diff --git a/KEK_Workshop_2015/Makefile b/KEK_Workshop_2015/Makefile
new file mode 100644
index 0000000..e4cf8e8
--- /dev/null
+++ b/KEK_Workshop_2015/Makefile
@@ -0,0 +1,9 @@
+all: mchrzasz.pdf
+
+mchrzasz.pdf: mchrzasz.tex
+	xelatex mchrzasz.tex
+#	bibtex mchrzasz
+	xelatex mchrzasz.tex
+#	xelatex mchrzasz.tex
+clean:
+	rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav 
diff --git a/KEK_Workshop_2015/beamercolorthemeFlip.sty b/KEK_Workshop_2015/beamercolorthemeFlip.sty
new file mode 100755
index 0000000..d6b9c50
--- /dev/null
+++ b/KEK_Workshop_2015/beamercolorthemeFlip.sty
@@ -0,0 +1,179 @@
+% Color style file for the BEAMER FLIP THEME
+% Copyright 2012 by Flip Tanedo
+% This file may be distributed and/or modified
+% 	1. under the LaTeX Project Public License and/or
+% 	2. under the GNU Public License.
+
+
+
+\mode<presentation>
+\newif\ifbeamer@Flip@dark
+\beamer@Flip@darkfalse
+\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue}
+\ProcessOptionsBeamer
+
+
+% These are a few colors that I like.
+
+\definecolor{crimsonred}{RGB}{153,0,0}		% Neurtal red, good for dark or light bg
+\definecolor{darkcharcoal}{RGB}{25,25,25}		% Darker gray
+\definecolor{charcoal}{RGB}{51,51,51}		% Darker gray
+\definecolor{ash}{RGB}{100,100,100}			% medium gray
+\definecolor{paleblue}{RGB}{0,102,102}		% More of an `ocean' color
+\definecolor{turtlegreen}{RGB}{51,153,0}	% A more neutral green
+\definecolor{paleale}{RGB}{204,204,102}		% Only for dark BG
+\definecolor{lager}{RGB}{140,110,10}		% Use instead of pale ale for white BG
+\definecolor{regal}{RGB}{90,0,120}			% A more neutral purple
+\definecolor{jeans}{RGB}{20,30,150}			% A more neutral blue
+
+
+% Define some "invariant colors" so that a color that doen't work with a
+% light/dark background will automatically be substituted with one that does.
+% These will be rewritten in beamercolorthemeFlipDark
+
+\ifbeamer@Flip@dark
+	\definecolor{FlipSand}{RGB}{204,204,102}		% paleale, Only for dark BG
+	\definecolor{FlipGreen}{RGB}{0,255,0}			% Neon-like green, only for dark BG
+\else
+	\definecolor{FlipSand}{RGB}{140,110,10}			% lager, Only for light BG
+	\definecolor{FlipGreen}{RGB}{51,153,0}			% turtlegreen, works for both
+\fi
+
+%% Future revision: It would be nice to define these in terms of the palette.
+
+
+\ifbeamer@Flip@dark
+	\setbeamercolor{normal text}{fg=white, bg=black}		
+	\setbeamercolor{structure}{fg=gray, bg=black}		% fg controls bullets
+	\setbeamercolor*{footerlike}{fg=white,bg=black}		% Controls the footerline
+\else
+	% Default to black on white
+	\setbeamercolor*{footerlike}{fg=white,bg=charcoal}	% for charcoal footer
+	\setbeamercolor{structure}{fg=charcoal, bg=white}	% fg controls bullets
+	% \setbeamercolor{normal text}{fg=white, bg=black}	
+\fi
+
+
+
+
+
+% These defined colors can be used in \textcolor{colorname}{text in that color}.
+
+% Colors for Keynote background: DARK
+\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38}
+\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16}
+\definecolor{keynotetop}{rgb}{0,0,0}
+%%% Example of usage:
+%% \setbeamertemplate{background canvas}[vertical shading]
+%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop]
+
+
+
+
+% ALERT AND COMMENT COLORS (just copies of the above colors)
+% (I don't know how ot do this more elegantly)
+\ifbeamer@Flip@dark
+	\definecolor{ALERT}{RGB}{153,0,0}			% crimsonred
+	\definecolor{Alert}{RGB}{51,153,0}			% turtlegreen
+	\definecolor{alert}{RGB}{204,204,102}		% paleale		
+	\definecolor{charcoal}{RGB}{51,51,51}		% charcoal
+	\definecolor{comment}{RGB}{80,80,80}		% light charcoal
+	\definecolor{Comment}{RGB}{100,100,100}		% ash
+	\definecolor{COMMENT}{RGB}{80,20,120}		% regal
+\else
+%	\definecolor{ALERT}{RGB}{153,0,0}			% crimsonred
+	\definecolor{ALERT}{RGB}{28,134,238}		% DodgerBlue2
+%	\definecolor{Alert}{RGB}{51,153,0}			% turtlegreen
+	\definecolor{Alert}{RGB}{255,127,36}		% chocolate1
+%	\definecolor{alert}{RGB}{140,110,10}		% lager
+	\definecolor{alert}{RGB}{0,205,102} 		% SpringGreen3
+	\definecolor{charcoal}{RGB}{80,80,80}		% light charcoal
+	\definecolor{comment}{RGB}{51,51,51}		% charcoal
+	\definecolor{Comment}{RGB}{100,100,100}		% ash
+	\definecolor{COMMENT}{RGB}{80,20,120}		% regal
+\fi
+
+
+% \definecolor{crimsonred}{RGB}{153,0,0}		% Neurtal red, good for dark or light bg
+% \definecolor{charcoal}{RGB}{51,51,51}		% Darker gray
+% \definecolor{ash}{RGB}{100,100,100}			% medium gray
+% \definecolor{paleblue}{RGB}{0,102,102}		% More of an `ocean' color
+% \definecolor{turtlegreen}{RGB}{51,153,0}	% A more neutral green
+% \definecolor{paleale}{RGB}{204,204,102}		% Only for dark BG
+% \definecolor{lager}{RGB}{140,110,10}		% Use instead of pale ale for white BG
+% \definecolor{regal}{RGB}{90,0,120}			% A more neutral purple
+% \definecolor{jeans}{RGB}{20,30,150}			% A more neutral blue
+
+
+% A few useful colors
+\setbeamercolor{alerted text}{fg=alert}
+
+%% I would like ot use these colors, but there seems to be a bug in Beamer
+%% where the footnote color infects the normal text color
+%% See:  http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268
+
+% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand}
+% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand}
+
+% Blocks
+\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal}
+\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white}
+
+\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black}
+\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white}
+% 
+\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black}
+\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white}
+
+
+
+% These "setbeamercolor" commands are more standardized. 
+
+
+%% From the Beamer User Guide:
+% Outer themes base the color of navigational elements and, possibly, also of other elements, on the 
+% four palette colors. The “primary” palette should be used for the most important navigational elements, 
+% which are usually the ones that change most often and hence require the most attention by the audience. 
+% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. 
+% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. 
+% For the sidebar, there is an extra set of palette colors, see palette sidebar primary.
+
+\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal}
+\setbeamercolor*{palette secondary}{fg=paleale,bg=lager}
+\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans}
+\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal}
+
+% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white}
+% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white}
+% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white}
+% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white}
+
+
+
+%% These are some structures that I define for use in the outer theme.
+
+\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred}
+\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2}
+%\setbeamercolor*{titlelike}{fg=crimsonred}
+\setbeamercolor*{titlelike}{fg=DodgerBlue2}
+\setbeamercolor*{topbarlike}{fg=white, bg=charcoal}
+
+
+
+
+
+%% Some old definitions that I might want to get back to
+%
+% \setbeamercolor*{frametitle}{bg=white,fg=charcoal}
+% \setbeamercolor*{part title}{bg=white,fg=charcoal}
+% \setbeamercolor*{item}{fg=charcoal, bg=white}
+% 
+% \setbeamercolor*{separation line}{}
+% \setbeamercolor*{fine separation line}{}
+
+
+
+
+
+\mode
+<all>
diff --git a/KEK_Workshop_2015/beamerinnerthemeFlip.sty b/KEK_Workshop_2015/beamerinnerthemeFlip.sty
new file mode 100755
index 0000000..9910f4d
--- /dev/null
+++ b/KEK_Workshop_2015/beamerinnerthemeFlip.sty
@@ -0,0 +1,95 @@
+% Inner style file for the BEAMER FLIP THEME
+% Copyright 2010 by Flip Tanedo
+% This file may be distributed and/or modified
+% 	1. under the LaTeX Project Public License and/or
+% 	2. under the GNU Public License.
+%
+% Based on: beamerinnerthemeFlip by Marco Barisione
+
+\mode<presentation>
+
+% % Use alternative title page style.
+% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}}
+
+% Logo to use in the alternative title page.
+% \def\beamer@Flip@titlepagelogo{}
+% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}}
+
+% Bullet shape.
+\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}}
+\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}}
+\ExecuteOptionsBeamer{shadow=false}
+
+
+% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square}
+\ProcessOptionsBeamer
+
+
+
+% Margins.
+\newlength{\beamer@Flip@normalmargin}
+\setlength{\beamer@Flip@normalmargin}{.06\paperwidth}
+\setbeamersize{text margin left=\beamer@Flip@normalmargin}
+\setbeamersize{text margin right=\beamer@Flip@normalmargin}
+\setlength\leftmargini{.6\beamer@Flip@normalmargin}
+\setlength\leftmarginii{.6\beamer@Flip@normalmargin}
+\setlength\leftmarginiii{.6\beamer@Flip@normalmargin}
+
+% Normal title page.
+\defbeamertemplate*{title page normal}{Flip theme}[1][]
+{
+  \vbox{}
+  \vfill
+  \begin{centering}
+    \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header}
+      \usebeamerfont{title}\inserttitle\par%
+      \ifx\insertsubtitle\@empty%
+      \else%
+        \vskip0.25em%
+        {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}%
+      \fi%     
+    \end{beamercolorbox}%
+    \vskip1em\par
+    \begin{beamercolorbox}[sep=8pt,center,#1]{author}
+      \usebeamerfont{author}\insertauthor
+    \end{beamercolorbox}
+    \begin{beamercolorbox}[sep=8pt,center,#1]{institute}
+      \usebeamerfont{institute}\insertinstitute
+    \end{beamercolorbox}
+    \begin{beamercolorbox}[sep=8pt,center,#1]{date}
+      \usebeamerfont{date}\insertdate
+    \end{beamercolorbox}\vskip0.5em
+    {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par}
+  \end{centering}
+  \vfill
+}
+
+
+% Items.
+\defbeamertemplate{itemize item}{squarealt}%
+{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}}
+\defbeamertemplate{itemize subitem}{squarealt}%
+{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}}
+\defbeamertemplate{itemize subsubitem}{squarealt}%
+{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}}
+% 
+\defbeamertemplate{itemize item}{circlealt}%
+{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}}
+\defbeamertemplate{itemize subitem}{circlealt}%
+{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}}
+\defbeamertemplate{itemize subsubitem}{circlealt}%
+{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}}
+\setbeamertemplate{items}[circlealt]
+% 
+\def\circletext{circle}
+\ifx\beamer@Flip@bullet\circletext
+  \setbeamertemplate{items}[circlealt]
+\else
+  \setbeamertemplate{items}[squarealt]
+\fi
+
+\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow]
+
+
+\mode<all>
+
diff --git a/KEK_Workshop_2015/beamerouterthemeFlip.sty b/KEK_Workshop_2015/beamerouterthemeFlip.sty
new file mode 100755
index 0000000..d12f6d6
--- /dev/null
+++ b/KEK_Workshop_2015/beamerouterthemeFlip.sty
@@ -0,0 +1,189 @@
+% Outer style file for the BEAMER FLIP THEME 212
+% Copyright 2012 by Flip Tanedo
+% This file may be distributed and/or modified
+% 	1. under the LaTeX Project Public License and/or
+% 	2. under the GNU Public License.
+%
+% Based on: beamerouterthemesplit by Till Tantau
+
+
+\mode<presentation>
+
+% Watermark
+\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}}
+\ExecuteOptionsBeamer{watermark=} % Default value is empty
+
+
+\newif\ifbeamer@Flip@bigpagenumber
+\beamer@Flip@bigpagenumberfalse
+\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue}
+
+
+\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx
+
+\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}}
+\ExecuteOptionsBeamer{topline=false} % Default
+
+
+
+% \ExecuteOptionsBeamer{topline=} % Default value is empty
+
+
+\ProcessOptionsBeamer
+
+
+\usepackage{tikz}	% For fancy decorations
+
+
+% I should fix these up to be more robust against color changes
+\setbeamercolor{section in head/foot}{parent=footerlike}
+\setbeamercolor{subsection in head/foot}{parent=footerlike}
+\setbeamercolor{author in head/foot}{parent=footerlike}
+\setbeamercolor{title in head/foot}{parent=footerlike}
+
+
+% \setbeamercolor{author in head/foot}{parent=section in head/foot}
+% \setbeamercolor{title in head/foot}{parent=subsection in head/foot}
+
+%\setbeamercolor{topbar}{parent=crimsontown}
+\setbeamercolor{topbar}{parent=bluetown}
+
+
+
+
+\usesectionheadtemplate
+  {\hfill\insertsectionhead}
+  {\hfill\color{fg!50!bg}\insertsectionhead}
+
+
+%%%%%%%%%%%%%%%%%%
+% The footer bar %
+%%%%%%%%%%%%%%%%%%
+
+\defbeamertemplate*{footline}{Flip theme}
+{%
+  \leavevmode% 
+% OBSERVATION: the "%" symbols inside hbox are all very important here.
+% The \hbox enviroment will insert spaces whenever there's whitespace
+% Adding a % at the END of each line ensures that any hard returns aren't
+% interpreted as white space. This allows the color boxes to be flush against
+% one another. If a faint white line appears one could probably do something like
+% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox.	
+
+\hbox{%
+\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}%
+	\usebeamerfont{author in head/foot}\insertshortauthor  \end{beamercolorbox}%
+%
+\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}%
+    \usebeamerfont{title in head/foot}{\textit \insertshorttitle}%
+    \hskip2ex plus1fill%
+		% \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number
+		\insertframenumber/\inserttotalframenumber
+ \end{beamercolorbox}%
+}%
+
+% This is a complete kludge for the faint white line which appears
+% between the beamer color boxes above. (It doesnt appear in presentation mode
+% but sometimes looks funny when the pdfs are viewed in a window)
+\begin{tikzpicture}[overlay]
+	\usebeamercolor[bg]{author in head/foot}
+	\draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex);
+	\draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex);
+	\draw[thick] (0,0) -- (\paperwidth,0);
+\end{tikzpicture}
+
+
+
+\ifbeamer@Flip@bigpagenumber
+	\begin{tikzpicture}[overlay]
+	\usebeamercolor[bg]{author in head/foot}
+	\draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex);
+	\usebeamercolor[fg]{author in head/foot}
+	\draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex);
+	\usebeamercolor[bg]{author in head/foot}
+	\node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$};
+	\end{tikzpicture}
+\fi
+}
+
+
+
+\defbeamertemplate*{frametitle}{Flip theme}[1][left]
+{
+% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}%
+\@tempdima=\textwidth%
+\advance\@tempdima by\beamer@leftmargin%
+\advance\@tempdima by\beamer@rightmargin%
+
+\vbox{}\vskip-3.5ex%
+%
+\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike}
+	\usebeamerfont{frametitle}%
+	\vbox{}\vskip-1ex%
+	\if@tempswa\else\csname beamer@fte#1\endcsname\fi%
+	% \strut{\bf\insertframetitle}\strut\par% 					%% Include the \bf
+	\strut{\insertframetitle}\strut\par%
+	{%
+  		\ifx\insertframesubtitle\@empty%
+  		\else
+			{\usebeamerfont{framesubtitle}
+			 \usebeamercolor[fg]{framesubtitle}
+			\insertframesubtitle\strut\par}%
+  		\fi
+ 	}%
+	%
+  	\vskip-1ex%
+  	\if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here...
+\end{beamercolorbox}%
+%%
+
+% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm}
+}
+
+
+
+
+% Sidebar right is important: anything placed here will be
+% visible *behind* the main text. This is where to put any
+% interesting watermarks.
+%
+% 
+\defbeamertemplate*{sidebar right}{Flip theme}
+{
+% \llap{\includegraphics[width=50px]{footdecoration}}
+% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}}
+%
+% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG
+% ... make a png of the background with TRANSPARENT BG
+% ... then put the image here (use \hfill to get it on the left)
+% Now one can FURTHER apply a slight gradient in the BG
+%
+% 
+% % Top Line 
+\ifx\beamer@Flip@topline\beamer@Flip@truetext
+	\begin{tikzpicture}[overlay]
+	\usebeamercolor[fg]{titlelike}	% alternately, topbarlike would be a good beamercolor
+%	\usebeamercolor[fg]{topbarlike}	% alternately, topbarlike would be a good beamercolor
+	\draw[fill] (-\paperwidth,0) rectangle (0,-3pt);
+	\end{tikzpicture}
+\fi
+%
+% 
+  \vskip.2\beamer@leftmargin%
+   %\llap{\insertlogo\hskip.5\beamer@leftmargin}%
+   \llap{\insertlogo\hskip.08\beamer@leftmargin}%
+    \vfill%
+  \if \beamer@Flip@watermark\@empty
+	% This is kind of a kludge since if I put anything in here, I automatically get errors
+	% Somehow LaTeX wants to read the \else part!
+	\else%
+	\llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}}
+  \fi
+}
+
+
+
+\mode<all>
+\endinput
+
+
diff --git a/KEK_Workshop_2015/beamerouterthemedecolines.sty b/KEK_Workshop_2015/beamerouterthemedecolines.sty
new file mode 100755
index 0000000..669e493
--- /dev/null
+++ b/KEK_Workshop_2015/beamerouterthemedecolines.sty
@@ -0,0 +1,168 @@
+% Copyright 2007 by Marco Barisione
+%
+% This file may be distributed and/or modified
+%
+% 1. under the LaTeX Project Public License and/or
+% 2. under the GNU Public License.
+
+\mode<presentation>
+
+% String used between the current page and the total page count.
+\def\beamer@decolines@pageofpages{/}
+\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}}
+
+% Show a line below the frame title.
+\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}}
+
+% Image used for the watermark.
+\def\beamer@decolines@watermarkorig{}
+\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}}
+
+% Height of the watermark.
+\def\beamer@decolines@watermarkheight{100px}
+\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}}
+
+% The original image height is watermarkheightmult * watermarkheight.
+\def\beamer@decolines@watermarkheightmult{1}
+\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}}
+
+\ExecuteOptionsBeamer{titleline=false}
+\ProcessOptionsBeamer
+
+% Enable/disable the watermark.
+\def\watermarkon{%
+  \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}%
+}
+\def\watermarkoff{\def\beamer@decolines@watermark{}}
+
+% Initially enable the watermark.
+\watermarkon
+
+% Colors.
+\setbeamercolor*{lineup}{parent=palette primary}
+\setbeamercolor*{linemid}{parent=palette secondary}
+\setbeamercolor*{linebottom}{parent=palette tertiary}
+\setbeamercolor*{page header}{parent=titlelike}
+
+% Lengths
+\newlength{\headerheight}
+\setlength{\headerheight}{.045\paperheight}
+\newlength{\beamer@decolines@lineup}
+\setlength{\beamer@decolines@lineup}{.025\paperheight}
+\newlength{\beamer@decolines@linemid}
+\setlength{\beamer@decolines@linemid}{.015\paperheight}
+\newlength{\beamer@decolines@linebottom}
+\setlength{\beamer@decolines@linebottom}{.01\paperheight}
+
+% The height of the watermark part below the 3 bottom lines.
+\newlength{\beamer@decolines@watermarkheightbottom}
+\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup}
+\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid}
+\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom}
+
+% The height of the watermark part over the 3 bottom lines before shrinking.
+\newlength{\beamer@decolines@watermarkheightupperorig}
+\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight}
+\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom}
+\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult
+
+% % Footer.
+% \defbeamertemplate*{footline}{decolines theme}
+% {
+%   \leavevmode%
+%   % Page number.
+%   \hbox{%
+%   \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}%
+%     \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber%
+%   \end{beamercolorbox}%
+%   \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}%
+%   \end{beamercolorbox}%
+%   } %
+%   % First line.
+%   \hbox{%
+%   \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}%
+%   \end{beamercolorbox}%
+%   \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}%
+%   \end{beamercolorbox}%
+%   } %
+%   % Second line.
+%   \hbox{%
+%   \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}%
+%   \end{beamercolorbox}%
+%   } %
+%   % Third line.
+%   \hbox{%
+%   \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}%
+%   \end{beamercolorbox}%
+%   \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}%
+%   \end{beamercolorbox}%
+%   }%
+%   % This seems to fix some alignment problems with the watermark. It has to be
+%   % always applied if you do not want to see the footer moving up and down when
+%   % moving from a page with watermark to a page without or vice versa.
+%   \vskip-.5px%
+%   % Watermark.
+%   \if\beamer@decolines@watermark\@empty\else%
+%     \vskip-\beamer@decolines@watermarkheightbottom%
+%     \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,%
+%       trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}%
+%   \fi%
+% }
+
+\defbeamertemplate*{headline}{decolines theme}
+{
+  \leavevmode%
+  \hbox{%
+  \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}%
+  \end{beamercolorbox}%
+  } %
+  \vskip0pt%
+}
+
+\defbeamertemplate*{frametitle}{decolines theme}[1][left]
+{
+  \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}%
+  \@tempdima=\textwidth%
+  \advance\@tempdima by\beamer@leftmargin%
+  \advance\@tempdima by\beamer@rightmargin%
+  \vbox{}\vskip-.5\beamer@leftmargin%
+  \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{}
+    \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}%
+    \vbox{}\vskip0ex%
+    \if@tempswa\else\csname beamer@fte#1\endcsname\fi%
+    \strut\insertframetitle\strut\par%
+    {%
+      \ifx\insertframesubtitle\@empty%
+      \else%
+      {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}%
+      \fi
+    }%
+    \vskip-1ex%
+    \if@tempswa\else\vskip-\beamer@leftmargin\fi
+  \end{beamercolorbox}%
+  \def\beamer@decolines@truetext{true}%
+  \ifx\beamer@decolines@titleline\beamer@decolines@truetext%
+    \vskip-.5\beamer@leftmargin%
+    \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}%
+    \end{beamercolorbox}%
+  \fi
+}
+
+% Frame title continuations, default
+\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)}
+
+
+
+\defbeamertemplate*{sidebar right}{decolines theme}
+{
+  \vskip.1\beamer@leftmargin%
+  \llap{\insertlogo\hskip.5\beamer@leftmargin}%
+  \vfill%
+  \if\beamer@decolines@watermark\@empty\else%
+  \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}%
+  \vskip-\beamer@decolines@watermarkheightbottom%
+  \fi
+}
+
+\mode
+<all>
diff --git a/KEK_Workshop_2015/beamerthemeFlip.sty b/KEK_Workshop_2015/beamerthemeFlip.sty
new file mode 100755
index 0000000..a615ff5
--- /dev/null
+++ b/KEK_Workshop_2015/beamerthemeFlip.sty
@@ -0,0 +1,59 @@
+% Main style file for the BEAMER FLIP THEME 2012
+% Copyright 2012 by Flip Tanedo
+% This file may be distributed and/or modified
+% 	1. under the LaTeX Project Public License and/or
+% 	2. under the GNU Public License.
+%
+% Comments: This is still a work in progress.
+% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html
+
+% \usepackage{beamerthemesplit}
+\mode<presentation>
+
+
+%% These are the options that are fed in through the driver file
+%% Some of them get passed on to the other theme files
+\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}}
+\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}}
+\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}}
+\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}}
+
+\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}}
+
+\ProcessOptionsBeamer
+
+\useinnertheme{Flip}	% Calls beamerinnerthemeFlip.sty
+\useoutertheme{Flip}	% Calls beamerouterthemeFlip.sty
+\usecolortheme{Flip}	% Calls beamercolorthemeFlip.sty
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%
+% Background  Gradient %
+%%%%%%%%%%%%%%%%%%%%%%%%
+
+
+%% Usually I would leave this on
+%% However, there seems to be problems with XeLaTeX
+%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds
+\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white]
+
+%% HOWEVER: it seems to make it impossible to change this later on in the document
+
+
+%% For a dark background: 
+% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop]
+
+
+%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2}
+%% In general: you want the gradient to be subtle!
+
+
+%%%%%%%%%%%%%%%%%%%%%%%
+% Navigation  symbols %
+%%%%%%%%%%%%%%%%%%%%%%%
+
+\setbeamertemplate{navigation symbols}{} 	% Turns off PDF navigation symbols
+
+\mode<all>
+\endinput
\ No newline at end of file
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+#!/bin/bash
+#FILES=*.pdf
+FILES="$(find . -name '*.pdf')"
+for f in $FILES
+do
+	echo "Processing $f ..."
+	gs -sDEVICE=pdfwrite -dCompatibilityLevel=1.4 -dUseCIEColor -dPDFSETTINGS=/printer -dSAFER -dNOPAUSE -dQUIET -dBATCH -sOutputFile="temp.pdf" "$f"
+	mv temp.pdf "$f"
+#	pdf2ps "$f" temp.ps
+#	ps2pdf temp.ps "$f"
+#	rm temp.ps
+done
+#rm temp.pdf
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@@ -0,0 +1,4 @@
+kinit egraveri@CERN.CH
+aklog
+cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0Align ./img/
+cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0AlignNoTT ./img/
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+<?xml version="1.0" encoding="UTF-8" standalone="no"?>
+<!-- Created with Inkscape (http://www.inkscape.org/) -->
+
+<svg
+   xmlns:dc="http://purl.org/dc/elements/1.1/"
+   xmlns:cc="http://creativecommons.org/ns#"
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+   xmlns:svg="http://www.w3.org/2000/svg"
+   xmlns="http://www.w3.org/2000/svg"
+   xmlns:sodipodi="http://sodipodi.sourceforge.net/DTD/sodipodi-0.dtd"
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+   id="svg2"
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+   sodipodi:docname="lhcb-logo2.pdf"><metadata
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+    \draw[crimsonred] ([yshift=-23.5pt]current page.north west)
+             -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}}
+
+
+
+% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % %
+\usepackage{tikzfeynman}		% For Feynman diagrams
+\usetikzlibrary{arrows,shapes}
+\usetikzlibrary{trees}
+\usetikzlibrary{matrix,arrows} 				% For commutative diagram
+% http://www.felixl.de/commu.pdf
+\usetikzlibrary{positioning}				% For "above of=" commands
+\usetikzlibrary{calc,through}				% For coordinates
+\usetikzlibrary{decorations.pathreplacing}  % For curly braces
+% http://www.math.ucla.edu/~getreuer/tikz.html
+\usepackage{pgffor}							% For repeating patterns
+
+\usetikzlibrary{decorations.pathmorphing}	% For Feynman Diagrams
+\usetikzlibrary{decorations.markings}
+\tikzset{
+	% >=stealth', %%  Uncomment for more conventional arrows
+	vector/.style={decorate, decoration={snake}, draw},
+	provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw},
+	antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw},
+	fermion/.style={draw=gray, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}},
+	fermionbar/.style={draw=gray, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}},
+	fermionnoarrow/.style={draw=gray},
+	gluon/.style={decorate, draw=black,
+		decoration={coil,amplitude=4pt, segment length=5pt}},
+	scalar/.style={dashed,draw=black, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}},
+	scalarbar/.style={dashed,draw=black, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}},
+	scalarnoarrow/.style={dashed,draw=black},
+	electron/.style={draw=black, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}},
+	bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw},
+}
+
+% TIKZ - for block diagrams, 
+% from http://www.texample.net/tikz/examples/control-system-principles/
+% \usetikzlibrary{shapes,arrows}
+\tikzstyle{block} = [draw, rectangle, 
+minimum height=3em, minimum width=6em]
+
+
+
+
+\usetikzlibrary{backgrounds}
+\usetikzlibrary{mindmap,trees}	% For mind map
+\newcommand{\degree}{\ensuremath{^\circ}}
+\newcommand{\E}{\mathrm{E}}
+\newcommand{\Var}{\mathrm{Var}}
+\newcommand{\Cov}{\mathrm{Cov}}
+\newcommand\Ts{\rule{0pt}{2.6ex}}       % Top strut
+\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut
+
+\graphicspath{{images/}}	% Put all images in this directory. Avoids clutter.
+
+% SOME COMMANDS THAT I FIND HANDY
+% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec
+\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild
+\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold
+\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold
+\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert
+\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert
+%% "\alert" is already a beamer pre-defined
+\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}%
+
+\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}}
+
+\usepackage{gmp}
+\usepackage[final]{feynmp-auto}
+
+\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex}
+\bibliography{bib}
+\setbeamertemplate{bibliography item}[text]
+
+\makeatletter\let\frametextheight\beamer@frametextheight\makeatother
+
+% suppress frame numbering for backup slides
+% you always need the appendix for this!
+\newcommand{\backupbegin}{
+	\newcounter{framenumberappendix}
+	\setcounter{framenumberappendix}{\value{framenumber}}
+}
+\newcommand{\backupend}{
+	\addtocounter{framenumberappendix}{-\value{framenumber}}
+	\addtocounter{framenumber}{\value{framenumberappendix}} 
+}
+
+
+\definecolor{links}{HTML}{2A1B81}
+%\hypersetup{colorlinks,linkcolor=,urlcolor=links}
+
+% For shapo's formulas:
+\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}}
+\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}}
+\newcommand{\lsim}{\mathop{\lsi}}
+\newcommand{\gsim}{\mathop{\gsi}}
+\newcommand{\wt}{\widetilde}
+%\newcommand{\ol}{\overline}
+\newcommand{\Tr}{\rm{Tr}}
+\newcommand{\tr}{\rm{tr}}
+\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&}
+\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}}
+\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}}
+\newcommand{\eV}{\rm{eV}}
+\newcommand{\keV}{\rm{keV}}
+\newcommand{\GeV}{\rm{GeV}}
+\newcommand{\MeV}{\rm{MeV}}
+\newcommand{\im}{\rm{Im}}
+\newcommand{\re}{{\rm Re}}
+\newcommand{\invfb}{\rm{fb^{-1}}}
+\newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}}
+\newcommand{\thetal}{\theta_l}
+\newcommand{\thetak}{\theta_k}
+\newcommand{\nn}{\nonumber}
+\newcommand{\eq}[1]{\begin{equation} #1 \end{equation}}
+%\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}}
+\newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}}
+\newcommand{\apeL}{{A_\perp^L}}
+\newcommand{\apeR}{{A_\perp^R}}
+\newcommand{\apeLR}{{A_\perp^{L,R}}}
+\newcommand{\apaL}{{A_\|^L}}
+\newcommand{\apaR}{{A_\|^R}}
+\newcommand{\apaLR}{{A_\|^{L,R}}}
+\newcommand{\azeL}{{A_0^L}}
+\newcommand{\azeR}{{A_0^R}}
+\newcommand{\azeLR}{{A_0^{L,R}}}
+\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace}
+\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace}
+
+\renewcommand{\C}[1]{{\cal C}_{#1}}
+\newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}}
+\newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}}
+\newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}}
+\def\FL       {\ensuremath{F_{\mathrm{L}}}\xspace}
+\def\ATDPH    {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace}
+\def\ATImPH     {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace}
+\def\ATRePH     {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace}
+\def\FLPH      {\ensuremath{F_{\mathrm{L,PR}}}\xspace}
+\def\ATDKG    {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace}
+\def\ATImKG     {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace}
+\def\ATReKG     {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace}
+\def\FLKG       {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace}
+\def\ATD     {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace}
+\def\ATIm     {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace}
+\def\ATRe     {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace}
+
+
+
+\newcommand{\disp}{\displaystyle}
+\def\be{\begin{equation}}
+\def\ee{\end{equation}}
+\def\ba{\begin{eqnarray}}
+\def\ea{\end{eqnarray}}
+\def\d{\partial}
+\def\l{\left(}
+\def\r{\right)}
+\def\la{\langle}
+\def\ra{\rangle}
+\def\e{{\rm e}}
+\def\Br{{\rm Br}}
+
+
+
+\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich)}
+\institute{UZH}
+\title[$\PBzero \to \PKstar \Pmuon \APmuon$ update]{$\PBzero \to \PKstar \Pmuon \APmuon$ update}
+\date{25 September 2014}
+
+
+\begin{document}
+\tikzstyle{every picture}+=[remember picture]
+
+{
+\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}}
+\begin{frame}[c]%{\phantom{title page}}
+\begin{center}
+\begin{center}
+  \begin{columns}
+    \begin{column}{0.9\textwidth}
+      \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Electroweak penguin measurements}
+      \end{column}
+    \begin{column}{0.2\textwidth}
+        %\includegraphics[width=\textwidth]{SHiP-2}
+      \end{column}
+    \end{columns}
+\end{center}
+\quad
+\vspace{3em}
+\begin{columns}
+\begin{column}{0.44\textwidth}
+\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}}
+
+\end{column}
+\begin{column}{0.53\textwidth}
+\includegraphics[height=1.3cm]{uzh-transp}
+\end{column}
+\end{columns}
+
+\vspace{1em}
+%\footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\
+\vspace{0.5em}
+\textcolor{normal text.fg!50!Comment}{$5^{th}$ KEK Flavour Factory Workshop \\October 26-27, 2015}
+\end{center}
+\end{frame}
+}
+
+\iffalse
+
+\begin{frame}{Outline}
+
+  \begin{minipage}{\textwidth}
+
+\begin{enumerate}
+\item Why flavour is important.
+\item $\Pbeauty \to \Pstrange \ell \ell$ theory in a nutshell.
+\item LHCb measurements of $\Pbeauty \to \Pstrange \ell \ell$.
+\item Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements.
+\item Conclusions.
+\end{enumerate}
+
+
+\end{minipage}
+  \vspace*{2.cm}
+\end{frame}
+
+\fi
+
+
+
+
+\begin{frame}
+\only<1>{\frametitle{LHCb detector - tracking}
+\begin{columns}
+\column{3in}
+\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg}
+
+\column{2in}
+\includegraphics[width=0.95\textwidth]{images/sketch.png}
+\end{columns}
+\begin{itemize}
+\item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\
+$\Rightarrow$ Identify secondary vertices from heavy flavour decays
+\item Proper time resolution $\sim~40~\rm fs$.\\
+$\Rightarrow$ Good separation of primary and secondary vertices.
+\item Excellent momentum ($\delta p/p \sim 0.4 - 0.6\%$) and inv. mass resolution.\\
+$\Rightarrow$ Low combinatorial background.
+
+\end{itemize}
+
+
+}
+
+\only<2>{\frametitle{LHCb detector - particle identification}
+\begin{columns}
+\column{3in}
+\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg}
+
+\column{2in}
+\includegraphics[width=0.95\textwidth]{images/cher.png}
+\end{columns}
+\begin{itemize}
+\item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$
+\item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$,  $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\
+$\Rightarrow$ Reject peaking backgrounds.
+\item High trigger efficiencies, low momentum thresholds.
+Muons: $p_T > 1.76 \GeV$ at L0, $p_T > 1.0 \GeV$ at HLT1,\\
+$B \to \PJpsi X $: Trigger $\sim 90\%$.
+
+\end{itemize}
+
+
+}
+
+
+\end{frame}
+
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Recent measurements}
+{~}
+\only<1>{
+
+  \begin{minipage}{\textwidth}
+
+
+\begin{columns}
+
+\column{0.5\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Branching fractions:}}
+\begin{description}
+\item [$\PB^{0,\pm} \to \PK^{0,\pm} \Pmuon \APmuon$] {~}{~}LHCb, Mar 14
+\item [$\PB^{0} \to \PKstar \Pmuon \APmuon$] {~}{~}CMS, Jul 15
+\item [$\PBs \to \Pphi \Pmuon \APmuon$] {~}{~}{~}LHCb, Jun 15
+\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}LHCb, Sep 15
+\item [$\PLambdab \to \PLambda  \Pmuon \APmuon$] {~}{~}{~}{~}LHCb, Mar 15
+\item [$\PB \to\Pmuon \APmuon$] {~}{~}{~}{~}{~}CMS+LHCb, Jun 15
+\end{description}
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{CP asymmetry:}}
+\begin{description}
+\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}{~}LHCb, Sep 15
+\end{description}
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Isospin asymmetry:}}
+\begin{description}
+\item [$\PB \to \PK \Pmuon \APmuon$] {~}{~}{~}{~}{~}LHCb, Mar 14
+\end{description}
+
+
+\column{0.5\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Lepton Universality:}}
+\begin{description}
+\item [$\PB^{\pm} \to \PK^{\pm} \Plepton \APlepton$] {~}{~}LHCb, Jun 14
+\end{description}
+
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Angular:}}
+\begin{description}
+\item [$\PB^{0} \to \PK^{\ast} \Plepton \APlepton$] {~}{~}{~}LHCb, Jan 15
+\item [$\PB^{\pm} \to \PK^{\ast,\pm} \Plepton \APlepton$] BaBar, Aug 15
+\item [$\PBs \to \Pphi \Plepton \APlepton$] {~}{~}{~}LHCb, Jun 15
+\item [$\PLambdab \to \PLambda  \Pmuon \APmuon$] {~}{~}LHCb, Mar 15
+\end{description}
+
+
+
+
+
+\end{columns}
+
+\end{minipage}
+}
+\only<2>{
+
+  \begin{minipage}{\textwidth}
+
+
+\begin{columns}
+
+\column{0.5\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Branching fractions:}}
+\begin{description}
+\item [{\color{red}{$\PB^{0,\pm} \to \PK^{0,\pm} \Pmuon \APmuon$}}] {~}{~}{\color{red}{LHCb, Mar 14}}
+\item [$\PB^{0} \to \PKstar \Pmuon \APmuon$] {~}{~}CMS, Jul 15
+\item [{\color{red}{$\PBs \to \Pphi \Pmuon \APmuon$}}] {~}{~}{~}{\color{red}{LHCb, Jun 15}}
+\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}LHCb, Sep 15
+\item [$\PLambdab \to \PLambda  \Pmuon \APmuon$] {~}{~}{~}{~}LHCb, Mar 15
+\item [{\color{red}{$\PB \to\Pmuon \APmuon$}}] {~}{~}{~}{~}{~}{\color{red}{CMS+LHCb, Jun 15}}
+\end{description}
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{CP asymmetry:}}
+\begin{description}
+\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}{~}LHCb, Sep 15
+\end{description}
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Isospin asymmetry:}}
+\begin{description}
+\item [$\PB \to \PK \Pmuon \APmuon$] {~}{~}{~}{~}{~}LHCb, Mar 14
+\end{description}
+
+
+\column{0.5\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Lepton Universality:}}
+\begin{description}
+\item [{\color{red}{$\PB^{\pm} \to \PK^{\pm} \Plepton \APlepton$}}] {~}{~}{\color{red}{LHCb, Jun 14}}
+\end{description}
+
+
+$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Angular:}}
+\begin{description}
+\item [{\color{red}{$\PB^{0} \to \PK^{\ast} \Plepton \APlepton$}}] {~}{~}{~}LHCb, Jan 15
+\item [{\color{red}{$\PB^{\pm} \to \PK^{\ast,\pm} \Plepton \APlepton$}}] {\color{red}{BaBar, Aug 15}}
+\item [$\PBs \to \Pphi \Plepton \APlepton$] {~}{~}{~}LHCb, Jun 15
+\item [{\color{red}{$\PLambdab \to \PLambda  \Pmuon \APmuon$}}] {~}{~}{\color{red}{LHCb, Mar 15}}
+\end{description}
+
+\begin{alertblock}{}
+$>2~\sigma$ deviations from SM
+
+\end{alertblock}
+
+\end{columns}
+
+\end{minipage}
+}
+
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics}
+{~}
+\begin{minipage}{\textwidth}
+
+$\color{JungleGreen}{\Rrightarrow}$ The kinematics of $\PBzero \to \PKstar \Pmuon \APmuon$ decay is described by three angles $\thetal$, $\thetak$, $\phi$ and invariant mass of the dimuon system ($q^2)$.
+
+  \only<1>{
+\begin{columns}
+\column{0.5\textwidth}
+
+$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetak$: the angle between the direction of the kaon in the $\PKstar$ ($\overline{\PKstar}$) rest frame and the direction of the $\PKstar$ ($\overline{\PKstar}$) in the $\PBzero$ ($\APBzero$) rest frame.\\
+$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetal$: the angle between the direction of the $\Pmuon$ ($\APmuon$) in the dimuon rest frame and the direction of the dimuon in the $\PBzero$ ($\APBzero$) rest frame.\\
+$\color{JungleGreen}{\Rrightarrow}$ $\phi$: the angle between the plane containing the $\Pmuon$ and $\APmuon$ and the plane containing the kaon and pion from the $\PKstar$.
+
+
+
+\column{0.5\textwidth}
+\includegraphics[width=0.95\textwidth]{images/angles.png}
+
+\end{columns}
+}
+  \only<2>{
+{\tiny{
+\eqa{\label{dist}
+\frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi}&=&\frac9{32\pi} \bigg[
+J_{1s} \sin^2\theta_K + J_{1c} \cos^2\theta_K + (J_{2s} \sin^2\theta_K + J_{2c} \cos^2\theta_K) \cos 2\theta_l\nn\\[1.5mm]
+&&\hspace{-2.7cm}+ J_3 \sin^2\theta_K \sin^2\theta_l \cos 2\phi + J_4 \sin 2\theta_K \sin 2\theta_l \cos\phi  + J_5 \sin 2\theta_K \sin\theta_l \cos\phi \nn\\[1.5mm]
+&&\hspace{-2.7cm}+ (J_{6s} \sin^2\theta_K +  {J_{6c} \cos^2\theta_K})  \cos\theta_l
++ J_7 \sin 2\theta_K \sin\theta_l \sin\phi  + J_8 \sin 2\theta_K \sin 2\theta_l \sin\phi \nn\\[1.5mm]
+&&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,,
+}
+}}
+$\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay.\\
+$\color{JungleGreen}{\Rrightarrow}$ The $CP$ averaged angular observables are defined:\\
+\eq{
+S_i = \dfrac{J_i+ \bar{J}_i}{(d \Gamma + d \bar{\Gamma})/dq^2}
+}
+
+}
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Transversity amplitudes }
+{~}
+\begin{minipage}{\textwidth}
+
+$\color{JungleGreen}{\Rrightarrow}$ One can link the angular observables to transversity amplitudes
+{\tiny{
+\eqa{
+J_{1s}  & = & \frac{(2+\beta_\ell^2)}{4} \left[|\apeL|^2 + |\apaL|^2 +|\apeR|^2 + |\apaR|^2 \right]
+    + \frac{4 m_\ell^2}{q^2} \re\left(\apeL\apeR^* + \apaL\apaR^*\right)\,,\nn\\[1mm]
+%
+J_{1c}  & = &  |\azeL|^2 +|\azeR|^2  + \frac{4m_\ell^2}{q^2} \left[|A_t|^2 + 2\re(\azeL^{}\azeR^*) \right] + \beta_\ell^2\, |A_S|^2 \,,\nn\\[1mm]
+%
+J_{2s} & = & \frac{ \beta_\ell^2}{4}\left[ |\apeL|^2+ |\apaL|^2 + |\apeR|^2+ |\apaR|^2\right],
+\hspace{0.92cm}    J_{2c}  = - \beta_\ell^2\left[|\azeL|^2 + |\azeR|^2 \right]\,,\nn\\[1mm]
+%
+J_3 & = & \frac{1}{2}\beta_\ell^2\left[ |\apeL|^2 - |\apaL|^2  + |\apeR|^2 - |\apaR|^2\right],
+\qquad   J_4  = \frac{1}{\sqrt{2}}\beta_\ell^2\left[\re (\azeL\apaL^* + \azeR\apaR^* )\right],\nn \\[1mm]
+%
+J_5 & = & \sqrt{2}\beta_\ell\,\Big[\re(\azeL\apeL^* - \azeR\apeR^* ) - \frac{m_\ell}{\sqrt{q^2}}\,
+\re(\apaL A_S^*+ \apaR^* A_S) \Big]\,,\nn\\[1mm]
+%
+J_{6s} & = &  2\beta_\ell\left[\re (\apaL\apeL^* - \apaR\apeR^*) \right]\,,
+\hspace{2.25cm} J_{6c} = 4\beta_\ell\, \frac{m_\ell}{\sqrt{q^2}}\, \re (\azeL A_S^*+ \azeR^* A_S)\,,\nn\\[1mm]
+%
+J_7 & = & \sqrt{2} \beta_\ell\, \Big[\im (\azeL\apaL^* - \azeR\apaR^* ) +
+\frac{m_\ell}{\sqrt{q^2}}\, \im (\apeL A_S^* - \apeR^* A_S)) \Big]\,,\nn\\[1mm]
+%
+J_8 & = & \frac{1}{\sqrt{2}}\beta_\ell^2\left[\im(\azeL\apeL^* + \azeR\apeR^*)\right]\,,
+%
+\hspace{1.9cm} J_9 = \beta_\ell^2\left[\im (\apaL^{*}\apeL + \apaR^{*}\apeR)\right] \,,
+\label{Js}}
+}}
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Link to effective operators}
+{~}
+\begin{minipage}{\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ So here is where the magic happens. At leading order the amplitudes can be written as:
+{\tiny{
+\eqa{
+\apeLR &=&\sqrt{2} N m_B(1- \hat s)\bigg[  (\Ceff9 + \Cpeff9) \mp (\C{10} + \Cp{10})
++\frac{2\hat{m}_b}{\hat s} (\Ceff7 + \Cpeff7) \bigg]\xi_{\bot}(E_{K^*})  \nn \\[2mm]
+\apaLR &=& -\sqrt{2} N m_B (1-\hat s)\bigg[(\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10})
++\frac{2\hat{m}_b}{\hat s}(\Ceff7 - \Cpeff7) \bigg] \xi_{\bot}(E_{K^*}) \nn \\[2mm]
+\azeLR  &=& -\frac{N m_B (1-\hat s)^2}{2 \hat{m}_{K^*} \sqrt{\hat s}} \bigg[ (\Ceff9 - \Cpeff9)  \mp (\C{10} - \Cp{10}) + 2\hat{m}_b (\Ceff7 - \Cpeff7) \bigg]\xi_{\|}(E_{K^*}),
+\label{LargeRecoilAs}}
+}}
+where $\hat s = q^2 /m_B^2$, $\hat{m}_i = m_i/m_B$. The $\xi_{\|,\bot }$ are the form factors. \\
+\pause
+$\color{JungleGreen}{\Rrightarrow}$ Now we can construct observables that cancel the $\xi$ form factors at leading order:
+\eq{P_5^{\prime} = \dfrac{J_5+\bar{J}_5}{2\sqrt{-(J_2^c+\bar{J}_2^c)(J_2^s+\bar{J}_2^s)} }
+}
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+% symmetries
+\begin{frame}{Symmetries in $\PB \to \PKstar \Pmu \Pmu$}
+{~}
+\begin{minipage}{\textwidth}
+$\color{JungleGreen}{\Rrightarrow}$ Eq.~\ref{dist} has 12 angular coefficients.\\
+$\color{JungleGreen}{\Rrightarrow}$ There exists 4 symmetry transformations that leave the angular distributions non changed:
+\begin{tiny}
+\eq{
+n_\|=\binom{A_\|^L}{A_\|^{R*}}\ ,\quad
+n_\bot=\binom{A_\bot^L}{-A_\bot^{R*}}\ ,\quad
+n_0=\binom{A_0^L}{A_0^{R*}}\ .
+}
+\end{tiny}
+\begin{tiny}
+\eq{
+  n_i^{'} = U n_i=
+  \left[
+    \begin{array}{ll}
+      e^{i\phi_L} & 0 \\
+      0 & e^{-i \phi_R}
+    \end{array}
+  \right]
+  \left[
+    \begin{array}{rr}
+      \cos \theta & -\sin \theta \\
+      \sin \theta &  \cos \theta
+    \end{array}
+  \right]
+  \left[
+    \begin{array}{rr}
+      \cosh i \tilde{\theta} &  -\sinh i \tilde{\theta} \\
+      - \sinh i \tilde{\theta} & \cosh i \tilde{\theta}
+    \end{array}
+  \right]
+  n_i \,.
+ \label{symmassless}}
+\end{tiny}
+$\color{JungleGreen}{\Rrightarrow}$ Using this symmetries one can show that there are 8 independent observables. The pdf can be wrote as:
+\begin{tiny}
+\begin{align}                                                                                                                                                                                                                                                                                                                 
+\left.\frac{1}{{\rm d}(\Gamma+\bar{\Gamma})/{\rm d}q^2}\frac{{\rm d}(\Gamma+\bar{\Gamma})}{{\rm dcos}\thetal\,{\rm dcos}\thetak\,{\rm d}\phi}\right|_{\rm P} =                                                                                                                                                                
+\tfrac{9}{32\pi}\bigl[                                                                                                                                                                                                                                                                                                        
+&\tfrac{3}{4} (1-{F_{\rm L}})\sin^2\thetak \label{eq:pdfpwave}\\[-0.75em]                                                                                                                                                                                                                                                     
+&+ {F_{\rm L}}\cos^2\thetak + \tfrac{1}{4}(1-{F_{\rm L}})\sin^2\thetak\cos 2\thetal\nonumber\\                                                                                                                                                                                                                                
+&- {F_{\rm L}} \cos^2\thetak\cos 2\thetal + {S_3}\sin^2\thetak \sin^2\thetal \cos 2\phi\nonumber\\                                                                                                                                                                                                                            
+&+ {S_4} \sin 2\thetak \sin 2\thetal \cos\phi + {S_5}\sin 2\thetak \sin \thetal \cos \phi\nonumber\\                                                                                                                                                                                                                          
+&+ \tfrac{4}{3} {A_{\rm FB}} \sin^2\thetak \cos\thetal + {S_7} \sin 2\thetak \sin\thetal \sin\phi\nonumber\\                                                                                                                                                                                                                  
+&+ {S_8} \sin 2\thetak \sin 2\thetal \sin\phi + {S_9}\sin^2\thetak \sin^2\thetal \sin 2\phi \nonumber                                                                                                                                                                                                                         
+\bigr].                                                                                                                                                                                                                                                                                                                       
+%\end{split}                                                                                                                                                                                                                                                                                                                  
+%\bigr],                                                                                                                                                                                                                                                                                                                      
+\end{align} 
+\end{tiny}
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+
+
+
+
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{LHCb update of the $\PBzero \to \PKstar \Pmuon \APmuon$, Selection}
+{~}
+\begin{minipage}{\textwidth}
+\begin{columns}
+
+\column{0.5\textwidth}
+\begin{itemize}
+\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background.
+\item Reject the regions of $\PJpsi$ and $\Ppsi(2S)$.
+\item Specific vetos for backgrounds: $\PLambdab \to \Pproton \PK \Pmu \Pmu$, $\PBs \to \Pphi \Pmu \Pmu$, etc.
+\item Using k-Fold technique and signal proxy $\PB \to \PJpsi \PKstar$ for training the BDT.
+\item Improved selection allowed for finer binning than the $1\invfb$ analysis.
+\end{itemize}
+
+
+\column{0.5\textwidth}
+
+\includegraphics[width=0.88\textwidth]{images/Fig1.pdf} \\
+\includegraphics[width=0.88\textwidth]{images/fold.png}
+
+\end{columns}
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{LHCb update of the $\PBzero \to \PKstar \Pmuon \APmuon$, Selection}
+{~}
+\begin{minipage}{\textwidth}
+
+\begin{itemize}
+\item Signal modelled by a sum of two Crystal-Ball functions.
+\item Shape is defined using $\PB \to \PJpsi \PKstar$ and corrected for $q^2$ dependency.
+\item Combinatorial background modelled by exponent.
+\end{itemize}
+
+\begin{columns}
+\column{0.5\textwidth}
+\begin{itemize}
+\item $\PK \Ppi$ system:
+\begin{itemize}
+\item Rel. Breit Wigner for P-wave
+\item Lass model for the S-wave.
+\item Linear model for background.
+\end{itemize}
+\end{itemize}
+
+\column{0.5\textwidth}
+
+\includegraphics[width=0.88\textwidth]{images/pbkg}
+
+\end{columns}
+
+\begin{large}
+\begin{itemize}
+\item In total we found $2398\pm57$ candidates in the $(0.1,19)~\GeV^2$ $q^2$ region.
+\item $624 \pm 30$ candidates in the theoretically the most interesting $(1.1-6.0)~\GeV^2$ region.
+\end{itemize}
+\end{large}
+
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Detector acceptance}
+{~}
+\begin{minipage}{\textwidth}
+\begin{columns}
+
+\column{0.6\textwidth}
+\begin{itemize}
+\item Detector distorts our angular distribution.
+\item We need to model this effect.
+\item 4D function is used:
+\begin{align*}
+\epsilon (\cos \thetal, \cos \thetak, \phi, q^2) = \\\sum_{ijkl} c_{ijkl} P_i(\cos \thetal) P_j(\cos \thetak ) P_k(\phi) P_l(q^2),
+\end{align*}
+where $P_i$ is the Legendre polynomial of order $i$.
+\item We use up to $4^{th}, 5^{th}, 6^{th}, 5^{th}$ order for the $\cos \thetal, \cos \thetak, \phi, q^2$.
+\end{itemize}
+
+
+
+
+\column{0.4\textwidth}
+\includegraphics[width=0.99\textwidth]{images/det.png}
+\end{columns}
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Control channel}
+{~}
+\begin{minipage}{\textwidth}
+
+
+\begin{itemize}
+\item We tested our unfolding procedure on $\PB \to \PJpsi \PKstar$.
+\item The result is in perfect agreement with other experiments and our different analysis of this decay.
+\end{itemize}
+
+\begin{columns}
+
+\column{0.5\textwidth}
+
+\includegraphics[width=0.95\textwidth]{images/mlogjpsi.png}
+\column{0.5\textwidth}
+\includegraphics[width=0.95\textwidth]{images/mkpijpsi.png}
+
+\end{columns}
+
+
+\includegraphics[width=0.99\textwidth]{images/angles2.png}
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Results in $\PB \to \PKstar \Pmu \Pmu$}
+  \begin{minipage}{\textwidth}
+    \begin{center}
+      \includegraphics[angle=-90,width=0.65\textwidth]{images/Fig17.pdf}\\
+      \end{center}
+
+\begin{itemize}
+\item Tension with $3~\invfb$ gets confirmed!
+\item The two bins deviate both in $2.8~\sigma$ from SM prediction.
+\item Result compatible with previous result.
+\end{itemize}
+
+
+\end{minipage}
+  \vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Branching fraction measurements of $\PB \to \PKstar^{\pm} \Pmu \Pmu$}
+{~}
+\includegraphics[width=0.5\textwidth]{images/ksmumu_BF.png}
+\includegraphics[width=0.5\textwidth]{images/kmumu_BF.png}
+
+\begin{center}
+\begin{columns}
+
+\column{0.4\textwidth}
+\begin{itemize}
+\item Despite large theoretical errors the results are consistently smaller then SM prediction.
+\end{itemize}
+\column{0.6\textwidth}
+\includegraphics[width=0.87\textwidth]{images/bukst_BF.png}
+
+
+\end{columns}
+
+
+
+
+
+
+
+\end{center}
+\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Branching fraction measurements of $\PBs \to \Pphi \Pmu \Pmu$}
+{~}
+\begin{minipage}{\textwidth}
+  \begin{center}
+    \includegraphics[width=0.65\textwidth]{images/bs2phipi.png}\\
+    \end{center}
+
+\begin{itemize}
+\item Recent LHCb measurement [JHEPP09 (2015) 179].
+\item Suppressed by $\frac{f_s}{f_d}$.
+\item Cleaner because of narrow $\Pphi$ resonance.
+\item $3.3~\sigma$ deviation in SM in the $1-6\GeV^2$ bin.
+\end{itemize}
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$}
+{~}
+\begin{minipage}{\textwidth}
+
+  \begin{center}
+    \only<1>{
+      \includegraphics[width=0.65\textwidth]{images/Lb_BR.png}
+}
+    \only<2>{
+      \includegraphics[width=0.45\textwidth]{images/Lblow.png}
+\includegraphics[width=0.45\textwidth]{images/Lbhigh.png}
+
+}
+
+
+    \end{center}
+
+
+\begin{itemize}
+\item This years LHCb measurement [JHEP 06 (2015) 115]].
+\item In total $\sim 300$ candidates in data set.
+\item Decay not present in the low $q^2$.
+
+\end{itemize}
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$}
+{~}
+\begin{minipage}{\textwidth}
+
+\begin{itemize}
+\item For the bins in which we have $>3~\sigma$ significance the forward backward asymmetry for the hadronic and leptonic system.
+\end{itemize}
+\begin{center}
+\includegraphics[width=0.9\textwidth]{{images/AFB_Lb}.png}
+\end{center}
+\begin{itemize}
+\item $A_{FB}^H$ is in good agreement with SM.
+\item $A_{FB}^{\ell}$ always in above SM prediction.
+\end{itemize}
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Lepton universality test}
+{~}
+\begin{minipage}{\textwidth}
+\begin{columns}
+\column{3.0in}
+\begin{itemize}
+\item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours?
+\includegraphics[width=0.9\textwidth]{images/uni2.png}
+\item Challenging analysis due to bremsstrahlung.
+\item Migration of events modeled by MC.
+\item Correct for bremsstrahlung.
+\item Take double ratio with $\PBplus \to \PJpsi \PKplus$ to cancel systematics.
+\item In $3\invfb$, LHCb measures $R_K=0.745^{+0.090}_{-0.074}(stat.)^{+0.036}_{-0.036}(syst.)$
+\item Consistent with SM at $2.6\sigma$.
+
+\end{itemize}
+\column{2.0in}
+\includegraphics[width=0.99\textwidth]{images/RK.png}\\
+\begin{itemize}
+\item \href{http://arxiv.org/abs/1406.6482}{Phys. Rev. Lett. 113, 151601 (2014)}
+\end{itemize}
+\end{columns}
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$}
+{~}
+\only<1>{
+  \begin{minipage}{\textwidth}
+    \begin{itemize}
+      \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$.
+        \item Electrons channels are extremely challenging experimentally:
+          \begin{itemize}
+            \item Bremsstrahlung.
+              \item Trigger efficiencies.
+                \end{itemize}
+          \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$:
+            \end{itemize}
+\begin{equation}
+  \label{eq:physPars}
+  \begin{split}
+  \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\
+  \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\
+  \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\
+  \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2},
+\end{split}
+\end{equation}
+
+\end{minipage}
+}
+\only<2>{
+\begin{center}
+\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\
+\end{center}
+\begin{itemize}
+\item Results in full agreement with the SM.
+\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays.
+\end{itemize}
+
+\begin{center}
+\includegraphics[width=0.9\textwidth]{images/Kstee2.png}
+\end{center}
+
+}
+\vspace*{2.1cm}
+\end{frame}
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Theory implications}
+{~}
+\begin{minipage}{\textwidth}
+
+\begin{itemize}
+\item A preliminary fit prepared by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, presented at \href{http://arxiv.org/abs/1510.04239}{\color{blue}{1510.04239}}
+\item Took into the fit:
+\begin{itemize}
+\item $\mathcal{B} ( \PB \to X_s \Pphoton) = (3.36 \pm 0.23) \times 10^{-4} $, Misiak et. al. 2015.
+\item $\mathcal{B} ( \PB \to\Pmu \Pmu)$, theory: Bobeth et al 2013, experiment: LHCb+CMS average (2015)
+\item $\mathcal{B} ( \PB \to X_s \Pmu \Pmu$), Huber et al 2015
+\item $\mathcal{B} ( \PB \to \PK \Pmu \Pmu$),Bouchard et al 2013, 2015
+\item $PB_{(s)} \to \PKstar(\Pphi) \Pmu \Pmu$, Horgan et al 2013
+\item $\PB \to \PK \Pe \Pe$, $\PB \to \PKstar \Pe \Pe$ and $R_k$.
+\end{itemize}
+\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM.
+\end{itemize}
+
+
+
+
+
+\end{minipage}
+\vspace*{2.1cm}
+\end{frame}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{frame}{Theory implications}
+{~}
+\begin{minipage}{\textwidth}
+
+\begin{itemize}
+\item A preliminary fit prepared by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, presented at \href{http://arxiv.org/abs/1510.04239}{\color{blue}{1510.04239}}
+\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}{Theory implications}
+{~}
+        \begin{minipage}{\textwidth}
+
+\includegraphics[height=0.9\textheight]{images/table.png}
+
+
+\end{minipage}
+                \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>{
+\includegraphics[width=0.9\textwidth]{images/charmloop.png}
+}
+\only<2>{
+\begin{center}
+\includegraphics[width=0.6\textwidth]{images/charmloop2.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}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\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}
+
+
+
+\backupbegin
+
+\begin{frame}\frametitle{Backup}
+\topline
+
+\end{frame}
+
+\backupend
+
+
+\end{document}
diff --git a/KEK_Workshop_2015/mchrzasz.tex~ b/KEK_Workshop_2015/mchrzasz.tex~
new file mode 100644
index 0000000..82e90f7
--- /dev/null
+++ b/KEK_Workshop_2015/mchrzasz.tex~
@@ -0,0 +1,306 @@
+\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer}
+
+\usepackage[english]{babel} 
+\usepackage{polski}         
+
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+
+%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}}
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+\usepackage{tikz}
+
+%\usepackage{hepparticles}    
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+
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+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}},
+	scalarbar/.style={dashed,draw=black, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}},
+	scalarnoarrow/.style={dashed,draw=black},
+	electron/.style={draw=black, postaction={decorate},
+		decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}},
+	bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw},
+}
+
+% TIKZ - for block diagrams, 
+% from http://www.texample.net/tikz/examples/control-system-principles/
+% \usetikzlibrary{shapes,arrows}
+\tikzstyle{block} = [draw, rectangle, 
+minimum height=3em, minimum width=6em]
+
+
+
+
+\usetikzlibrary{backgrounds}
+\usetikzlibrary{mindmap,trees}	% For mind map
+\newcommand{\degree}{\ensuremath{^\circ}}
+\newcommand{\E}{\mathrm{E}}
+\newcommand{\Var}{\mathrm{Var}}
+\newcommand{\Cov}{\mathrm{Cov}}
+\newcommand\Ts{\rule{0pt}{2.6ex}}       % Top strut
+\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut
+
+\graphicspath{{images/}}	% Put all images in this directory. Avoids clutter.
+
+% SOME COMMANDS THAT I FIND HANDY
+% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec
+\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild
+\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold
+\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold
+\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert
+\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert
+%% "\alert" is already a beamer pre-defined
+\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}%
+
+\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}}
+
+\usepackage{gmp}
+\usepackage[final]{feynmp-auto}
+
+\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex}
+\bibliography{bib}
+\setbeamertemplate{bibliography item}[text]
+
+\makeatletter\let\frametextheight\beamer@frametextheight\makeatother
+
+% suppress frame numbering for backup slides
+% you always need the appendix for this!
+\newcommand{\backupbegin}{
+	\newcounter{framenumberappendix}
+	\setcounter{framenumberappendix}{\value{framenumber}}
+}
+\newcommand{\backupend}{
+	\addtocounter{framenumberappendix}{-\value{framenumber}}
+	\addtocounter{framenumber}{\value{framenumberappendix}} 
+}
+
+
+\definecolor{links}{HTML}{2A1B81}
+%\hypersetup{colorlinks,linkcolor=,urlcolor=links}
+
+% For shapo's formulas:
+\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}}
+\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}}
+\newcommand{\lsim}{\mathop{\lsi}}
+\newcommand{\gsim}{\mathop{\gsi}}
+\newcommand{\wt}{\widetilde}
+%\newcommand{\ol}{\overline}
+\newcommand{\Tr}{\rm{Tr}}
+\newcommand{\tr}{\rm{tr}}
+\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&}
+\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}}
+\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}}
+\newcommand{\eV}{\rm{eV}}
+\newcommand{\keV}{\rm{keV}}
+\newcommand{\GeV}{\rm{GeV}}
+\newcommand{\im}{\rm{Im}}
+\newcommand{\disp}{\displaystyle}
+\def\be{\begin{equation}}
+\def\ee{\end{equation}}
+\def\ba{\begin{eqnarray}}
+\def\ea{\end{eqnarray}}
+\def\d{\partial}
+\def\l{\left(}
+\def\r{\right)}
+\def\la{\langle}
+\def\ra{\rangle}
+\def\e{{\rm e}}
+\def\Br{{\rm Br}}
+
+
+
+\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich)}
+\institute{UZH}
+\title[$\PBzero \to \PKstar \Pmuon \APmuon$ update]{$\PBzero \to \PKstar \Pmuon \APmuon$ update}
+\date{25 September 2014}
+
+
+\begin{document}
+\tikzstyle{every picture}+=[remember picture]
+
+{
+\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}}
+\begin{frame}[c]%{\phantom{title page}} 
+\begin{center}
+\begin{center}
+	\begin{columns}
+		\begin{column}{0.75\textwidth}
+			\flushright\fontspec{Trebuchet MS}\bfseries \Huge {$\PBzero \to \PKstar \Pmuon \APmuon$ update}
+		\end{column}
+                \begin{column}{0.02\textwidth}
+                  {~}
+                  \end{column}
+                \begin{column}{0.23\textwidth}
+                 % \hspace*{-1.cm}
+                  \vspace*{-3mm}
+                  \includegraphics[width=0.6\textwidth]{lhcb-logo}
+                  \end{column}
+	        
+	\end{columns}
+\end{center}
+	\quad
+	\vspace{3em}
+\begin{columns}
+\begin{column}{0.44\textwidth}
+\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}}
+
+\end{column}
+\begin{column}{0.53\textwidth}
+\includegraphics[height=1.3cm]{uzh-transp}
+\end{column}
+\end{columns}
+
+\vspace{1em}
+%		\footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\
+\vspace{0.5em}
+
+	\textcolor{normal text.fg!50!Comment}{Zurich meeting, CERN\\September 24, 2014}
+\end{center}
+\end{frame}
+}
+
+
+\begin{frame}[c]{A short introduction to the $\nu$MSM}%{{\footnotesize\href{http://arxiv.org/abs/hep-ph/0503065}{[T. Asaka et al. 2005]}}}
+\topline
+	\begin{minipage}{\textwidth}
+\topline  
+	\begin{exampleblock}{}
+		Leptons and quarks get their mass through the Yukawa interaction:
+		\vspace*{-0.7em}\begin{align*}
+			\mathcal{L} = m\,\psi^\dagger_L\, h\, \psi_R + c.c.
+		\end{align*}
+	\end{exampleblock}
+	\begin{figure}
+		%		\centering
+		\flushleft
+		%\includegraphics<1-1>[width=0.48\textwidth]{img/neutrinos-sm}
+		%%\hfill
+		%\phantom{\includegraphics<1-1>[width=0.48\textwidth]{img/neutrinos-nusm}}
+		%\includegraphics<2-2>[width=0.48\textwidth]{img/neutrinos-nusm}		
+	\end{figure}
+	\only<1-2>{\Put(170,180){\begin{minipage}{0.45\textwidth}\vskip0pt plus 1filll
+			\Alert{\vskip0pt plus 1filll Neutrinos need a right-handed partner to get their masses like the other SM fermions!}
+			\newline{}%\vskip0pt plus 1filll
+			%\only<1-1>{\vskip0pt plus 1filll\phantom{An extra \ALERT{$N$} field could exist. It would be a $SU(2)$ singlet, as it is still unobserved.}}
+			%\only<2-2>{An extra \ALERT{$N$} field could exist. It would be a $SU(2)$ singlet, as it is still unobserved.}
+			\onslide<2-2>{Three extra \ALERT{$N$} field could exist (\Alert{\textit{sterile neutrinos}}). They would be $SU(2)$ singlets, as they are still unobserved.}
+	\end{minipage}}}
+%		\vskip0pt plus 1filll
+%		\only<1-1>{\phantom{
+%			\begin{align*}
+%			&\mathcal{L} = \bar{N_i}i\slashed\partial N_i - f_{i\alpha}H\bar{N_i}L_\alpha - \frac{M_i}{2}\bar{N_i}^c N_i + h.c.
+%			\end{align*}}}
+%				Sterile neutrinos would \Alert{mix to $\nu_{e,\mu,\tau}$} with very small couplings \Alert{$U^2_{e,\mu,\tau}$}.}}
+		\only<2-2>{
+\vspace{-0.5cm}
+			\begin{align*}
+				&\mathcal{L} = \mathcal{L}_{SM} \bar{N_i}i\slashed\partial N_i - f_{i\alpha}H\bar{N_i}L_{\alpha} - \frac{M_i}{2}\bar{N_i}^c N_i + h.c.
+			\end{align*}
+\kern-0.9em
+\ALERT{\textbf{Sterile neutrinos}} would \Alert{mix to $\nu_{e,\mu,\tau}$} with very small couplings \Alert{$U^2_{e,\mu,\tau}$}.
+		}
+	\end{minipage}
+		\vspace*{2.cm}
+\end{frame}
+
+\backupbegin   
+
+\begin{frame}\frametitle{Backup}
+\topline 
+
+\end{frame}
+
+\backupend			
+
+\end{document}
diff --git a/KEK_Workshop_2015/mchrzasz.toc b/KEK_Workshop_2015/mchrzasz.toc
new file mode 100644
index 0000000..429917f
--- /dev/null
+++ b/KEK_Workshop_2015/mchrzasz.toc
@@ -0,0 +1,5 @@
+\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax 
+\defcounter {refsection}{0}\relax 
+\beamer@endinputifotherversion {3.24pt}
+\defcounter {refsection}{0}\relax 
+\select@language {english}
diff --git a/KEK_Workshop_2015/tikzfeynman.sty b/KEK_Workshop_2015/tikzfeynman.sty
new file mode 100755
index 0000000..521fc65
--- /dev/null
+++ b/KEK_Workshop_2015/tikzfeynman.sty
@@ -0,0 +1,43 @@
+% Tikz Feynman Diagrams
+% by Flip Tanedo
+% 4 January 2011, work in progress
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%% TIKZ - for drawing Feynman diagrams %%%%
+%%% ... use with pdflatex   			%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\usepackage{tikz}
+\usetikzlibrary{arrows,shapes}
+\usetikzlibrary{trees}
+\usetikzlibrary{matrix,arrows} 				% For commutative diagram
+											% http://www.felixl.de/commu.pdf
+\usetikzlibrary{positioning}				% For "above of=" commands
+\usetikzlibrary{calc,through}				% For coordinates
+\usetikzlibrary{decorations.pathreplacing}  % For curly braces
+\usepackage[tikz]{bclogo} 					% For cute logo boxes
+\usepackage{pgffor}							% For repeating patterns
+
+\usetikzlibrary{decorations.pathmorphing}	% For Feynman Diagrams
+\usetikzlibrary{decorations.markings}
+\tikzset{
+	% >=stealth', %% Different kind of arrows
+    vector/.style={decorate, decoration={snake}, draw},
+    fermion/.style={postaction={decorate},
+        decoration={markings,mark=at position .55 with {\arrow{>}}}},
+    fermionbar/.style={draw, postaction={decorate},
+        decoration={markings,mark=at position .55 with {\arrow{<}}}},
+    fermionnoarrow/.style={},
+    gluon/.style={decorate,
+        decoration={coil,amplitude=4pt, segment length=5pt}},
+    scalar/.style={dashed, postaction={decorate},
+        decoration={markings,mark=at position .55 with {\arrow{>}}}},
+    scalarbar/.style={dashed, postaction={decorate},
+        decoration={markings,mark=at position .55 with {\arrow{<}}}},
+    scalarnoarrow/.style={dashed,draw},
+%
+%% 	Special vectors (when you need to fine-tune wiggles)
+	provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw},
+	antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw},
+}
+