
-{~}
-Lets see how this works in practice:
-\begin{equation}
-f(x)=\dfrac{x^{a-1}e^{-x/b}} {b^a \Gamma(a)}
-\end{equation}
-we measure the moments:\\
-\begin{center} $m_1=\dfrac{X_1+X_2+...+X_n}{n}$,\\ $m_2=\dfrac{X_1^2+X_2^2+...+X_n^2}{n}$.\\\end{center}
-and calculate them analytically:
-\begin{center} $m_1=ab$, $m_2=b^2a(a+1)$\end{center}
-So one just needs to solve this and get the answer:
-\center $a=\dfrac{m_1^2}{m_2-m_1^2}$, $b=\dfrac{m_2-m_1^2}{m_1}$
-\end{frame}
-
-\section{Moments of Ss}
-
-
-\begin{frame}\frametitle{Our PDF}
-{~}
-The angular terms:
-\begin{small}
-\begin{multline}
-PDF(\cos \theta_k ,\cos \theta_l, \phi) =\dfrac{9}{32\pi}( \dfrac{3}{4}(1-F_l)\sin^2 \theta_k + F_l \cos^2 \theta_k + (\dfrac{1}{4}(1-F_l)\sin^2 \theta_k \\ -F_l\cos^2) \cos 2\theta_l  + S_3 \sin^2 \theta_k \sin^2 \theta_l cos2\phi + S_4 \sin2 \theta_k \sin \theta_l \cos\phi +\\ S_5 \sin 2 \theta_k \sin \theta_l \cos \phi +  (S_{6s} \sin^2 \theta_k + S_{6c} \cos^2 \theta_k) \cos \theta_l + \\ S_7 \sin  2\theta_k \sin \theta_l \sin \phi +  S_8 \sin 2 \theta_k \sin 2 \theta_l \sin \phi + S_9 \sin^2 \theta_k  \sin^2 \theta_l \sin 2 \phi)
-\end{multline}
-\end{small}
-\only<1>{
-Since we are fitting a PDF we need to ensure it is normalized:
-\begin{equation}
-\int_{-\pi}^{\pi} d\phi \int_{-1}^{1} d cos\theta_l \int_{-1}^{1} d cos\theta_k \dfrac{d^4\Gamma}{dq^2 dcos\theta_k dcos\theta_l d\phi}=1
-\end{equation}
-}
-\only<2>
-{
-\begin{small}
-For further use let's introduce a notation:
-\begin{multline}
-PDF(\cos \theta_k ,\cos \theta_l, \phi) =\dfrac{9}{32\pi}( \dfrac{3}{4}(1-F_l)\sin^2 \theta_k + F_l \cos^2 \theta_k + \\(\dfrac{1}{4}(1-F_l)\sin^2 \theta_k -F_l\cos^2) \cos 2\theta_l  + \sum_{x=3}^{9} S_x f_x(\cos \theta_k ,\cos \theta_l, \phi)
-\end{multline}
-\end{small}
-}
-
-\end{frame}
-
-\begin{frame}\frametitle{Moments for $\PB \to \PKstar \mu \mu$ 1/2}
-{~}
-\begin{footnotesize}
-
-
-
-Let's calculate the moments(means of the given distribution):
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) \sin^2 \theta_k =\frac{2}{5} (2-F_l)
-\end{equation}
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) \cos^2 \theta_k =\frac{1}{5} (2F_l+1)
-\end{equation}
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) \cos^2 \theta_k =-\dfrac{2}{25}(2 + F_l)
-\end{equation}
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) \sin^2 \theta_k =-\dfrac{1}{25}(1+8F_l)
-\end{equation}
-\end{footnotesize}
-
-\end{frame}
-
-
-\begin{frame}\frametitle{Moments for $\PB \to \PKstar \mu \mu$ 2/2}
-{~}
-
-
-\begin{small}
-
-Let's calculate the moments(means of the given distribution):
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) f_{S_x}= \frac{8}{25}S_x,
-\end{equation}
-for $x=3,4,8,9$, and:
-
-%%
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF(\cos \theta_k ,\cos \theta_l, \phi) f_{S_x}= \frac{2}{5}S_x,
-\end{equation}
-for $x=5,6,7$.\\
-New physics apparently as we like orthogonal world:
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi~( f_{S_x} \times f_{S_y})		= \alpha_{xy} \delta_{x~y}
-\end{equation}
-
-\end{small}
-\end{frame}
-
-
-
-\begin{frame}\frametitle{Moments for $\PB \to \PKstar \mu \mu$}
-{~}
-\begin{itemize}
-\item We are abusing the fact that the basis is orthogonal and moments do not mix.
-\item Makes live easier and reduces the systematics.
-\item Each of the S does not know about other.
-\item In case of full PDF, $S_{1s}$, $S_{2s}$, $S_{1c}$, $S_{2c}$ $S_{6s}$, $S_{6c}$ are not orthogonal.
-\item Still we can get them solving equation system:
-\end{itemize}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi} sin^2 \theta_k cos \theta_l = 0.1(S_6c+4S_6s)
-\end{equation}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi} cos \theta_l = 0.25(S_{6}c+2S_{6s})
-\end{equation}
-
-\small solution: $S_{6c}=2 (4 M_{S_{6c}} - 5 M_{S_{6s}})$, $S_{6s}= -2 M_{S_{6c}} + 5 M_{S_{6s}}$
-
-
-
-\end{frame}
-
-
-
-\section{Toy MC study}
-
-\begin{frame}\frametitle{Moments for $\PB \to \PKstar \mu \mu$}
-{~}
-Lets see if this method actually works. Let's take some random parameters for the PDF and make a toy.
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.25]{images/J3.png}
-
-\column{2.5in}
-\includegraphics[scale=0.25]{images/J9.png}
-
-
-\end{columns}
-
-\end{frame}
-
-
-
-
-
-\begin{frame}\frametitle{Error Estimation}
-{~}
-\begin{itemize}
-\item Since moment is the mean of a given distribution the error can be estimated as $mean/RMS$
-\item use TOY MC to check this assumption
-\item Do not worry, detail description an numbers will come in other presentation.
-\end{itemize}
-
-\includegraphics[scale=0.3]{plots/conw.png}\\
-
-
-\end{frame}
-%%%%%%%%%%%%%%%%%%%%%%%%5
-\begin{frame}\frametitle{Correlation check}
-{~}
-\begin{itemize}
-\item In theory $S_i$ shouldn't be correlated to $S_j$ in the moment calculation.
-\item Lets put this to a test.
-\end{itemize}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J9J4.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J8J5.png}\\
-
-
-\end{columns}
-
-
-\end{frame}
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%5
-\begin{frame}\frametitle{Correlation check 2}
-{~}
-\begin{itemize}
-\item Let's now FIX $J_x$ and simulate different $J_y$
-\item Again theory would suggest that one J shouldn't know about the other, so $J_x$ shouldn't change with scanning $J_y$ parameter
-\end{itemize}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.24]{plots/J5_vs_J9_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.24]{plots/J3_vs_J9_300.png}\\
-
-
-\end{columns}
-
-
-\end{frame}
-
-
-
-\section{S-wave}
-
-
-
-\begin{frame}\frametitle{S-wave pollution}
-{~}
+\begin{frame}\frametitle{How to use Moments}
 \begin{columns}
 \column{3in}
+\begin{enumerate}
+\item Method of moments still uses fits.
+\item Extended likelihood fit is used to extract number of signal and background events.
+\item Calculate raw moments in bck window$~masss>5350$ and signal window$~mass\in[5230,5330]$
+\only<1>{\item Use a simple weighted average:}
+\only<2>{\item Extract signal moments:}
+\end{enumerate}
+
+\column{2.2in}
+\includegraphics[width=0.9\textwidth]{mass3.png}
+
+\end{columns}
+{~}\\
+\only<1>{
+\begin{equation}
+M_{mix}= \dfrac{n_{sig} M_{sig}+n_{bkg}M_{bkg}}{n_{sig}+n_{bkg}}
+\end{equation}
+}
+\only<2>{
+\begin{equation}
+M_{sig}=\dfrac{ (n_{sig}+n_{bkg}) M_{mix}}{n_{sig}} - \dfrac{n_{bkg} m_{bkg}}{n_{sig}}
+\end{equation}
+}
+
+\end{frame}
+
+\begin{frame}\frametitle{How to use fits 1/2}
+\begin{columns}
+\column{3.0in}
 \begin{itemize}
-\item Unfortunately in our perfect orthogonal world lives an imposter.
-\item This imposter is $\PBzero \to (\PK \Ppi)_{S-wave}~\mu \mu$
-\item This "ghost" dilutes our NP! Like dark matter the universe.
-\item We need something to bust this ghost away
+\item Assuming we can decouple in the PDF the angular and mass part:
+$PDF(\theta_l, \theta_k, \phi, m)= PDF_1(\theta_l, \theta_k, \phi) \times PDF_2(m)$
+
+\item $PDF_1$ is our PDF defined in previous presentation.
+\item $PDF_2$ is double CB as defined in Christoph toy creation. 
+\item For background we assume 2nd order Chebyshev polynomials($PDF_{1,bck}$)
+\item And single exponential for bkg part($PDF_{2,bck}$)
 \end{itemize}
 
-\column{2in}
-\includegraphics[width=0.95\textwidth]{P5.png}\\
-
-\includegraphics[width=0.5\textwidth]{gb.jpg}
+\column{2.2in}
+\includegraphics[width=0.6\textwidth]{cosk_tmp.png}\\
+\includegraphics[width=0.6\textwidth]{cosl_tmp.png}
 \end{columns}
 
-
 \end{frame}
 
-
-
-
-
-%%%%%%%%%%%%%%%%%%%5
-\begin{frame}\frametitle{S-wave hunting}
-{~}
-Our PDF with the S-wave will look as follows:
-\begin{multline}
-PDF_{full}(\cos \theta_k ,\cos \theta_l, \phi) =\dfrac{9}{32\pi}(  \textcolor{red}{(1-F_s)}(\dfrac{3}{4}(1-F_l)\sin^2 \theta_k + F_l \cos^2 \theta_k + \\ (\dfrac{1}{4}(1-F_l)\sin^2 \theta_k  -F_l\cos^2) \cos 2\theta_l  + S_3 \sin^2 \theta_k \sin^2 \theta_l cos2\phi + \\S_4 \sin2 \theta_k \sin \theta_l \cos\phi + S_5 \sin 2 \theta_k \sin \theta_l \cos \phi +  \\ (S_{6s} \sin^2 \theta_k + S_{6c} \cos^2 \theta_k) \cos \theta_l +  S_7 \sin  2\theta_k \sin \theta_l \sin \phi + \\ S_8 \sin 2 \theta_k \sin 2 \theta_l \sin \phi + S_9 \sin^2 \theta_k  \sin^2 \theta_l \sin 2 \phi) + \\
-\textcolor{red}{\dfrac{2}{3} F_s \sin^2 \theta_l + \frac{4}{3} A_s \sin^2 \theta_l \cos \theta_k + I_4 \sin \theta_k \sin 2 \theta_l \cos \phi} \\ \textcolor{red}{+ I_5 \sin \theta_k \sin \theta_l \cos \phi + I_7 \sin \theta_k \sin \theta_l + \sin \phi + I_8 \sin \theta_k \sin 2\theta_l \sin\phi})
-\end{multline}
-
-\small In this form we ensure normalization.
-\end{frame}
-
-\begin{frame}\frametitle{How does the dilution work? 1/2}
-{~}
-\begin{small}
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF_{full}(\cos \theta_k ,\cos \theta_l, \phi) f_{S_x}= \frac{8}{25}S_x\textcolor{red}{(1-F_s)},
-\end{equation}
-for $x=3,4,8,9$, and:
-
-%%
-\begin{equation}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF_{full}(\cos \theta_k ,\cos \theta_l, \phi) f_{S_x}= \frac{2}{5}S_x\textcolor{red}{(1-F_s)},
-\end{equation}
-for $x=5,6,7$.\\
-Not much harm and easy to control.
-\end{small}
-
-\end{frame}
-
-\begin{frame}\frametitle{How does the dilution work? 2/2}
-{~}
-\begin{small}
-Unfortunately $F_l$ and $F_s$ will mix with each other:
-\begin{multline}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF_{full}(\cos \theta_k ,\cos \theta_l, \phi) \sin^2 \theta_k= \\ \frac{2}{15} (6 + 3 F_l (F_s-1) - F_s)=M_{F_l}
-\end{multline}
-\begin{multline}
-\int_{-1}^{1}d\cos \theta_l \int_{-1}^{1}d\cos \theta_k \int_{-\pi}^{\pi}d\phi PDF_{full}(\cos \theta_k ,\cos \theta_l, \phi) \sin^2 \theta_l= \\ \frac{1}{5} (3 + F_l + F_s - F_l F_s)=M_{F_s}
-\end{multline}
-
-They can solve this system:
-
-$ \begin{cases} F_s = \frac{15}{4} (M_{F_l} + 2 M_{F_s}) \\ F_l = \frac{(15 M_{F_l} + 10 M_{F_s}-18)}{(15 M_{F_l} + 30 M_{F_s}-34)}  \end{cases}$
-
-
-\end{small}
-
-\end{frame}
-
-
-\begin{frame}\frametitle{S-wave moments}
-{~}
-We can even measure directly the S-wave:
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi }sin^2 \theta_l cos \theta_k = \dfrac{32 I_{1b} }{45}
-\end{equation}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi } sin \theta_k sin 2 \theta_l cos \phi = \dfrac{16 I_4 }{45}
-\end{equation}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi } sin\theta_k sin\theta_l cos\phi = \dfrac{4 I_5 }{9}
-\end{equation}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi} sin  \theta_k sin 2 \theta_l sin \phi = \dfrac{4 I_7 }{9}
-\end{equation}
-\begin{equation}
- \dfrac{d^3\Gamma}{\Gamma dcos\theta_k dcos\theta_l d\phi} sin  \theta_k sin2 \theta_l sin \phi = \dfrac{16 S_8 }{45}
-\end{equation}
-
-
-
-\end{frame}
-
-
-\begin{frame}\frametitle{Conclusions}
-{~}
+\begin{frame}\frametitle{How to use fits 2/2}
+\begin{columns}
+\column{3.2in}
+What is left free in the fit:
 \begin{itemize}
-\item Method of moments very suitable for $\PBzero \to \PKstar \mu \mu$.
-\item The method converge fast and works for the "simple case", i.e. signal only.
-\item Method very insensitive to S-wave component, thanks to orthogonality. 
-\item Complementary one can measure in-depended S-wave component.
-\item No problem with boundary problems.
+\item $\lambda$ for exponent.
+\item $F_l$, $S_x$ for angular distribution.
+\item Relative normalization of signal and bkg.
+\end{itemize}
+Other remarks:
+\begin{enumerate}
+\item I am using good old Roofit, not custom developed fitter.
+\item No s-wave in the fits, or systematics include in this study.
+\item individual toys are now provided by Christoph, so one can compare $1:1$.
+\end{enumerate}
+\column{2.2in}
+\includegraphics[width=0.6\textwidth]{phi_tmp.png}\\
+\includegraphics[width=0.6\textwidth]{mass.png}
+\end{columns}
+
+\end{frame}
+
+
+\begin{frame}\frametitle{Small things}
+General remark:
+\begin{itemize}
+\item All pull plots/fits are available: \href{http://nz17-p1.ifj.edu.pl/work_public/LHCb/Kst_mumu/Face2Face_meeting/}{LINK}
+\item User: lhcb, password: $2924$.
+
 
 \end{itemize}
-What comes in the next talks(stay tuned):
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{MM results $1GeV$ binning, Mean bias}
+
+
+ \tiny{  
+    \begin{tabular}{|*{10}{c|}}
+	
+ \hline
+$Q^2$ & \scalebox{0.5}{$F_l$} & \scalebox{0.5}{$S_3$} & \scalebox{0.5}{$S_4$} & \scalebox{0.5}{$S_5$} & \scalebox{0.5}{$S_6$} \\ \hline                                                                      
+0 & \scalebox{0.5}{\textcolor{blue}{$-0.431 \pm 0.0184(-23.4)$}} & \scalebox{0.5}{$0.00218 \pm 0.0186(0.118)$} & \scalebox{0.5}{$0.0389 \pm 0.0183(2.13)$} & \scalebox{0.5}{$0.0104 \pm 0.0183(0.564)$} & \scalebox{0.5}{$0.0357 \pm 0.0183(1.96)$}           \\ \hline 
+1 & \scalebox{0.5}{$-0.029 \pm 0.0188(-1.56)$} & \scalebox{0.5}{$0.0247 \pm 0.0187(1.32)$} & \scalebox{0.5}{$0.016 \pm 0.0184(0.872)$} & \scalebox{0.5}{$-0.0125 \pm 0.0191(-0.657)$} & \scalebox{0.5}{$-0.00833 \pm 0.0186(-0.449)$}       \\ \hline 
+2 & \scalebox{0.5}{$0.0090 \pm 0.0181(0.501)$} & \scalebox{0.5}{$-0.0226 \pm 0.0186(-1.21)$} & \scalebox{0.5}{$-0.00623 \pm 0.018(-0.347)$} & \scalebox{0.5}{$-0.0235 \pm 0.018(-1.3)$} & \scalebox{0.5}{$-0.0201 \pm 0.0183(-1.1)$}        \\ \hline 
+3 & \scalebox{0.5}{$-0.046 \pm 0.0183(-2.56)$} & \scalebox{0.5}{$-0.00942 \pm 0.0183(-0.515)$} & \scalebox{0.5}{$-0.00109 \pm 0.0188(-0.0579)$} & \scalebox{0.5}{$0.0108 \pm 0.0188(0.577)$} & \scalebox{0.5}{$-0.0519 \pm 0.0184(-2.83)$}  \\ \hline 
+4 & \scalebox{0.5}{$-0.031 \pm 0.0183(-1.71)$} & \scalebox{0.5}{$0.0268 \pm 0.0181(1.48)$} & \scalebox{0.5}{$-0.00687 \pm 0.0182(-0.378)$} & \scalebox{0.5}{$-0.00106 \pm 0.0187(-0.0568)$} & \scalebox{0.5}{$0.00908 \pm 0.0189(0.481)$}   \\ \hline 
+5 & \scalebox{0.5}{$-0.034 \pm 0.0178(-1.96)$} & \scalebox{0.5}{$0.0231 \pm 0.0189(1.22)$} & \scalebox{0.5}{$-0.0169 \pm 0.0183(-0.92)$} & \scalebox{0.5}{$-0.0138 \pm 0.0183(-0.75)$} & \scalebox{0.5}{$9.56e-05 \pm 0.0184(0.00521)$}    \\ \hline 
+6 & \scalebox{0.5}{$-0.031 \pm 0.0186(-1.69)$} & \scalebox{0.5}{$0.0184 \pm 0.0183(1)$} & \scalebox{0.5}{$-0.000709 \pm 0.0182(-0.039)$} & \scalebox{0.5}{$-0.00728 \pm 0.0189(-0.386)$} & \scalebox{0.5}{$0.0223 \pm 0.0182(1.22)$}       \\ \hline 
+7 & \scalebox{0.5}{$0.0042 \pm 0.0188(0.22)$} & \scalebox{0.5}{$0.022 \pm 0.0181(1.22)$} & \scalebox{0.5}{$-0.00412 \pm 0.0188(-0.22)$} & \scalebox{0.5}{$0.0044 \pm 0.0187(0.236)$} & \scalebox{0.5}{$0.0291 \pm 0.0188(1.55)$}           \\ \hline 
+8 & \scalebox{0.5}{$0.0061 \pm 0.018(0.34)$} & \scalebox{0.5}{$0.0118 \pm 0.0184(0.643)$} & \scalebox{0.5}{$-0.0169 \pm 0.0185(-0.915)$} & \scalebox{0.5}{$0.0244 \pm 0.0182(1.34)$} & \scalebox{0.5}{$0.00532 \pm 0.0188(0.283)$}         \\ \hline 
+9 & \scalebox{0.5}{$0.0056 \pm 0.0184(0.30)$} & \scalebox{0.5}{$-0.00938 \pm 0.0182(-0.514)$} & \scalebox{0.5}{$-0.0405 \pm 0.0182(-2.22)$} & \scalebox{0.5}{$0.00885 \pm 0.0182(0.487)$} & \scalebox{0.5}{$0.0361 \pm 0.0185(1.96)$}      \\ \hline 
+10 & \scalebox{0.5}{$-0.0156 \pm 0.0185(-0.84)$} & \scalebox{0.5}{$-0.00611 \pm 0.018(-0.34)$} & \scalebox{0.5}{$-0.0241 \pm 0.0184(-1.31)$} & \scalebox{0.5}{$0.0204 \pm 0.0186(1.09)$} & \scalebox{0.5}{$-0.00378 \pm 0.0189(-0.201)$}   \\ \hline 
+11 & \scalebox{0.5}{$-0.0079 \pm 0.018(-0.44)$} & \scalebox{0.5}{$0.0539 \pm 0.0182(2.96)$} & \scalebox{0.5}{$-0.0063 \pm 0.0189(-0.334)$} & \scalebox{0.5}{$-0.0297 \pm 0.019(-1.57)$} & \scalebox{0.5}{$-0.00305 \pm 0.0183(-0.166)$}    \\ \hline 
+
+    \end{tabular}
+   
+ \begin{tabular}{|*{10}{c|}}                                                                                                                                                                                                                                                                                                                                                                                                                           
+ \hline
+$Q^2$ &  \scalebox{0.5}{$S_7$} & \scalebox{0.5}{$S_8$} & \scalebox{0.5}{$S_9$} \\ \hline        
+0 & \scalebox{0.5}{$-0.0179 \pm 0.018(-0.997)$} & \scalebox{0.5}{$-0.0311 \pm 0.0187(-1.66)$} & \scalebox{0.5}{$0.0274 \pm 0.0184(1.49)$} \\ \hline           
+1 & \scalebox{0.5}{$-0.0221 \pm 0.0183(-1.21)$} & \scalebox{0.5}{$-0.0592 \pm 0.0185(-3.2)$} & \scalebox{0.5}{$0.0151 \pm 0.0181(0.836)$} \\ \hline           
+2 & \scalebox{0.5}{$-0.00449 \pm 0.0185(-0.243)$} & \scalebox{0.5}{$-0.00996 \pm 0.0188(-0.529)$} & \scalebox{0.5}{$0.00609 \pm 0.0186(0.328)$} \\ \hline     
+3 & \scalebox{0.5}{$0.0274 \pm 0.0177(1.55)$} & \scalebox{0.5}{$-0.00217 \pm 0.0186(-0.117)$} & \scalebox{0.5}{$-0.00915 \pm 0.0187(-0.49)$} \\ \hline        
+4 & \scalebox{0.5}{$0.0156 \pm 0.0181(0.861)$} & \scalebox{0.5}{$-0.0141 \pm 0.0186(-0.759)$} & \scalebox{0.5}{$0.00498 \pm 0.0178(0.279)$} \\ \hline         
+5& \scalebox{0.5}{$0.0158 \pm 0.0186(0.848)$} & \scalebox{0.5}{$0.00727 \pm 0.0191(0.381)$} & \scalebox{0.5}{$0.029 \pm 0.0185(1.57)$} \\ \hline              
+6& \scalebox{0.5}{$-0.00232 \pm 0.0186(-0.125)$} & \scalebox{0.5}{$0.00974 \pm 0.0177(0.551)$} & \scalebox{0.5}{$-0.00613 \pm 0.018(-0.341)$}\\ \hline        
+7& \scalebox{0.5}{$-0.00853 \pm 0.0184(-0.463)$} & \scalebox{0.5}{$-0.00649 \pm 0.0182(-0.356)$} & \scalebox{0.5}{$0.00402 \pm 0.0183(0.22)$} \\ \hline       
+8& \scalebox{0.5}{$-0.0137 \pm 0.0185(-0.739)$} & \scalebox{0.5}{$-0.0167 \pm 0.0185(-0.903)$} & \scalebox{0.5}{$-0.0278 \pm 0.0183(-1.52)$} \\ \hline        
+9& \scalebox{0.5}{$-0.0229 \pm 0.019(-1.2)$} & \scalebox{0.5}{$-0.0506 \pm 0.0183(-2.77)$} & \scalebox{0.5}{$-0.0269 \pm 0.0183(-1.46)$} \\ \hline            
+10& \scalebox{0.5}{$-0.0155 \pm 0.0185(-0.84)$} & \scalebox{0.5}{$0.0276 \pm 0.0184(1.5)$} & \scalebox{0.5}{$0.0137 \pm 0.0185(0.742)$} \\ \hline              
+11& \scalebox{0.5}{$-0.0503 \pm 0.0183(-2.75)$} & \scalebox{0.5}{$-0.0137 \pm 0.0181(-0.758)$} & \scalebox{0.5}{$0.0169 \pm 0.0187(0.902)$} \\ \hline          
+
+    \end{tabular}
+    }
+
+\end{frame}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                                                                                                                                                                                                                                                                                                                                                                                                  
+\begin{frame}\frametitle{MM results $1GeV$ binning, Sigma bias}                                                                                                                                                                                                                                                                                                                                                                                             
+                                                                                                                                                                                                                                                                                                                                                                                                                                                           
+                                                                                                                                                                                                                                                                                                                                                                                                                                                           
+ \tiny{                                                                                                                                                                                                                                                                                                                                                                                                                                                    
+    \begin{tabular}{|*{10}{c|}}    
+           \hline                                                                                                                                                                                                                                                                                                                                                                                                                                                                    
+$Q^2$ & \scalebox{0.5}{$F_l$} & \scalebox{0.5}{$S_3$} & \scalebox{0.5}{$S_4$} & \scalebox{0.5}{$S_5$} & \scalebox{0.5}{$S_6$} \\ \hline   
+0 & \scalebox{0.5}{$0.969 \pm 0.014(2.24)$} & \scalebox{0.5}{$0.979 \pm 0.0142(1.45)$} & \scalebox{0.5}{$0.958 \pm 0.0136(3.11)$} & \scalebox{0.5}{$0.969 \pm 0.0139(2.21)$} & \scalebox{0.5}{$0.975 \pm 0.014(1.8)$} \\ \hline  
+1 & \scalebox{0.5}{$0.998 \pm 0.0154(0.128)$} & \scalebox{0.5}{$0.99 \pm 0.0141(0.684)$} & \scalebox{0.5}{$0.982 \pm 0.014(1.31)$} & \scalebox{0.5}{$1 \pm 0.0142(-0.327)$} & \scalebox{0.5}{$0.988 \pm 0.0152(0.812)$} \\ \hline  
+2 & \scalebox{0.5}{$0.957 \pm 0.0134(3.23)$} & \scalebox{0.5}{$0.989 \pm 0.0142(0.807)$} & \scalebox{0.5}{$0.96 \pm 0.0142(2.79)$} & \scalebox{0.5}{$0.965 \pm 0.0135(2.6)$} & \scalebox{0.5}{$0.973 \pm 0.0143(1.9)$} \\ \hline  
+3 & \scalebox{0.5}{$0.971 \pm 0.0139(2.11)$} & \scalebox{0.5}{$0.971 \pm 0.0137(2.1)$} & \scalebox{0.5}{$0.996 \pm 0.0152(0.277)$} & \scalebox{0.5}{$0.995 \pm 0.0142(0.374)$} & \scalebox{0.5}{$0.967 \pm 0.014(2.39)$} \\ \hline  
+4 & \scalebox{0.5}{$0.971 \pm 0.014(2.09)$} & \scalebox{0.5}{$0.965 \pm 0.0138(2.51)$} & \scalebox{0.5}{$0.966 \pm 0.0137(2.46)$} & \scalebox{0.5}{$0.994 \pm 0.0139(0.44)$} & \scalebox{0.5}{$1 \pm 0.0142(0.00431)$} \\ \hline  
+5 & \scalebox{0.5}{$0.947 \pm 0.0136(3.88)$} & \scalebox{0.5}{$1 \pm 0.0138(-0.165)$} & \scalebox{0.5}{$0.967 \pm 0.0138(2.4)$} & \scalebox{0.5}{$0.978 \pm 0.0137(1.63)$} & \scalebox{0.5}{$0.981 \pm 0.0132(1.46)$} \\ \hline  
+6 & \scalebox{0.5}{$0.983 \pm 0.0142(1.19)$} & \scalebox{0.5}{$0.981 \pm 0.0139(1.35)$} & \scalebox{0.5}{$0.967 \pm 0.0134(2.46)$} & \scalebox{0.5}{$1 \pm 0.0145(-0.126)$} & \scalebox{0.5}{$0.969 \pm 0.0134(2.29)$} \\ \hline  
+7 & \scalebox{0.5}{$1 \pm 0.0144(-0.01)$} & \scalebox{0.5}{$0.968 \pm 0.0142(2.26)$} & \scalebox{0.5}{$0.993 \pm 0.0143(0.474)$} & \scalebox{0.5}{$0.989 \pm 0.0136(0.775)$} & \scalebox{0.5}{$0.991 \pm 0.0138(0.671)$} \\ \hline  
+8 & \scalebox{0.5}{$0.956 \pm 0.0133(3.33)$} & \scalebox{0.5}{$0.98 \pm 0.0138(1.43)$} & \scalebox{0.5}{$0.983 \pm 0.0145(1.18)$} & \scalebox{0.5}{$0.966 \pm 0.0136(2.46)$} & \scalebox{0.5}{$0.996 \pm 0.0145(0.309)$}  \\ \hline  
+9 & \scalebox{0.5}{$0.959 \pm 0.013(3.14)$} & \scalebox{0.5}{$0.968 \pm 0.0145(2.21)$} & \scalebox{0.5}{$0.954 \pm 0.0128(3.64)$} & \scalebox{0.5}{$0.963 \pm 0.013(2.8)$} & \scalebox{0.5}{$0.985 \pm 0.0142(1.03)$} \\ \hline  
+10 & \scalebox{0.5}{$0.972 \pm 0.0131(2.11)$} & \scalebox{0.5}{$0.955 \pm 0.0131(3.46)$} & \scalebox{0.5}{$0.978 \pm 0.0141(1.59)$} & \scalebox{0.5}{$0.991 \pm 0.014(0.635)$} & \scalebox{0.5}{$1.01 \pm 0.0137(-0.502)$} \\ \hline  
+11 & \scalebox{0.5}{$0.952 \pm 0.014(3.43)$} & \scalebox{0.5}{$0.969 \pm 0.0141(2.22)$} & \scalebox{0.5}{$0.999 \pm 0.0146(0.0445)$} & \scalebox{0.5}{$1 \pm 0.0144(-0.22)$} & \scalebox{0.5}{$0.979 \pm 0.0143(1.45)$}   \\ \hline  
+
+      
+      
+   \end{tabular}                                                                                                                                                                                                                                                                                                                                                                                                                                          
+  \begin{columns}
+  \column{2in}
+\begin{tabular}{|c|c|c|c|}                                                                                                                                                                                                                                                                                                                                                                                                                               
+ \hline                                                                                                                                                                                                                                                                                                                                                                                                                                                    
+$Q^2$ & \scalebox{0.5}{$S_7$} & \scalebox{0.5}{$S_8$} & \scalebox{0.5}{$S_9$} \\ \hline             
+
+0 & \scalebox{0.5}{$0.958 \pm 0.0139(2.98)$} & \scalebox{0.5}{$0.994 \pm 0.0151(0.42)$} & \scalebox{0.5}{$0.972 \pm 0.0145(1.91)$} \\ \hline  
+1 & \scalebox{0.5}{$0.969 \pm 0.0138(2.24)$} & \scalebox{0.5}{$0.98 \pm 0.0145(1.4)$} & \scalebox{0.5}{$0.963 \pm 0.0137(2.74)$} \\ \hline  
+2 & \scalebox{0.5}{$0.983 \pm 0.0145(1.17)$} & \scalebox{0.5}{$0.998 \pm 0.0146(0.147)$} & \scalebox{0.5}{$0.986 \pm 0.0143(0.98)$} \\ \hline   
+3 & \scalebox{0.5}{$0.942 \pm 0.013(4.43)$} & \scalebox{0.5}{$0.987 \pm 0.0132(0.957)$} & \scalebox{0.5}{$0.996 \pm 0.0145(0.295)$} \\ \hline  
+4 & \scalebox{0.5}{$0.965 \pm 0.0137(2.58)$} & \scalebox{0.5}{$0.986 \pm 0.0138(1)$} & \scalebox{0.5}{$0.965 \pm 0.0131(2.24)$} \\ \hline       
+5 & \scalebox{0.5}{$0.979 \pm 0.0135(1.55)$} & \scalebox{0.5}{$0.978 \pm 0.0149(1.46)$} & \scalebox{0.5}{$0.981 \pm 0.0143(1.33)$} \\ \hline  
+6 & \scalebox{0.5}{$0.983 \pm 0.0139(1.22)$} & \scalebox{0.5}{$0.942 \pm 0.013(4.48)$} & \scalebox{0.5}{$0.955 \pm 0.0136(3.33)$} \\ \hline  
+7 & \scalebox{0.5}{$0.979 \pm 0.0129(1.63)$} & \scalebox{0.5}{$0.97 \pm 0.0145(2.06)$} & \scalebox{0.5}{$0.972 \pm 0.0135(2.05)$} \\ \hline   
+8 & \scalebox{0.5}{$0.979 \pm 0.014(1.5)$} & \scalebox{0.5}{$0.985 \pm 0.0139(1.08)$} & \scalebox{0.5}{$0.971 \pm 0.0136(2.13)$} \\ \hline     
+9 & \scalebox{0.5}{$0.995 \pm 0.0139(0.368)$} & \scalebox{0.5}{$0.975 \pm 0.0142(1.73)$} & \scalebox{0.5}{$0.975 \pm 0.0137(1.82)$} \\ \hline  
+10 & \scalebox{0.5}{$0.988 \pm 0.0132(0.907)$} & \scalebox{0.5}{$0.977 \pm 0.0142(1.59)$} & \scalebox{0.5}{$0.978 \pm 0.0142(1.56)$} \\ \hline  
+11 & \scalebox{0.5}{$0.971 \pm 0.0149(1.97)$} & \scalebox{0.5}{$0.968 \pm 0.0142(2.25)$} & \scalebox{0.5}{$0.988 \pm 0.0137(0.886)$}  \\ \hline           
+ \end{tabular} 
+  \column{2in}
+Conclusions:
 \begin{itemize}
-\item This method reduces the error on unfolding.
-\item No problem with convergence.
-\item Systematics easy accessible.
+\item MM does not bias the mean!
+\item There is a trend that it overestimates the errors.
+\item From all possible things that could go wrong this is the best. 
 \end{itemize}
-
-
-\end{frame}
-%%%%%%%%%%%%%%%%%%%%%%%%%55
-\begin{frame}\frametitle{~}
-{~}
-\center \Huge BACKUPS
-
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_75E.png}
-
-
 \end{columns}
-\end{frame}
+  }                                                                                                                                                                                                                                                                                                                                                                                                                                                      
+                                                                                                                                                                                                                                                                                                                                                                                                                                                           
+\end{frame}               
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%                                                                                                                                                                                                                                                                                                                                                                                                  
+\begin{frame}\frametitle{Fit $1GeV$ binning, Mean bias}                                                                                                                                                                                                                                                                                                                                                                                             
+\tiny{                                                                                                                                     
+   \begin{tabular}{|*{10}{c|}}                                                                                                             
+                                                                                                                                           
+\hline                                                                                                                                     
+$Q^2$ & \scalebox{0.6}{$F_l$} & \scalebox{0.6}{$S_3$} & \scalebox{0.6}{$S_4$} & \scalebox{0.6}{$S_5$} & \scalebox{0.6}{$S_6$} \\ \hline     
 
-\begin{frame}
-{~}
+0 & \scalebox{0.6}{$-0.54 \pm 0.02091(-25.82)$} & \scalebox{0.6}{$0.01246 \pm 0.0213(0.585)$} & \scalebox{0.6}{$0.01828 \pm 0.02126(0.8598)$} & \scalebox{0.6}{$0.02513 \pm 0.02078(1.209)$} & \scalebox{0.6}{$0.0646 \pm 0.02081(3.104)$} \\ \hline   
+1 & \scalebox{0.6}{$-0.27 \pm 0.02232(-12.1)$} & \scalebox{0.6}{$0.03261 \pm 0.02401(1.358)$} & \scalebox{0.6}{$0.08175 \pm 0.02376(3.441)$} & \scalebox{0.6}{$-0.1473 \pm 0.0246(-5.987)$} & \scalebox{0.6}{$-0.244 \pm 0.02276(-10.72)$} \\ \hline
+2 & \scalebox{0.6}{$-0.7574 \pm 0.02208(-34.3)$} & \scalebox{0.6}{$-0.0307 \pm 0.02267(-1.354)$} & \scalebox{0.6}{$-0.07512 \pm 0.02344(-3.204)$} & \scalebox{0.6}{$0.03054 \pm 0.02523(1.21)$} & \scalebox{0.6}{$-0.2317 \pm 0.02327(-9.957)$} \\ \hline
+3 & \scalebox{0.6}{$-0.7548 \pm 0.02333(-32.35)$} & \scalebox{0.6}{$-0.01416 \pm 0.02193(-0.6458)$} & \scalebox{0.6}{$-0.1786 \pm 0.02354(-7.588)$} & \scalebox{0.6}{$0.2604 \pm 0.02232(11.67)$} & \scalebox{0.6}{$-0.05868 \pm 0.02325(-2.524)$} \\ \hline 
+4 & \scalebox{0.6}{$-0.5667 \pm 0.02163(-26.2)$} & \scalebox{0.6}{$0.0153 \pm 0.02265(0.6756)$} & \scalebox{0.6}{$-0.2313 \pm 0.02105(-10.99)$} & \scalebox{0.6}{$0.4372 \pm 0.02207(19.81)$} & \scalebox{0.6}{$0.03735 \pm 0.02385(1.566)$} \\ \hline  
+5 & \scalebox{0.6}{$-0.4589 \pm 0.02156(-21.29)$} & \scalebox{0.6}{$0.0305 \pm 0.02265(1.347)$} & \scalebox{0.6}{$-0.2186 \pm 0.02141(-10.21)$} & \scalebox{0.6}{$0.5118 \pm 0.02161(23.69)$} & \scalebox{0.6}{$0.1218 \pm 0.02321(5.249)$} \\ \hline 
+6 & \scalebox{0.6}{$-0.3408 \pm 0.02351(-14.5)$} & \scalebox{0.6}{$-0.005133 \pm 0.0235(-0.2184)$} & \scalebox{0.6}{$-0.3205 \pm 0.02116(-15.15)$} & \scalebox{0.6}{$0.628 \pm 0.02207(28.45)$} & \scalebox{0.6}{$0.2972 \pm 0.02256(13.17)$}\\ \hline
+7 & \scalebox{0.6}{$-0.2309 \pm 0.02362(-9.778)$} & \scalebox{0.6}{$-0.003081 \pm 0.02186(-0.1409)$} & \scalebox{0.6}{$-0.4115 \pm 0.02268(-18.14)$} & \scalebox{0.6}{$0.6794 \pm 0.02274(29.88)$} & \scalebox{0.6}{$0.4305 \pm 0.02204(19.53)$} \\ \hline     
+8 & \scalebox{0.6}{$0.3543 \pm 0.02837(12.49)$} & \scalebox{0.6}{$0.157 \pm 0.02254(6.969)$} & \scalebox{0.6}{$-0.3984 \pm 0.02223(-17.93)$} & \scalebox{0.6}{$0.3877 \pm 0.02171(17.86)$} & \scalebox{0.6}{$0.8208 \pm 0.02474(33.18)$} \\ \hline 
+9 & \scalebox{0.6}{$0.2385 \pm 0.02778(8.586)$} & \scalebox{0.6}{$0.1185 \pm 0.02156(5.499)$} & \scalebox{0.6}{$-0.3564 \pm 0.02171(-16.42)$} & \scalebox{0.6}{$0.3164 \pm 0.02264(13.98)$} & \scalebox{0.6}{$0.7744 \pm 0.02437(31.78)$} \\ \hline 
+10 & \scalebox{0.6}{$0.2395 \pm 0.0273(8.774)$} & \scalebox{0.6}{$0.2025 \pm 0.02106(9.617)$} & \scalebox{0.6}{$-0.3328 \pm 0.02126(-15.66)$} & \scalebox{0.6}{$0.2583 \pm 0.02247(11.5)$} & \scalebox{0.6}{$0.5419 \pm 0.02453(22.09)$} \\ \hline
+11 & \scalebox{0.6}{$0.139 \pm 0.02676(5.194)$} & \scalebox{0.6}{$0.3433 \pm 0.02149(15.98)$} & \scalebox{0.6}{$-0.3043 \pm 0.02151(-14.15)$} & \scalebox{0.6}{$0.1217 \pm 0.02339(5.205)$} & \scalebox{0.6}{$0.3523 \pm 0.02402(14.67)$} \\ \hline
 
+
+\end{tabular}  
+
+ \begin{columns}
+  \column{3in}
+ \begin{tabular}{|*{10}{c|}}                                                                                                                                   
+ \hline                                                                                                                                                        
+$Q^2$ &  \scalebox{0.6}{$S_7$} & \scalebox{0.6}{$S_8$} & \scalebox{0.6}{$S_9$} \\ \hline                                                                       
+0 & \scalebox{0.6}{$-0.03252 \pm 0.02039(-1.595)$} & \scalebox{0.6}{$-0.02852 \pm 0.02148(-1.328)$} & \scalebox{0.6}{$0.03152 \pm 0.0207(1.523)$}  \\ \hline          
+1 & \scalebox{0.6}{$-0.01799 \pm 0.02456(-0.7325)$} & \scalebox{0.6}{$-0.03414 \pm 0.02435(-1.402)$} & \scalebox{0.6}{$0.04347 \pm 0.02277(1.909)$}  \\ \hline        
+2 & \scalebox{0.6}{$-0.1108 \pm 0.02502(-4.429)$} & \scalebox{0.6}{$-0.007344 \pm 0.02559(-0.287)$} & \scalebox{0.6}{$0.04804 \pm 0.02257(2.129)$}  \\ \hline         
+3 & \scalebox{0.6}{$-0.009689 \pm 0.02367(-0.4093)$} & \scalebox{0.6}{$0.03343 \pm 0.0234(1.429)$} & \scalebox{0.6}{$-0.01668 \pm 0.0209(-0.7982)$}  \\ \hline        
+4 & \scalebox{0.6}{$-0.03027 \pm 0.02361(-1.282)$} & \scalebox{0.6}{$0.05424 \pm 0.02354(2.304)$} & \scalebox{0.6}{$-0.02207 \pm 0.02167(-1.018)$}  \\ \hline         
+5 & \scalebox{0.6}{$-0.07159 \pm 0.02324(-3.08)$} & \scalebox{0.6}{$0.02229 \pm 0.02396(0.9304)$} & \scalebox{0.6}{$-0.03396 \pm 0.02147(-1.582)$}  \\ \hline         
+6 & \scalebox{0.6}{$-0.06034 \pm 0.02395(-2.52)$} & \scalebox{0.6}{$0.04234 \pm 0.02284(1.854)$} & \scalebox{0.6}{$-0.01762 \pm 0.02174(-0.8102)$}  \\ \hline         
+7 & \scalebox{0.6}{$-0.05002 \pm 0.02386(-2.097)$} & \scalebox{0.6}{$0.03382 \pm 0.02289(1.477)$} & \scalebox{0.6}{$0.009742 \pm 0.02147(0.4538)$}  \\ \hline         
+8 & \scalebox{0.6}{$-0.05097 \pm 0.0245(-2.08)$} & \scalebox{0.6}{$-0.02328 \pm 0.02359(-0.9872)$} & \scalebox{0.6}{$-0.03285 \pm 0.023(-1.428)$}  \\ \hline          
+9 & \scalebox{0.6}{$-0.03206 \pm 0.02543(-1.261)$} & \scalebox{0.6}{$-0.009805 \pm 0.02334(-0.4201)$} & \scalebox{0.6}{$-0.04927 \pm 0.02272(-2.169)$}  \\ \hline     
+10 & \scalebox{0.6}{$-0.02589 \pm 0.02487(-1.041)$} & \scalebox{0.6}{$-0.005148 \pm 0.02376(-0.2166)$} & \scalebox{0.6}{$-0.02395 \pm 0.02422(-0.9889)$}  \\ \hline    
+11 & \scalebox{0.6}{$-0.04134 \pm 0.02664(-1.552)$} & \scalebox{0.6}{$-0.03522 \pm 0.02517(-1.399)$} & \scalebox{0.6}{$-0.02359 \pm 0.0246(-0.9592)$}  \\ \hline       
+                                                                                                                                              
+    \end{tabular}                                                                                                                                              
+                                                                                                                                               
+\column{1.5in}
+\begin{itemize}
+\item With agreement with Michel previous studies \href{https://indico.cern.ch/event/290857/contribution/3/material/slides/0.pdf}{LINK}
+\end{itemize}                                                                                                                                           
+                                                                                                                                              
+
+                                                                                                                                                                                                                                                                                                                                                                                                                                                           \end{columns}
+}
+                                                                                                                                                                                                                                                                                                                                                                                                                                                           
+\end{frame}               
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{Conclusion on $1GeV$ binning}
 \begin{columns}
 \column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_175.png}\\
-
-
+\begin{itemize}
+\item Fits Highly bias and not usable.
+\item MM work fine.
+\item Christian developed his own fitter
+\item Let's try comparing those(not very fair comparison)!
+\end{itemize}
 \column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_400.png}\\
-
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1c_400E.png}\\
-
-
-
-\end{columns}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%55
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_400.png}\\
-
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J1s_400E.png}\\
-
-
-
-\end{columns}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_300.png}\\
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-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_300E.png}
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-\end{columns}
-\end{frame}
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-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_500.png}\\
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-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J2c_500E.png}\\
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-\end{columns}
-\end{frame}
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-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_75.png}\\
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-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_75E.png}
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-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_175.png}\\
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-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_175E.png}
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-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_300.png}\\
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-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_300E.png}
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-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J3_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J3_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J4_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J4_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J5_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J5_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J7_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J7_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J8_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J8_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_50.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_75.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_50E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_75E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_125.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_175.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_125E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_175E.png}
-
-
-\end{columns}
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_225.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_300.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_225E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_300E.png}
-
-
-\end{columns}
-\end{frame}
-
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_400.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_500.png}\\
-
-
-\column{2.5in}
-\includegraphics[scale=0.17]{plots/pool_plots/J9_400E.png}\\
-\includegraphics[scale=0.17]{plots/pool_plots/J9_500E.png}\\
-
-
-\end{columns}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J9J8.png}\\
-\includegraphics[scale=0.2]{plots/J9J5.png}\\
-
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J9J7.png}\\
-\includegraphics[scale=0.2]{plots/J9J4.png}\\
-
-\end{columns}
-
-\end{frame}
-
-\begin{frame}
-{~}
-
-\begin{columns}
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J9J3.png}\\
-\includegraphics[scale=0.2]{plots/J8J7.png}\\
-
-\column{2.5in}
-\includegraphics[scale=0.2]{plots/J8J5.png}\\
-\includegraphics[scale=0.2]{plots/J8J4.png}\\
+\includegraphics[width=0.8\textwidth]{Q2_4_S8.png}\\
+\includegraphics[width=0.8\textwidth]{Q2_5_S5.png}
 
 \end{columns}
 
 \end{frame}
 
 
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{MM vs Fit\footnote{Taken form Christoph's presentation}}
 
 
+\begin{tiny}
+\begin{columns}
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $F_l^{MM}$ & $F_l^{Fit}$ \\ \hline
+ $0$ & $0.0397$ & $0.025$\\ \hline
+ $1$ & $0.0802$ & $0.051$\\ \hline
+ $2$ & $0.0869$ & $0.057$\\ \hline
+ $3$ & $0.0893$ & $0.050$\\ \hline
+ $4$ & $0.0878$ & $0.051$\\ \hline
+ $5$ & $0.0848$ & $0.048$\\ \hline
+ $6$ & $0.0812$ & $0.047$\\ \hline
+ $7$ & $0.0775$ & $0.046$\\ \hline
+ $8$ & $0.0657$ & $0.041$\\ \hline
+ $9$ & $0.0687$ & $0.044$\\ \hline
+ $10$ & $0.0755$ & $0.045$\\ \hline
+ $11$ & $0.0967$ & $0.061$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_3^{MM}$ & $S_3^{Fit}$ \\ \hline
+ $0$ & $0.0656$ & $0.058$\\ \hline
+ $1$ & $0.109$ & $0.100$\\ \hline
+ $2$ & $0.116$ & $0.102$\\ \hline
+ $3$ & $0.12$ & $0.102$\\ \hline
+ $4$ & $0.118$ & $0.101$\\ \hline
+ $5$ & $0.115$ & $0.098$\\ \hline
+ $6$ & $0.112$ & $0.092$\\ \hline
+ $7$ & $0.108$ & $0.087$\\ \hline
+ $8$ & $0.0989$ & $0.090$\\ \hline
+ $9$ & $0.104$ & $0.098$\\ \hline
+ $10$ & $0.114$ & $0.108$\\ \hline
+ $11$ & $0.146$ & $0.155$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_4^{MM}$ & $S_4^{Fit}$ \\ \hline
+ $0$ & $0.0639$ & $0.054$\\ \hline
+ $1$ & $0.123$ & $0.115$\\ \hline
+ $2$ & $0.134$ & $0.114$\\ \hline
+ $3$ & $0.137$ & $0.123$\\ \hline
+ $4$ & $0.134$ & $0.116$\\ \hline
+ $5$ & $0.129$ & $0.112$\\ \hline
+ $6$ & $0.123$ & $0.104$\\ \hline
+ $7$ & $0.117$ & $0.100$\\ \hline
+ $8$ & $0.099$ & $0.086$\\ \hline
+ $9$ & $0.103$ & $0.098$\\ \hline
+ $10$ & $0.112$ & $0.109$\\ \hline
+ $11$ & $0.144$ & $0.160$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_5^{MM}$ & $S_5^{Fit}$ \\ \hline
+ $0$ & $ 0.0563$ & $0.050$\\ \hline
+ $1$ & $0.118$ & $0.114$\\ \hline
+ $2$ & $0.131$ & $0.108$\\ \hline
+ $3$ & $0.133$ & $0.117$\\ \hline
+ $4$ & $0.129$ & $0.105$\\ \hline
+ $5$ & $0.122$ & $0.106$\\ \hline
+ $6$ & $0.116$ & $0.097$\\ \hline
+ $7$ & $0.109$ & $0.094$\\ \hline
+ $8$ & $0.0884$ & $0.080$\\ \hline
+ $9$ & $0.0925$ & $0.085$\\ \hline
+ $10$ & $0.101$ & $0.096$\\ \hline
+ $11$ & $0.13$ & $0.144$\\ \hline
+    \end{tabular}                                                                                                                                              
+
+
+
+    \end{columns}
+    
+    
+    
+    
+\begin{columns}
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ &  $S_6^{MM}$ & $S_6^{Fit}$ \\ \hline
+ $0$ & $0.0632$ & $0.058$\\ \hline
+ $1$ & $0.0936$ & $0.085$\\ \hline
+ $2$ & $0.097$ & $0.093$\\ \hline
+ $3$ & $0.101$ & $0.085$\\ \hline
+ $4$ & $0.101$ & $0.083$\\ \hline
+ $5$ & $0.0999$ & $0.085$\\ \hline
+ $6$ & $0.0975$ & $0.080$\\ \hline
+ $7$ & $0.0941$ & $0.079$\\ \hline
+ $8$ & $0.0873$ & $0.073$\\ \hline
+ $9$ & $0.0925$ & $0.080$\\ \hline
+ $10$ & $0.104$ & $0.100$\\ \hline
+ $11$ & $0.137$ & $0.121$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_7^{MM}$ & $S_7^{Fit}$ \\ \hline
+ $0$ & $0.0574$ & $0.051$\\ \hline
+ $1$ & $0.118$ & $0.100$\\ \hline
+ $2$ & $0.131$ & $0.105$\\ \hline
+ $3$ & $0.134$ & $0.111$\\ \hline
+ $4$ & $0.131$ & $0.111$\\ \hline
+ $5$ & $0.125$ & $0.104$\\ \hline
+ $6$ & $0.119$ & $0.102$\\ \hline
+ $7$ & $0.113$ & $0.097$\\ \hline
+ $8$ & $0.0958$ & $0.085$\\ \hline
+ $9$ & $0.101$ & $0.091$\\ \hline
+ $10$ & $0.112$ & $0.101$\\ \hline
+ $11$ & $0.144$ & $0.136$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_8^{MM}$ & $S_8^{Fit}$ \\ \hline
+ $0$ & $0.0641$ & $0.058$\\ \hline
+ $1$ & $0.123$ & $0.113$\\ \hline
+ $2$ & $0.134$ & $0.120$\\ \hline
+ $3$ & $0.138$ & $0.119$\\ \hline
+ $4$ & $0.135$ & $0.112$\\ \hline
+ $5$ & $0.13$ & $0.108$\\ \hline
+ $6$ & $0.124$ & $0.103$\\ \hline
+ $7$ & $0.118$ & $0.101$\\ \hline
+ $8$ & $0.104$ & $0.092$\\ \hline
+ $9$ & $0.109$ & $0.095$\\ \hline
+ $10$ & $0.121$ & $0.115$\\ \hline
+ $11$ & $0.156$ & $0.149$\\ \hline
+    \end{tabular}                                                                                                                                              
+\column{1in}
+ \begin{tabular}{|c|c|c|}
+ \hline
+ $Q^2$ & $S_9^{MM}$ & $S_9^{Fit}$ \\ \hline
+ $0$ & $0.0656$ & $0.057$\\ \hline
+ $1$ & $0.109$ & $0.099$\\ \hline
+ $2$ & $0.116$ & $0.109$\\ \hline
+ $3$ & $0.12$ & $0.104$\\ \hline
+ $4$ & $0.119$ & $0.102$\\ \hline
+ $5$ & $0.116$ & $0.097$\\ \hline
+ $6$ & $0.112$ & $0.094$\\ \hline
+ $7$ & $0.108$ & $0.091$\\ \hline
+ $8$ & $0.0993$ & $0.079$\\ \hline
+ $9$ & $0.105$ & $0.088$\\ \hline
+ $10$ & $0.115$ & $0.103$\\ \hline
+ $11$ & $0.149$ & $0.143$\\ \hline
+    \end{tabular}                                                                                                                                              
+
+
+
+    \end{columns}
+\end{tiny}
+\end{frame}
 % ------------------------------------------------------------------------------
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{Conclusion}
+
+\begin{itemize}
+\item Method of moments a bit worse($\sim 15\%$) then optimistic fit.
+\item MM overestimates the error by fiew \%, fits understimates the error by fiew \%.
+\item Fit needs more study to understand why roofit is biased and Christoph fit is not.
+\end{itemize}
+
+
+\end{frame}
+
+
+
+
+
+
 \end{document}
diff --git a/Kstmumu/Face2Face_meeting/Comparison/Comparison.toc b/Kstmumu/Face2Face_meeting/Comparison/Comparison.toc
index bedbea4..bc756c5 100644
--- a/Kstmumu/Face2Face_meeting/Comparison/Comparison.toc
+++ b/Kstmumu/Face2Face_meeting/Comparison/Comparison.toc
@@ -1,7 +1,3 @@
 \beamer@endinputifotherversion {3.10pt}
 \select@language {english}
 \beamer@sectionintoc {1}{Introduction}{4}{0}{1}
-\beamer@sectionintoc {2}{Method of Moments - Theory}{5}{0}{2}
-\beamer@sectionintoc {3}{Moments of Ss}{7}{0}{3}
-\beamer@sectionintoc {4}{Toy MC study}{12}{0}{4}
-\beamer@sectionintoc {5}{S-wave}{16}{0}{5}
diff --git a/Kstmumu/Face2Face_meeting/Comparison/Q2_4_S8.png b/Kstmumu/Face2Face_meeting/Comparison/Q2_4_S8.png
new file mode 100644
index 0000000..9176de4
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/Q2_4_S8.png
Binary files differ
diff --git a/Kstmumu/Face2Face_meeting/Comparison/Q2_5_S5.png b/Kstmumu/Face2Face_meeting/Comparison/Q2_5_S5.png
new file mode 100644
index 0000000..17f67b8
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/Q2_5_S5.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/cosk_tmp.png b/Kstmumu/Face2Face_meeting/Comparison/cosk_tmp.png
new file mode 100644
index 0000000..843bb89
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/cosk_tmp.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/cosl_tmp.png b/Kstmumu/Face2Face_meeting/Comparison/cosl_tmp.png
new file mode 100644
index 0000000..554a8ef
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/cosl_tmp.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/mass.png b/Kstmumu/Face2Face_meeting/Comparison/mass.png
new file mode 100644
index 0000000..1179330
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/mass.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/mass2.png b/Kstmumu/Face2Face_meeting/Comparison/mass2.png
new file mode 100644
index 0000000..8e64acd
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/mass2.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/mass3.png b/Kstmumu/Face2Face_meeting/Comparison/mass3.png
new file mode 100644
index 0000000..189b135
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/mass3.png
Binary files differ
diff --git a/Kstmumu/Face2Face_meeting/Comparison/phi_tmp.png b/Kstmumu/Face2Face_meeting/Comparison/phi_tmp.png
new file mode 100644
index 0000000..598069d
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/phi_tmp.png
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diff --git a/Kstmumu/Face2Face_meeting/Comparison/tables/tables.aux b/Kstmumu/Face2Face_meeting/Comparison/tables/tables.aux
new file mode 100644
index 0000000..79f14a7
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/tables/tables.aux
@@ -0,0 +1,22 @@
+\relax 
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+  0 & \scalebox{0.5}{$-0.431 \pm 0.0184(-23.4)$} & \scalebox{0.5}{$0.00218 \pm 0.0186(0.118)$} & \scalebox{0.5}{$0.0389 \pm 0.0183(2.13)$} & \scalebox{0.5}{$0.0104 \pm 0.0183(0.564)$} & \scalebox{0.5}{$0.0357 \pm 0.0183(1.96)$} & \scalebox{0.5}{$-0.0179 \pm 0.018(-0.997)$} & \scalebox{0.5}{$-0.0311 \pm 0.0187(-1.66)$} & \scalebox{0.5}{$0.0274 \pm 0.0184(1.49)$} \\ \hline             
+1 & \scalebox{0.5}{$-0.029 \pm 0.0188(-1.56)$} & \scalebox{0.5}{$0.0247 \pm 0.0187(1.32)$} & \scalebox{0.5}{$0.016 \pm 0.0184(0.872)$} & \scalebox{0.5}{$-0.0125 \pm 0.0191(-0.657)$} & \scalebox{0.5}{$-0.00833 \pm 0.0186(-0.449)$} & \scalebox{0.5}{$-0.0221 \pm 0.0183(-1.21)$} & \scalebox{0.5}{$-0.0592 \pm 0.0185(-3.2)$} & \scalebox{0.5}{$0.0151 \pm 0.0181(0.836)$} \\ \hline         
+2 & \scalebox{0.5}{$0.0090 \pm 0.0181(0.501)$} & \scalebox{0.5}{$-0.0226 \pm 0.0186(-1.21)$} & \scalebox{0.5}{$-0.00623 \pm 0.018(-0.347)$} & \scalebox{0.5}{$-0.0235 \pm 0.018(-1.3)$} & \scalebox{0.5}{$-0.0201 \pm 0.0183(-1.1)$} & \scalebox{0.5}{$-0.00449 \pm 0.0185(-0.243)$} & \scalebox{0.5}{$-0.00996 \pm 0.0188(-0.529)$} & \scalebox{0.5}{$0.00609 \pm 0.0186(0.328)$} \\ \hline    
+3 & \scalebox{0.5}{$-0.046 \pm 0.0183(-2.56)$} & \scalebox{0.5}{$-0.00942 \pm 0.0183(-0.515)$} & \scalebox{0.5}{$-0.00109 \pm 0.0188(-0.0579)$} & \scalebox{0.5}{$0.0108 \pm 0.0188(0.577)$} & \scalebox{0.5}{$-0.0519 \pm 0.0184(-2.83)$} & \scalebox{0.5}{$0.0274 \pm 0.0177(1.55)$} & \scalebox{0.5}{$-0.00217 \pm 0.0186(-0.117)$} & \scalebox{0.5}{$-0.00915 \pm 0.0187(-0.49)$} \\ \hline 
+4 & \scalebox{0.5}{$-0.031 \pm 0.0183(-1.71)$} & \scalebox{0.5}{$0.0268 \pm 0.0181(1.48)$} & \scalebox{0.5}{$-0.00687 \pm 0.0182(-0.378)$} & \scalebox{0.5}{$-0.00106 \pm 0.0187(-0.0568)$} & \scalebox{0.5}{$0.00908 \pm 0.0189(0.481)$} & \scalebox{0.5}{$0.0156 \pm 0.0181(0.861)$} & \scalebox{0.5}{$-0.0141 \pm 0.0186(-0.759)$} & \scalebox{0.5}{$0.00498 \pm 0.0178(0.279)$} \\ \hline   
+5 & \scalebox{0.5}{$-0.034 \pm 0.0178(-1.96)$} & \scalebox{0.5}{$0.0231 \pm 0.0189(1.22)$} & \scalebox{0.5}{$-0.0169 \pm 0.0183(-0.92)$} & \scalebox{0.5}{$-0.0138 \pm 0.0183(-0.75)$} & \scalebox{0.5}{$9.56e-05 \pm 0.0184(0.00521)$} & \scalebox{0.5}{$0.0158 \pm 0.0186(0.848)$} & \scalebox{0.5}{$0.00727 \pm 0.0191(0.381)$} & \scalebox{0.5}{$0.029 \pm 0.0185(1.57)$} \\ \hline         
+6 & \scalebox{0.5}{$-0.031 \pm 0.0186(-1.69)$} & \scalebox{0.5}{$0.0184 \pm 0.0183(1)$} & \scalebox{0.5}{$-0.000709 \pm 0.0182(-0.039)$} & \scalebox{0.5}{$-0.00728 \pm 0.0189(-0.386)$} & \scalebox{0.5}{$0.0223 \pm 0.0182(1.22)$} & \scalebox{0.5}{$-0.00232 \pm 0.0186(-0.125)$} & \scalebox{0.5}{$0.00974 \pm 0.0177(0.551)$} & \scalebox{0.5}{$-0.00613 \pm 0.018(-0.341)$}\\ \hline      
+7 & \scalebox{0.5}{$0.0042 \pm 0.0188(0.22)$} & \scalebox{0.5}{$0.022 \pm 0.0181(1.22)$} & \scalebox{0.5}{$-0.00412 \pm 0.0188(-0.22)$} & \scalebox{0.5}{$0.0044 \pm 0.0187(0.236)$} & \scalebox{0.5}{$0.0291 \pm 0.0188(1.55)$} & \scalebox{0.5}{$-0.00853 \pm 0.0184(-0.463)$} & \scalebox{0.5}{$-0.00649 \pm 0.0182(-0.356)$} & \scalebox{0.5}{$0.00402 \pm 0.0183(0.22)$} \\ \hline         
+8 & \scalebox{0.5}{$0.0061 \pm 0.018(0.34)$} & \scalebox{0.5}{$0.0118 \pm 0.0184(0.643)$} & \scalebox{0.5}{$-0.0169 \pm 0.0185(-0.915)$} & \scalebox{0.5}{$0.0244 \pm 0.0182(1.34)$} & \scalebox{0.5}{$0.00532 \pm 0.0188(0.283)$} & \scalebox{0.5}{$-0.0137 \pm 0.0185(-0.739)$} & \scalebox{0.5}{$-0.0167 \pm 0.0185(-0.903)$} & \scalebox{0.5}{$-0.0278 \pm 0.0183(-1.52)$} \\ \hline        
+9 & \scalebox{0.5}{$0.0056 \pm 0.0184(0.30)$} & \scalebox{0.5}{$-0.00938 \pm 0.0182(-0.514)$} & \scalebox{0.5}{$-0.0405 \pm 0.0182(-2.22)$} & \scalebox{0.5}{$0.00885 \pm 0.0182(0.487)$} & \scalebox{0.5}{$0.0361 \pm 0.0185(1.96)$} & \scalebox{0.5}{$-0.0229 \pm 0.019(-1.2)$} & \scalebox{0.5}{$-0.0506 \pm 0.0183(-2.77)$} & \scalebox{0.5}{$-0.0269 \pm 0.0183(-1.46)$} \\ \hline         
+10 & \scalebox{0.5}{$-0.0156 \pm 0.0185(-0.84)$} & \scalebox{0.5}{$-0.00611 \pm 0.018(-0.34)$} & \scalebox{0.5}{$-0.0241 \pm 0.0184(-1.31)$} & \scalebox{0.5}{$0.0204 \pm 0.0186(1.09)$} & \scalebox{0.5}{$-0.00378 \pm 0.0189(-0.201)$} & \scalebox{0.5}{$-0.0155 \pm 0.0185(-0.84)$} & \scalebox{0.5}{$0.0276 \pm 0.0184(1.5)$} & \scalebox{0.5}{$0.0137 \pm 0.0185(0.742)$} \\ \hline        
+11 & \scalebox{0.5}{$-0.0079 \pm 0.018(-0.44)$} & \scalebox{0.5}{$0.0539 \pm 0.0182(2.96)$} & \scalebox{0.5}{$-0.0063 \pm 0.0189(-0.334)$} & \scalebox{0.5}{$-0.0297 \pm 0.019(-1.57)$} & \scalebox{0.5}{$-0.00305 \pm 0.0183(-0.166)$} & \scalebox{0.5}{$-0.0503 \pm 0.0183(-2.75)$} & \scalebox{0.5}{$-0.0137 \pm 0.0181(-0.758)$} & \scalebox{0.5}{$0.0169 \pm 0.0187(0.902)$} \\ \hline     
+
+    \end{tabular}
+    }
+  \end{frame}
+\end{document}
\ No newline at end of file
diff --git a/Kstmumu/Face2Face_meeting/Comparison/tables/tables.toc b/Kstmumu/Face2Face_meeting/Comparison/tables/tables.toc
new file mode 100644
index 0000000..e06b51d
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/tables/tables.toc
@@ -0,0 +1 @@
+\beamer@endinputifotherversion {3.10pt}
diff --git a/Kstmumu/Face2Face_meeting/Comparison/tmp.png b/Kstmumu/Face2Face_meeting/Comparison/tmp.png
new file mode 100644
index 0000000..574cb07
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/Comparison/tmp.png
Binary files differ
diff --git a/Kstmumu/Face2Face_meeting/mass.png b/Kstmumu/Face2Face_meeting/mass.png
new file mode 100644
index 0000000..1179330
--- /dev/null
+++ b/Kstmumu/Face2Face_meeting/mass.png
Binary files differ
diff --git a/Kstmumu/TOY_anal1/group_meeting.log b/Kstmumu/TOY_anal1/group_meeting.log
index 5d215ae..57d7171 100644
--- a/Kstmumu/TOY_anal1/group_meeting.log
+++ b/Kstmumu/TOY_anal1/group_meeting.log
@@ -1,4 +1,4 @@
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+Output written on group_meeting.pdf (17 pages, 1492143 bytes).
 PDF statistics:
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diff --git a/Kstmumu/TOY_anal1/group_meeting.pdf b/Kstmumu/TOY_anal1/group_meeting.pdf
index 675811c..dcac50a 100644
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Binary files differ
diff --git a/Kstmumu/TOY_anal1/group_meeting.synctex.gz b/Kstmumu/TOY_anal1/group_meeting.synctex.gz
index 7f5a84c..89c88c6 100644
--- a/Kstmumu/TOY_anal1/group_meeting.synctex.gz
+++ b/Kstmumu/TOY_anal1/group_meeting.synctex.gz
Binary files differ
diff --git a/Kstmumu/TOY_anal2/group_meeting.log b/Kstmumu/TOY_anal2/group_meeting.log
index 25e5646..fa88796 100644
--- a/Kstmumu/TOY_anal2/group_meeting.log
+++ b/Kstmumu/TOY_anal2/group_meeting.log
@@ -1,4 +1,4 @@
-This is pdfTeX, Version 3.1415926-1.40.10 (TeX Live 2009/Debian) (format=pdflatex 2014.3.24)  30 APR 2014 01:19
+This is pdfTeX, Version 3.1415926-1.40.10 (TeX Live 2009/Debian) (format=pdflatex 2014.3.24)  23 MAY 2014 23:56
 entering extended mode
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 **group_meeting.tex
@@ -1450,10 +1450,10 @@
 
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- 444021 string characters out of 1152823
- 576651 words of memory out of 3000000
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+ 24072 strings out of 493848
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+Output written on group_meeting.pdf (19 pages, 1419703 bytes).
 PDF statistics:
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diff --git a/Kstmumu/TOY_anal2/group_meeting.pdf b/Kstmumu/TOY_anal2/group_meeting.pdf
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