diff --git a/Seminars/IFJ_2016/mchrzasz.aux b/Seminars/IFJ_2016/mchrzasz.aux
index f9ff9e4..c33edbe 100644
--- a/Seminars/IFJ_2016/mchrzasz.aux
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diff --git a/Seminars/IFJ_2016/mchrzasz.log b/Seminars/IFJ_2016/mchrzasz.log
index 056e25f..757c51f 100644
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diff --git a/Seminars/IFJ_2016/mchrzasz.pdf b/Seminars/IFJ_2016/mchrzasz.pdf
index cd5fbcb..3b2441d 100644
--- a/Seminars/IFJ_2016/mchrzasz.pdf
+++ b/Seminars/IFJ_2016/mchrzasz.pdf
Binary files differ
diff --git a/Seminars/IFJ_2016/mchrzasz.snm b/Seminars/IFJ_2016/mchrzasz.snm
index 9c6786f..21df2a1 100644
--- a/Seminars/IFJ_2016/mchrzasz.snm
+++ b/Seminars/IFJ_2016/mchrzasz.snm
@@ -1,3 +1 @@
-\beamer@slide {Js}{32}
-\beamer@slide {LargeRecoilAs}{33}
-\beamer@slide {eq:physPars}{66}
+\beamer@slide {eq:physPars}{78}
diff --git a/Seminars/IFJ_2016/mchrzasz.synctex.gz b/Seminars/IFJ_2016/mchrzasz.synctex.gz
index e924361..c674551 100644
--- a/Seminars/IFJ_2016/mchrzasz.synctex.gz
+++ b/Seminars/IFJ_2016/mchrzasz.synctex.gz
Binary files differ
diff --git a/Seminars/IFJ_2016/mchrzasz.tex b/Seminars/IFJ_2016/mchrzasz.tex
index e114e8c..057c965 100644
--- a/Seminars/IFJ_2016/mchrzasz.tex
+++ b/Seminars/IFJ_2016/mchrzasz.tex
@@ -8,8 +8,7 @@
 	bullet=circle,		% Other option: square
 	bigpagenumber,		% circled page number on lower right
 	topline=true,			% colored bar at the top of the frame
-	shadow=false,			% Shading for beamer blocks
-	watermark=BG_lower,	% png file for the watermark
+	shadow=false,			% Shading for beamer blocks	watermark=BG_lower,	% png file for the watermark
 	]{Flip}
 
 %\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}}
@@ -367,16 +366,6 @@
 
 
 
-\fixme \fixme \fixme
-
-
-
-
-
-
-
-
-
 
 
 
@@ -384,16 +373,12 @@
 \begin{enumerate}
 \item Why flavour is important.
 \item LHCb detector.
-\item $\Pbeauty \to \Pstrange \ell \ell$ theory in a nutshell.
-\item LHCb measurements of $\PBd \to \PKstar \Pmu \Pmu$
-\begin{itemize}
-\item Maximum likelihood fit.
-\item Method of moments.
-\item Amplitudes fit.
-\end{itemize}
-\item Other related LHCb measurements.
-\item Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements.
-\item Disclaimers about some theory predictions. 
+\item Lepton Flavour Violation.
+\item Dark Boson searches.
+\item Electroweak penguins.
+\item Measurement of Higher $\PKstar$ states in Electroweak Penguin decays.
+\item Theory interpretation.
+\item Disclaimers about some theory predictions.
 \item Conclusions.
 \end{enumerate}
 
@@ -778,10 +763,12 @@
 \ARROW Each $\tau$ source ha it's own ''targer'' classifier.\\
 \ARROW 5 classifiers are then ''blended'' together.\\
 \ARROW Gain $6\%$ on signal efficiency.\\
-\ARROW Up to today the most advanced MVA used in LHCb!\\
+\begin{exampleblock}{}
+ Up to today the most advanced MVA used in LHCb!
+\end{exampleblock} 
 ~\\
 \ARROW Calibrated on data using $\PDs \to \phi \pi$
-\includegraphics[angle=-90,width=.75\textwidth]{m3body_2012.pdf}
+\includegraphics[angle=-90,width=.6\textwidth]{m3body_2012.pdf}
 
 \column{2in}
 \includegraphics[width=.99\textwidth]{images/diagram.png}\\
@@ -871,10 +858,12 @@
             \column{0.33\textwidth}
  \includegraphics[angle=-90,width=.78\textwidth]{images/RAD.pdf}\\
 \begin{small}
- \begin{itemize}
 
- \item M.Chrzaszcz, T.Przedzinski, Z.Was, J.Zareba\\ \href{https://arxiv.org/abs/1609.04617}{\color{blue}\texttt{arXiv:1609.04617 }}\\{~}\\{~}\\
- \end{itemize}
+\begin{exampleblock}{}
+M.Chrzaszcz, T.Przedzinski, Z.Was, J.Zareba\\ \href{https://arxiv.org/abs/1609.04617}{\color{blue}\texttt{arXiv:1609.04617 }}\\{~}\\
+
+\end{exampleblock}
+{~}\\
 \end{small}
 
 
@@ -914,11 +903,15 @@
 
 \ARROW To ''squeeze'' the most of the LFV New Physics exclusions there was an idea to combine the limits for LHCb and B factories.\\
 \ARROW As a result I have been enrolled as HFAG member.\\
-\ARROW $\tau \to \mu \mu \mu$ is the most cited number of the HFAG report!!!\\
-
+\begin{exampleblock}{}
+$\tau \to \mu \mu \mu$ is the most cited number of the HFAG report!!!\\
+\end{exampleblock}
 {~}\\
-  \includegraphics[width=0.95\textwidth]{images/TauLFV_UL_2014001_averaged.png} 
+  \includegraphics[width=0.9\textwidth]{images/TauLFV_UL_2014001_averaged.png} 
 
+\begin{exampleblock}{}
+\texttt{arXiv:1412.7515}, [HFAG, M.Chrzaszcz, et. al.]
+\end{exampleblock}
 
 \end{frame}  
 
@@ -1014,7 +1007,7 @@
 \ARROW The inflaton has a small width and non zero life-time. \\
 \ARROW The analysis is a peak search.\\
 \begin{exampleblock}{}
-It has passed the collaboration review and will be shown first time by my PhD student at the Epiephany conference.
+It has passed the collaboration review and will be shown first time by my PhD student at the Epiphany conference.
 \end{exampleblock}
 
 
@@ -1147,7 +1140,7 @@
 \end{frame}
 
 
-
+\iffalse
 
 \begin{frame}{Analysis of Rare decays}
 \begin{footnotesize}
@@ -1206,6 +1199,7 @@
 
 \end{frame}
 
+\fi
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
 
@@ -1306,6 +1300,9 @@
 \end{minipage}
 		\vspace*{2.1cm}
 \end{frame}
+
+\iffalse
+
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{frame}{Transversity amplitudes }
 {~}
@@ -1430,6 +1427,7 @@
 		\vspace*{2.1cm}
 \end{frame}
 
+\fi
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{frame}{Peaking backgrounds}
 {~}
@@ -1485,6 +1483,12 @@
 \item Completely data driven. 
 \end{footnotesize}
 \end{itemize}
+\begin{footnotesize}
+\begin{exampleblock}{}
+The k-Folding became a standard in LHCb
+\end{exampleblock}
+\end{footnotesize}
+
 \begin{center}
 \includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf}
 \end{center}
@@ -1522,7 +1526,7 @@
 \end{frame}
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
-
+\iffalse
 \begin{frame}{Mass modelling}
 {~}
 \begin{minipage}{\textwidth}
@@ -1552,6 +1556,8 @@
 \end{minipage}
 		\vspace*{2.1cm}
 \end{frame}
+
+
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{frame}{Monte Carlo corrections}
 {~}
@@ -1579,6 +1585,7 @@
 		\vspace*{2.1cm}
 \end{frame}
 
+\fi
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
@@ -1793,7 +1800,9 @@
 {~}
 \begin{footnotesize}
 	\begin{minipage}{\textwidth}
-\ARROW See {\color{blue}{\href{http://arxiv.org/abs/1503.04100}{Phys.Rev.D91(2015)114012}}}, F.Beaujean , M.Chrzaszcz, N.Serra, D. van Dyk for details.\\
+	\begin{exampleblock}{}
+See {\color{blue}{\href{http://arxiv.org/abs/1503.04100}{Phys.Rev.D91(2015)114012}}}, F.Beaujean , M.Chrzaszcz, N.Serra, D. van Dyk for details.\\
+\end{exampleblock}
 \ARROW The idea behind Method of Moments is simple: Use orthogonality of spherical harmonics, $f_j(\overrightarrow{\Omega})$ to solve for coefficients within a $q^2$ bin:
 \begin{align*}
 \int f_i(\overrightarrow{\Omega})  f_j(\overrightarrow{\Omega}) = \delta_{ij}
@@ -1823,7 +1832,9 @@
 	
 \only<3>
 {
-\ARROW Method of Moments allowed us to measure for the first time a new observable:
+\begin{exampleblock}{}
+Method of Moments allowed us to measure for the first time a new observable:
+\end{exampleblock}
 }	
 	
 \begin{center}
@@ -1954,6 +1965,437 @@
 
 
 
+\begin{frame}
+\begin{center}
+\begin{huge}
+
+Measurement of Higher $\PKstar$ states\\ in Electroweak Penguin decays
+
+\end{huge}
+\end{center}
+\end{frame}
+
+
+
+\begin{frame}\frametitle{$\PB \to \PKstar(1430) \Pmu \Pmu$}
+\begin{minipage}{\textwidth}
+{~}\\
+\ARROW If the NP effects the present in the $\PB  \to \PKstar \Pmu \Pmu$ there is no reason why this should not appear in the higher resonances.\\
+\ARROW One the $m_{\PK \Ppi}$ spectrum: $1330 < m_{\PK \Ppi} < 1530~\MeV/c^2$.\\
+\ARROW Variety of states in that region: $\PKstar(1410)$, $\PKstar_0(1430)$, $\PKstar_2(1430)$.\\
+%\ARROW D-wave needs to be included in the moments analysis.\\
+\ARROW 
+{~}\\
+\includegraphics[width=0.45\textwidth]{images/mkpi.png}
+\includegraphics[width=0.5\textwidth]{images/brk1430.png}
+
+\begin{exampleblock}{}
+First observation of this decay!
+
+\end{exampleblock}
+\end{minipage}		
+\vspace*{2.1cm}
+\end{frame}
+
+
+\begin{frame}\frametitle{$\PB \to \PKstar(1430) \Pmu \Pmu$}
+\begin{minipage}{\textwidth}
+{~}\\
+\ARROW D-wave needs to be included in the moments analysis.\\
+\ARROW You end up with 42 angular coefficients...\\
+\ARROW With current statistics only Method of Moments can handle this.\\
+{~}\\
+\includegraphics[width=0.45\textwidth]{images/Fig6a.png}
+\includegraphics[width=0.5\textwidth]{images/Fig6b.png}
+
+\begin{exampleblock}{}
+First angular analysis!\\
+Theory predictions in behind.
+
+\end{exampleblock}
+\end{minipage}		
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+
+
+
+
+
+
+
+
+
+\begin{frame}{Link the observables}
+\begin{footnotesize}
+
+\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}}
+
+\begin{itemize}
+
+\item Inclusive
+
+\begin{itemize}
+\item $B\to X_s\gamma$ {\color{gray}($BR$)
+.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$)
+............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+\end{itemize}
+
+\item Exclusive leptonic
+
+\begin{itemize}
+\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$)
+........................................................ } {\color{red} $\C{10}^{(\prime)}$}
+\end{itemize}
+
+\item Exclusive radiative/semileptonic
+\begin{itemize}
+\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$)
+................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+
+\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$)
+.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+
+\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.})
+.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+
+\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables)
+.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
+
+\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)}
+\item etc.
+\end{itemize}
+
+
+
+\end{itemize}
+\end{footnotesize}
+
+\end{frame}
+
+\frame{ \frametitle{Statistic details}
+
+\begin{footnotesize}
+
+\ARROW Frequentist approach:
+\medskip
+
+$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$
+
+
+\begin{itemize}
+\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time 
+\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters
+\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm]
+\end{itemize}
+For the Fit:
+\begin{itemize}
+\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$)  
+\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$
+%\item Compute pulls by inversion of the above formula
+\end{itemize}
+\medskip
+\ARROW The results from 1D scans:{~}\\{~}\\
+\begin{tiny}
+\begin{tabular}{crccc}
+%\toprule[1.6pt]
+Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\   \hspace{10mm} \\[5mm] 
+% \midrule 
+  $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ &  $\,\,\,\,\,\,\bf 4.5 
+ \cred \Leftarrow$  \hspace{5mm}  \\[3mm] 
+  $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad  4.2 
+   $\cred\Leftarrow$  \hspace{5mm}  \\[3mm] 
+   $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ &  \quad \quad \quad \,\,\quad 4.8
+     $\cred\Leftarrow$ (no $R_K$)\hspace{5mm}  \\[3mm] 
+
+ \hspace{5mm}  \\[3mm] 
+%  \bottomrule[1.6pt] 
+\end{tabular}
+\end{tiny}
+\end{footnotesize}
+
+}
+
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Theory implications}
+{~}
+	\begin{minipage}{\textwidth}
+
+\begin{itemize}
+\item The data can be explained by modifying the $C_9$ Wilson coefficient.
+\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM.
+\end{itemize}
+\includegraphics[width=0.9\textwidth]{images/C9.png}
+
+
+
+
+\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+
+
+\begin{frame}{2D scans}
+{~}
+\begin{footnotesize}
+
+	\begin{minipage}{\textwidth}
+\begin{columns}
+\begin{column}{0.5cm}
+
+
+\end{column}
+\begin{column}{17cm}
+
+\renewcommand{\arraystretch}{1.4}
+ \setlength{\tabcolsep}{13pt}
+\begin{tabular}{cccr}
+\hline
+Coefficient & Best Fit Point & Pull$_{\rm SM}$  \\  \hline
+
+  $(\C7^{\rm NP},\C9^{\rm NP})$ &  $(-0.00,-1.07)$  &  {\bf 4.1}  \hspace{5mm} \\ 
+ $(\C9^{\rm NP},\C{10}^{\rm NP})$ &  $(-1.08,0.33)$  &  {\bf 4.3}  \hspace{5mm} \\ 
+ $(\C9^{\rm NP},\C{7'}^{\rm NP})$ &  $(-1.09,0.02)$  &  {\bf 4.2}  \hspace{5mm} \\ 
+ $(\C9^{\rm NP},\C{9'}^{\rm NP})$ &  $(-1.12,0.77)$  &  {\bf 4.5}  \hspace{5mm} \\ 
+ $(\C9^{\rm NP},\C{10'}^{\rm NP})$ &  $(-1.17,-0.35)$  & {\bf  4.5}  \hspace{5mm} \\ 
+ $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-1.15,0.34)$  & \!\!\!\!\!\!\!\!\!\!\! {\bf 4.7} \\ 
+ $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-1.06,0.06)$  &  {\bf 4.4}  \hspace{5mm} \\ 
+ $(\C{9}^{\rm NP}=\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-0.64,-0.21)$  &  3.9  \hspace{5mm} \\ 
+ $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-0.72,0.29)$  &  3.8  \hspace{5mm} \\ 
+% $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-0.66,0.03)$  &  2.0 & 23.0  
+ %$(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-0.69,0.05)$  &  1.9 & 22.0 \hspace{5mm} \\ 
+
+\end{tabular}
+\end{column}
+\end{columns}
+
+
+\medskip
+\begin{itemize}
+\item $C_9^{NP}$ always play a dominant role
+\item All 2D scenarios above 4$\sigma$ are quite indistinguishable. We have done a  systematic study to check 
+ what are the most relevant Wilson Coefficients to explain all deviations, by allowing progressively different WC to get NP contributions and comparing the pulls.
+
+
+\end{itemize}
+
+
+
+\end{minipage}
+
+\end{footnotesize}
+		\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{If not NP?}
+{~}
+	\begin{minipage}{\textwidth}
+\begin{itemize}
+\item We are not there yet!
+\item There might be something not taken into account in the theory.
+\item Resonances ($\PJpsi$, $\Ppsi(2S)$) tails can mimic NP effects.
+\item There might be some non factorizable QCD corrections.\\
+'' However, the central value of this effect would have to be significantly larger than expected on the basis of existing estimates'' \texttt{D.Straub, 1503.06199}
+.
+\end{itemize}
+\only<1>{
+\begin{center}
+
+\includegraphics[width=0.9\textwidth]{images/QCDSHIT.png}
+\end{center}
+}
+\only<2>{
+\begin{center}
+\includegraphics[width=0.6\textwidth]{images/charmloop2.png}
+\end{center}
+}
+\only<3>{
+\begin{center}
+\includegraphics[width=0.6\textwidth]{images/charmloop3.png}
+\end{center}
+}
+\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{If not NP?}
+{~}
+	\begin{minipage}{\textwidth}
+\begin{itemize}
+\item How about our clean $P_i$ observables?
+\item The QCD cancel as mentioned only at leading order.
+\item Comparison to normal observables with the optimised ones.
+\end{itemize}
+\includegraphics[width=0.9\textwidth]{images/C9_S_P.png}
+
+
+	\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Why flavour physics
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}
+\begin{center}
+\begin{Huge}
+Disclaimers about some theory predictions
+\end{Huge}
+\end{center}
+
+
+
+
+\end{frame}
+
+
+
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Disclaimer 1 }
+{~}
+
+
+
+	\begin{minipage}{\textwidth}
+\ARROW \href{http://arxiv.org/abs/1512.07157}{\color{blue}{arXiv:1512.07157}}, Ciuchini, Fedele, Franco, Mishima, Paul, Silvestrini, Valli\\
+\begin{itemize} 
+\item Introduce a fully arbitrary parametrization for non-factorizable  power correction:
+\begin{align*}
+\H_\lambda \to H_\lambda + h_\lambda  \,\, {\rm where} \,\, h_{\lambda}=h_{\lambda}^{(0)}+h_{\lambda}^{(1)} q^2 + h_{\lambda}^{(2)} q^4  \quad {\rm and} \\ \quad  h_{\lambda}^{(0)}\to C_7^{NP}, h_{\lambda}^{(1)}\to C_9^{\rm NP}
+\end{align*}
+ with ($\lambda=0,\pm$)\hfill(copied from JC'14).\\
+{\bf Complications:}  complete lack of theory input/output $\Rightarrow$ {\bf no predictivity} with 18 free parameters (any shape). Specific problems...  
+
+\item Because of the polynomial parametrization this is completely unphysical as it will never reproduce the amplitudes that where measured at the $B \to K^{\ast} \PJpsi$.  
+
+
+ \end{itemize}
+ 
+	\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+
+\begin{frame}{Disclaimer 1 }
+{~}
+\begin{minipage}{\textwidth}
+\ARROW If one put some physics in their complete random parametrization.\\
+\ARROW For example at the $m_{\PJpsi}$ and $m_{\Ppsi(2S)}$ it has to reproduce the Babar, Belle, LHCb.\\
+\begin{exampleblock}{}
+\texttt{arXiv:1512.XXXX}, C.Bobeth, M.Chrzaszcz, D. van Dyk, J.Virto
+\end{exampleblock}
+\begin{center}
+\includegraphics[width=0.65\textwidth]{{images/fig-btokstarll-p5prime}.pdf}
+\end{center}
+
+
+	\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{Disclaimer 2}
+\ARROW arXiv::1603.04355
+\begin{center}
+\includegraphics[width=0.9\textwidth]{images/NP.png}
+\end{center}
+\only<2>{
+\includegraphics[width=0.55\textwidth]{images/rahul.png}
+}
+
+
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}\frametitle{Disclaimer 2}
+\ARROW arXiv::1603.04355
+\begin{columns}
+\column{0.1in}
+{~}
+\column{3in}
+\ARROW ''{\it The relation in Eq. (24) between form factors is expected to be satisfied in the large $q^2$ region. Eq. (24) is naturally satisfied if it is valid at each order in the Taylor expansion of the form factors}''\\
+\ARROW They need Eq. 24 to be valid with at least leading order at the Taylor expansion.\\ 
+\ARROW But this is not guaranteed as a resonant contribution can violate this expression.\\
+\ARROW  Futhermore the width of the of the $\PKstar$ screws up totally the end-points relations.
+\column{2in}
+\includegraphics[width=0.9\textwidth]{images/mist.png}\\
+\includegraphics[width=0.9\textwidth]{images/reson.png}\\
+
+\end{columns}
+\includegraphics[angle=-90,width=0.4\textwidth]{{images/ForTom_Q2_FLATQ2_Kmumu}.pdf} 
+\includegraphics[angle=-90,width=0.4\textwidth]{{images/ForTom_Q2_FLATQ2}.pdf} 
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Conclusions}
+{~}
+	\begin{minipage}{\textwidth}
+\begin{itemize}
+\item Enormous NP program searched performed!
+\item Clear tensions wrt. SM predictions!
+\item Measurements cluster in the same direction.
+\item We are not opening the champagne yet!
+\item Still need improvement both on theory and experimental side.
+\item Time will tell if this is QCD+fluctuations or new Physics:
+\end{itemize}
+\pause
+... when you have eliminated all the\\
+Standard Model explanations, whatever remains,\\
+however improbable, must be New Physics.\\
+
+
+	\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}
+{~}
+	\begin{minipage}{\textwidth}
+\begin{center}
+\begin{LARGE}
+Thank you for the attention!
+\end{LARGE}
+\includegraphics[width=0.8\textwidth]{images/Joke.jpg}
+
+\end{center}
+
+
+
+	\end{minipage}
+		\vspace*{2.1cm}
+\end{frame}
+
+
+
+\backupbegin
+
+\begin{frame}\frametitle{Backup}
+
+
+\end{frame}
+
+
+
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{frame}
@@ -2203,381 +2645,6 @@
 \end{frame}
 
 
-
-\begin{frame}{Link the observables}
-\begin{footnotesize}
-
-\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}}
-
-\begin{itemize}
-
-\item Inclusive
-
-\begin{itemize}
-\item $B\to X_s\gamma$ {\color{gray}($BR$)
-.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$)
-............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-\end{itemize}
-
-\item Exclusive leptonic
-
-\begin{itemize}
-\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$)
-........................................................ } {\color{red} $\C{10}^{(\prime)}$}
-\end{itemize}
-
-\item Exclusive radiative/semileptonic
-\begin{itemize}
-\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$)
-................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-
-\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$)
-.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-
-\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.})
-.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-
-\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables)
-.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$}
-
-\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)}
-\item etc.
-\end{itemize}
-
-
-
-\end{itemize}
-\end{footnotesize}
-
-\end{frame}
-
-\frame{ \frametitle{Statistic details}
-
-\begin{footnotesize}
-
-\ARROW Frequentist approach:
-\medskip
-
-$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$
-
-
-\begin{itemize}
-\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time 
-\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters
-\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm]
-\end{itemize}
-For the Fit:
-\begin{itemize}
-\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$)  
-\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$
-%\item Compute pulls by inversion of the above formula
-\end{itemize}
-\medskip
-\ARROW The results from 1D scans:{~}\\{~}\\
-\begin{tiny}
-\begin{tabular}{crccc}
-%\toprule[1.6pt]
-Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\   \hspace{10mm} \\[5mm] 
-% \midrule 
-  $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ &  $\,\,\,\,\,\,\bf 4.5 
- \cred \Leftarrow$  \hspace{5mm}  \\[3mm] 
-  $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad  4.2 
-   $\cred\Leftarrow$  \hspace{5mm}  \\[3mm] 
-   $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ &  \quad \quad \quad \,\,\quad 4.8
-     $\cred\Leftarrow$ (no $R_K$)\hspace{5mm}  \\[3mm] 
-
- \hspace{5mm}  \\[3mm] 
-%  \bottomrule[1.6pt] 
-\end{tabular}
-\end{tiny}
-\end{footnotesize}
-
-}
-
-
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{Theory implications}
-{~}
-	\begin{minipage}{\textwidth}
-
-\begin{itemize}
-\item The data can be explained by modifying the $C_9$ Wilson coefficient.
-\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM.
-\end{itemize}
-\includegraphics[width=0.9\textwidth]{images/C9.png}
-
-
-
-
-\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
-
-
-\begin{frame}{2D scans}
-{~}
-\begin{footnotesize}
-
-	\begin{minipage}{\textwidth}
-\begin{columns}
-\begin{column}{0.5cm}
-
-
-\end{column}
-\begin{column}{17cm}
-
-\renewcommand{\arraystretch}{1.4}
- \setlength{\tabcolsep}{13pt}
-\begin{tabular}{cccr}
-\hline
-Coefficient & Best Fit Point & Pull$_{\rm SM}$  \\  \hline
-
-  $(\C7^{\rm NP},\C9^{\rm NP})$ &  $(-0.00,-1.07)$  &  {\bf 4.1}  \hspace{5mm} \\ 
- $(\C9^{\rm NP},\C{10}^{\rm NP})$ &  $(-1.08,0.33)$  &  {\bf 4.3}  \hspace{5mm} \\ 
- $(\C9^{\rm NP},\C{7'}^{\rm NP})$ &  $(-1.09,0.02)$  &  {\bf 4.2}  \hspace{5mm} \\ 
- $(\C9^{\rm NP},\C{9'}^{\rm NP})$ &  $(-1.12,0.77)$  &  {\bf 4.5}  \hspace{5mm} \\ 
- $(\C9^{\rm NP},\C{10'}^{\rm NP})$ &  $(-1.17,-0.35)$  & {\bf  4.5}  \hspace{5mm} \\ 
- $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-1.15,0.34)$  & \!\!\!\!\!\!\!\!\!\!\! {\bf 4.7} \\ 
- $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-1.06,0.06)$  &  {\bf 4.4}  \hspace{5mm} \\ 
- $(\C{9}^{\rm NP}=\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-0.64,-0.21)$  &  3.9  \hspace{5mm} \\ 
- $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=\C{10'}^{\rm NP})$ &  $(-0.72,0.29)$  &  3.8  \hspace{5mm} \\ 
-% $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-0.66,0.03)$  &  2.0 & 23.0  
- %$(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ &  $(-0.69,0.05)$  &  1.9 & 22.0 \hspace{5mm} \\ 
-
-\end{tabular}
-\end{column}
-\end{columns}
-
-
-\medskip
-\begin{itemize}
-\item $C_9^{NP}$ always play a dominant role
-\item All 2D scenarios above 4$\sigma$ are quite indistinguishable. We have done a  systematic study to check 
- what are the most relevant Wilson Coefficients to explain all deviations, by allowing progressively different WC to get NP contributions and comparing the pulls.
-
-
-\end{itemize}
-
-
-
-\end{minipage}
-
-\end{footnotesize}
-		\vspace*{2.1cm}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{If not NP?}
-{~}
-	\begin{minipage}{\textwidth}
-\begin{itemize}
-\item We are not there yet!
-\item There might be something not taken into account in the theory.
-\item Resonances ($\PJpsi$, $\Ppsi(2S)$) tails can mimic NP effects.
-\item There might be some non factorizable QCD corrections.\\
-'' However, the central value of this effect would have to be significantly larger than expected on the basis of existing estimates'' \texttt{D.Straub, 1503.06199}
-.
-\end{itemize}
-\only<1>{
-\begin{center}
-
-\includegraphics[width=0.9\textwidth]{images/QCDSHIT.png}
-\end{center}
-}
-\only<2>{
-\begin{center}
-\includegraphics[width=0.6\textwidth]{images/charmloop2.png}
-\end{center}
-}
-\only<3>{
-\begin{center}
-\includegraphics[width=0.6\textwidth]{images/charmloop3.png}
-\end{center}
-}
-\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{If not NP?}
-{~}
-	\begin{minipage}{\textwidth}
-\begin{itemize}
-\item How about our clean $P_i$ observables?
-\item The QCD cancel as mentioned only at leading order.
-\item Comparison to normal observables with the optimised ones.
-\end{itemize}
-\includegraphics[width=0.9\textwidth]{images/C9_S_P.png}
-
-
-	\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{There is more!}
-{~}
-	\begin{minipage}{\textwidth}
-
-\begin{itemize}
-\item There is one other LUV decay recently measured by LHCb.
-\item $R(\PDstar)=\dfrac{\mathcal{B}(\PB \to \PDstar \Ptau \Pnu)}{\mathcal{B}(\PB \to \PDstar \Pmu \Pnu)}$
-\item Clean SM prediction: $R(\PDstar)=0.252(3)$, PRD 85 094025 (2012)
-\item LHCb result: $R(\PDstar)= 0.336 \pm 0.027 \pm 0.030$, HFAG average: $R(\PDstar)=0.322 \pm 0.022$
-\item $3.9~\sigma$ discrepancy wrt. SM.
-\end{itemize}
-
-\begin{center}
-
-\includegraphics[width=0.52\textwidth]{images/RDstar.png}
-
-\end{center}
-	\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-% Why flavour physics
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-\begin{center}
-\begin{Huge}
-Disclaimers about some theory predictions
-\end{Huge}
-\end{center}
-
-
-
-
-\end{frame}
-
-
-
-
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{Disclaimer 1 }
-{~}
-
-
-
-	\begin{minipage}{\textwidth}
-\ARROW \href{http://arxiv.org/abs/1512.07157}{\color{blue}{arXiv:1512.07157}}, Ciuchini, Fedele, Franco, Mishima, Paul, Silvestrini, Valli\\
-\begin{itemize} 
-\item Introduce a fully arbitrary parametrization for non-factorizable  power correction:
-\begin{align*}
-\H_\lambda \to H_\lambda + h_\lambda  \,\, {\rm where} \,\, h_{\lambda}=h_{\lambda}^{(0)}+h_{\lambda}^{(1)} q^2 + h_{\lambda}^{(2)} q^4  \quad {\rm and} \\ \quad  h_{\lambda}^{(0)}\to C_7^{NP}, h_{\lambda}^{(1)}\to C_9^{\rm NP}
-\end{align*}
- with ($\lambda=0,\pm$)\hfill(copied from JC'14).\\
-{\bf Complications:}  complete lack of theory input/output $\Rightarrow$ {\bf no predictivity} with 18 free parameters (any shape). Specific problems...  
-
-\item Because of the polynomial parametrization this is completely unphysical as it will never reproduce the amplitudes that where measured at the $B \to K^{\ast} \PJpsi$.  
-
-
- \end{itemize}
-	\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
-
-
-
-
-
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}\frametitle{Disclaimer 2}
-\ARROW arXiv::1603.04355
-\begin{center}
-\includegraphics[width=0.9\textwidth]{images/NP.png}
-\end{center}
-
-
-\end{frame}
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}\frametitle{Disclaimer 2}
-\ARROW arXiv::1603.04355
-\begin{columns}
-\column{0.1in}
-{~}
-\column{3in}
-\ARROW ''{\it The relation in Eq. (24) between form factors is expected to be satisfied in the large $q^2$ region. Eq. (24) is naturally satisfied if it is valid at each order in the Taylor expansion of the form factors}''\\
-\ARROW They need Eq. 24 to be valid with at least leading order at the Taylor expansion.\\ 
-\ARROW But this is not guaranteed as a resonant contribution can violate this expression.\\
-
-\column{2in}
-\includegraphics[width=0.9\textwidth]{images/mist.png}\\
-\includegraphics[width=0.9\textwidth]{images/reson.png}\\
-
-\end{columns}
-
-
-\end{frame}
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}{Conclusions}
-{~}
-	\begin{minipage}{\textwidth}
-\begin{itemize}
-\item Clear tensions wrt. SM predictions!
-\item Measurements cluster in the same direction.
-\item We are not opening the champagne yet!
-\item Still need improvement both on theory and experimental side.
-\item Time will tell if this is QCD+fluctuations or new Physics:
-\end{itemize}
-\pause
-''... when you have eliminated all the\\
-Standard Model explanations, whatever remains,\\
-however improbable, must be New Physics.''\\
-prof. Joaquim Matias
-
-	\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
-
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-\begin{frame}
-{~}
-	\begin{minipage}{\textwidth}
-\begin{center}
-\begin{LARGE}
-Thank you for the attention!
-\end{LARGE}
-\includegraphics[width=0.8\textwidth]{images/Joke.jpg}
-
-\end{center}
-
-
-
-	\end{minipage}
-		\vspace*{2.1cm}
-\end{frame}
-
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