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{69}} +\headcommand {\def \inserttotalframenumber {55}} diff --git a/Seminars/Padova/mchrzasz.pdf b/Seminars/Padova/mchrzasz.pdf index 3499f1b..a2ff1e5 100644 --- a/Seminars/Padova/mchrzasz.pdf +++ b/Seminars/Padova/mchrzasz.pdf Binary files differ diff --git a/Seminars/Padova/mchrzasz.snm b/Seminars/Padova/mchrzasz.snm index c9c08fe..fbfe156 100644 --- a/Seminars/Padova/mchrzasz.snm +++ b/Seminars/Padova/mchrzasz.snm @@ -1,3 +1,3 @@ -\beamer@slide {Js}{16} -\beamer@slide {LargeRecoilAs}{17} -\beamer@slide {eq:physPars}{50} +\beamer@slide {Js}{15} +\beamer@slide {LargeRecoilAs}{16} +\beamer@slide {eq:physPars}{49} diff --git a/Seminars/Padova/mchrzasz.synctex.gz b/Seminars/Padova/mchrzasz.synctex.gz index 8567562..e729282 100644 --- a/Seminars/Padova/mchrzasz.synctex.gz +++ b/Seminars/Padova/mchrzasz.synctex.gz Binary files differ diff --git a/Seminars/Padova/mchrzasz.tex b/Seminars/Padova/mchrzasz.tex index ecf6616..d1566cd 100644 --- a/Seminars/Padova/mchrzasz.tex +++ b/Seminars/Padova/mchrzasz.tex @@ -409,7 +409,7 @@ \item Cabibbo angle was successful in explaining dozens of decay rates in the 1960s. \item There was, however, one that was not observed by experiments: $\PKzero \to \Pmuon \APmuon$. -\item Glashow, Iliopoulos, Maiani (GIM) mechanism was proposed in the 1970 to fix this problem. The mechanism required the existence of the $4^{th}$ quark. +\item Glashow, Iliopoulos, Maiani (GIM) mechanism was proposed in the 1970 to fix this problem. The mechanism required the existence of a $4^{th}$ quark. \item At that point most of the people were skeptical about that. Fortunately in 1974 the discovery of the $\PJpsi$ meson silenced the skeptics. \end{footnotesize} \end{itemize} @@ -443,9 +443,9 @@ -\item Similarly CP violation was discovered in 1960s in the neutral kaons decays. +\item Similarly, CP violation was discovered in 1960s in the neutral kaons decays. \item $2 \times 2$ Cabbibo matrix could not allow for any CP violation. -\item For the CP violation to be possible one needs at least a $3 \times 3$ unitary matrix \\ $\looparrowright$ Cabibbo-Kobayashi-Maskawa matrix (1973). +\item For CP violation to be possible one needs at least a $3 \times 3$ unitary matrix \\ $\looparrowright$ Cabibbo-Kobayashi-Maskawa matrix (1973). \item It predicts existence of $\Pbottom$ (1977) and $\Ptop$ (1995) quarks. \end{small} @@ -481,7 +481,7 @@ \begin{small} -\item Weak neutral currents were first, introduced in 1958 by Buldman. +\item Weak neutral currents were first introduced in 1958 by Buldman. \item Later on they were naturally incorporated into unification of weak and electromagnetic interactions. \item 't Hooft proved that the GWS models was renormalizable. \item Everything was there on theory side, only missing piece was the experiment, till 1973. @@ -622,13 +622,13 @@ \begin{columns} \column{4in} \begin{itemize} -\item In SM allows only the charged interactions to change flavour. +\item The SM allows only the charged interactions to change flavour. \begin{itemize} \item Other interactions are flavour conserving. \end{itemize} -\item One can escape this constrain and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. \begin{itemize} -\item This kind of processes are suppressed in SM $\to$~Rare decays. +\item These kind of processes are suppressed in SM $\to$~Rare decays. \item New Physics can enter in the loops. \end{itemize} \end{itemize} @@ -643,7 +643,7 @@ \end{frame} - +\iffalse \begin{frame}{Tools in rare $\PBzero$ decays} {~} @@ -690,7 +690,7 @@ \vspace*{2.1cm} \end{frame} - +\fi \begin{frame}{Analysis of Rare decays} @@ -1017,7 +1017,7 @@ \begin{footnotesize} \item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. \item BDT with k-Folding technique. -\item Completely data drive. +\item Completely data driven. \end{footnotesize} \end{itemize} \begin{center} @@ -1045,11 +1045,11 @@ \begin{minipage}{\textwidth} \begin{footnotesize} -\ARROW BDT was also check in order not to bias our angular distribution: +\ARROW BDT was also checked in order not to bias our angular distribution: \begin{center} \includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} \end{center} -\ARROW The BDT has small impact on our angular observables. We will correct for this effects later on. +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. \end{footnotesize} \end{minipage} @@ -1060,15 +1060,15 @@ \begin{frame}{Mass modelling} {~} - \begin{minipage}{\textwidth} +\begin{minipage}{\textwidth} \begin{tiny} \begin{columns} \column{0.1in} {~} \column{2.5in} -\ARROW The signal is modelled by a sum of two Crystal-Ball function with common mean.\\ -\ARROW The background is a single exponent\\ -\ARROW The base parameters is performed in the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ +\ARROW The signal is modelled by a sum of two Crystal-Ball functions with common mean.\\ +\ARROW The background is a single exponential.\\ +\ARROW The base parameters are obtained from the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ \ARROW All the parameters are fixed in the signal pdf.\\ \ARROW Scaling factors for resolution are determined from MC.\\ \ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ @@ -1076,7 +1076,7 @@ \includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ \end{center} -\ARROW We got $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. +\ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. \column{2.5in} \includegraphics[angle=-90,width=0.95\textwidth]{{images/FitJpsiKstar_withBDT_withoutPartially}.pdf}\\ \includegraphics[angle=-90,width=0.95\textwidth]{{images/Scaling_factor}.pdf}\\ @@ -1093,7 +1093,7 @@ \begin{minipage}{\textwidth} \begin{footnotesize} \ARROW No Monte Carlo simulation is perfect! One needs to correct for remaining differences.\\ -\ARROW We reweighed our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. +\ARROW We reweighted our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. \only<1>{ \begin{center} \includegraphics[angle=-90,width=0.38\textwidth]{images/pt.pdf} @@ -1143,7 +1143,7 @@ \item We use up to $4^{th}, 5^{th}, 6^{th}, 5^{th}$ order for the $\cos \thetal, \cos \thetak, \phi, q^2$. \item The coefficients were determined using Method of Moments, with a huge simulation sample. \item The simulation was done assuming a flat phase space and reweighing the $q^2$ distribution to make is flat. -\item To make this work the $q^2$ distribution needs to be reweighed to be flat. +\item To make this work the $q^2$ distribution needs to be reweighted to be flat. \end{itemize} %\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} @@ -1304,7 +1304,7 @@ \begin{itemize} \item Tension with $3~\invfb$ gets confirmed! -\item The two bins deviate both in $2.8~\sigma$ from SM prediction. +\item two bins both deviate by $2.8~\sigma$ from SM prediction. \item Result compatible with previous result. \end{itemize} @@ -1341,7 +1341,7 @@ \begin{align*} \hat{M}_i=\dfrac{1}{\sum_e \omega_e} \sum_e \omega_e f_i(\overrightarrow{\Omega}_e) \end{align*} -\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights do not matter. +\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights does not matter. \end{minipage} @@ -1394,12 +1394,12 @@ \begin{footnotesize} \begin{minipage}{\textwidth} -\ARROW Fit for amplitudes as (continues)functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ \ARROW Needs some Ansatz: \begin{align*} A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} \end{align*} -\ARROW The assumption is test extensively with toys.\\ +\ARROW The assumption is tested extensively with toys.\\ \ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} \item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. \item Scalar amplitudes: $+4$ DoF. @@ -1411,7 +1411,7 @@ \item At current point the method is limited by statistics. \item In the future the power of this method will increase. \end{itemize} -\ARROW Allows to measure the zero-crossing points for free and with smaller errors then previous methods. +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. \end{minipage} \end{footnotesize} \vspace*{2.1cm} @@ -1527,7 +1527,7 @@ \column{0.4\textwidth} \begin{itemize} -\item Despite large theoretical errors the results are consistently smaller then SM prediction. +\item Despite large theoretical errors the results are consistently smaller than SM prediction. \end{itemize} \column{0.6\textwidth} \includegraphics[width=0.87\textwidth]{images/bukst_BF.png} @@ -1717,7 +1717,7 @@ \begin{frame}{Link the observables} \begin{footnotesize} -\ARROW Fit prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} +\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} @@ -1867,8 +1867,8 @@ \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 work to check - what are the most relevant Wilson Coefficients to explain all deviations, by allowing progressively different WC to get NP contributions and compare the pulls. +\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} @@ -1996,7 +1996,7 @@ \end{align*} \hfill where $\delta_a$ and $\delta_b$ are function of product of tiny $P_6^\prime$, $P_8^\prime$, $P_3$.\medskip\\ -\ARROW {\it This is true independently of any crazy non-factorizable, factorizable, or New Physics (with no weak phases) that is included inside the $H_\lambda$ (or $A_{\perp,\|,0}$)} +\ARROW {\it This is truly independently of any crazy non-factorizable, factorizable, or New Physics (with no weak phases) that is included inside the $H_\lambda$ (or $A_{\perp,\|,0}$)} \end{itemize} @@ -2080,7 +2080,7 @@ {~} \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 the Eq. 24 to be valid with at least leading order at the Taylor expansion.\\ +\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} diff --git a/b2sll_barcelona/Makefile b/b2sll_barcelona/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/b2sll_barcelona/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/b2sll_barcelona/beamercolorthemeFlip.sty b/b2sll_barcelona/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/b2sll_barcelona/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 +\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 + diff --git a/b2sll_barcelona/beamerinnerthemeFlip.sty b/b2sll_barcelona/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/b2sll_barcelona/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 + +% % 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 + diff --git a/b2sll_barcelona/beamerouterthemeFlip.sty b/b2sll_barcelona/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/b2sll_barcelona/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 + +% 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 +\endinput + + diff --git a/b2sll_barcelona/beamerouterthemedecolines.sty b/b2sll_barcelona/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/b2sll_barcelona/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 + +% 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 + diff --git a/b2sll_barcelona/beamerthemeFlip.sty b/b2sll_barcelona/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/b2sll_barcelona/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 + + +%% 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 +\endinput \ No newline at end of file diff --git a/b2sll_barcelona/distracted_ilissa-ocko-cartoon.jpg b/b2sll_barcelona/distracted_ilissa-ocko-cartoon.jpg new file mode 100644 index 0000000..5f007b0 --- /dev/null +++ b/b2sll_barcelona/distracted_ilissa-ocko-cartoon.jpg Binary files differ diff --git a/b2sll_barcelona/images/.DS_Store b/b2sll_barcelona/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- 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+\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \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} +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\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}} + +\newcommand{\av}[1]{\langle #1 \rangle} +% particles +\def\LstFTTT {\ensuremath{\PLambda^{*}(1520)^{0}}\xspace} +\def\dll {\ensuremath{\mathrm{DLL}}\xspace} + \def\Lb {\ensuremath{\PLambda_b}} + + +% useful decays +\def\BdToKpimm {\decay{\Bd}{\Kp\pim\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsToJPsiKst {\decay{\Bs}{\jpsi\Kstarz}} +\def\BdTopsitwosKst {\decay{\Bd}{\psitwos\Kstarz}} +\def\LstFTTTT {\decay{\LstFTTT}{p\Km}} +%\def\LbToLstmm {\decay{\Lb}{\PLambda^{*}(1520)^{0} \mumu}} +\def\LbTopKmm {\decay{\Lb}{p\Km\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsTophimm {\decay{\Bs}{\Pphi\mumu}} + +% interesting variables +\def\mkpi {\ensuremath{m_{K\pi}}\xspace} +\def\mkpimm{\ensuremath{m_{K\pi\mu\mu}}\xspace} + +%% peaking background mass hypotheses +\def\mkmm {\ensuremath{m_{K\mu\mu}}\xspace} +\def\mSwappKmm {\ensuremath{m_{(\pi\to p)K\mu\mu}}\xspace} +\def\mSwappiK {\ensuremath{m_{(\pi\to K)K}}\xspace} +\def\mSwappiKmm {\ensuremath{m_{(\pi\to K)K\mu\mu}}\xspace} +\def\mSwappK {\ensuremath{m_{(\pi\to p)K}}\xspace} +\def\mDoubleSwappKmm {\ensuremath{m_{(K\to p)(\pi\to K)\mu\mu}}\xspace} +\def\mDoubleSwappK {\ensuremath{m_{(K\to p)(\pi\to K)}}\xspace} +\def\mSwapKst {\ensuremath{m_{K\leftrightarrow\pi}}\xspace} + +%% some other decays +\def\BsToPhimm {\decay{\Bs}{\phi\mumu}} +\def\BsToPhimmFULL {\decay{\Bs}{\phi(\to\!K^{+}K^{-})\mumu}} +\def\BsToKKmm {\decay{\Bs}{\Kp\Km\mumu}} + +\newcommand{\delC}[1]{\delta {\cal C}_{#1}} +\newcommand{\dC}[1]{{\cal C}_{#1}^{\rm NP}} +\newcommand{\dCp}[1]{{\cal C}_{#1^\prime}^{\rm NP}} + + + + +\definecolor{green}{rgb}{0.2,0.6,0.2} +\definecolor{lightgreen}{rgb}{0.4,1,0.4} +\definecolor{verylightgreen}{rgb}{0.7,1,0.7} +\def\cgreen{\color{green}} +\definecolor{brown}{rgb}{0.4,0.2,0.0} +\def\cbrown{\color{brown}} +\def\cred{\color{red}} +\definecolor{darkblue}{rgb}{0.0,0.0,1.0} +\def\cdarkblue{\color{darkblue}} +\definecolor{darkgrey}{rgb}{0.4,0.4,0.4} +\definecolor{lightgrey}{rgb}{0.7,0.7,0.7} +\definecolor{verylightblue}{rgb}{0.8,0.8,1.0} +\definecolor{lightblue}{rgb}{0.6,0.6,1.0} +\definecolor{verylightyellow}{rgb}{1.0,1.0,0.5} +\definecolor{lightyellow}{rgb}{1.0,0.7,0.3} +\definecolor{darkred}{rgb}{0.6,0.0,0.0} + +\definecolor{green}{rgb}{0.3,0.6,0.2} +\definecolor{green}{rgb}{0.3,0.7,0.4} + + + + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich, IFJ PAN)} +\institute{UZH} +\title[Rare B Decays: Theory and Experiment 2016]{Rare B Decays: Theory and Experiment 2016} +\date{18 April 2016} + + +\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 {Recent results \\from LHCb +} + \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}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\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}{Barcelona, \\April 18, 2016} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} +{~}\\ + +\begin{enumerate} + +\item Conclusions. +\end{enumerate} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Why flavour physics +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% DETECTOR +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\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} + + + + + +\iffalse + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Modern challenges: loops come in to the game} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\item Standard Model contributions suppressed or absent: +\begin{itemize} +\item Flavour Changing Neutral Currents. +\item CP violation +\item Lepton Flavour/Number or Lepton Universality violation. +\end{itemize} +\item In general can probe physics beyond General Purpose Detectors reach. +\end{itemize} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{{images/TauLFV_UL_2014001_averaged}.png} + + +\end{columns} +\begin{center} +\includegraphics[width=0.75\textwidth]{images/Bsmumu.png} +\includegraphics[width=0.20\textwidth]{{images/bsmumu_SM}.png} +\end{center} +\end{minipage} + + \vspace*{2.1cm} +\end{frame} +\fi + + + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{Why rare decays?} + +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kind of processes are suppressed in SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{lupa.png} +\includegraphics[scale=0.3]{example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{couplings.png} +\end{columns} + +\end{frame} + + + + +\begin{frame}{Tools in rare $\PBzero$ decays} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item \textbf{Operator Product Expansion and Effective Field Theory} +\end{itemize} +\begin{columns} +\column{0.1in}{~} +\column{3.2in} +\begin{footnotesize} + + +\begin{align*} +H_{eff} = - \dfrac{4G_f}{\sqrt{2}} V V^{\prime \ast}\ \sum_i \left[\underbrace{C_i(\mu)O_i(\mu)}_\text{left-handed} +\ +\underbrace{C'_i(\mu)O'_i(\mu)}_\text{right-handed}\right], +\end{align*} + \end{footnotesize} +\column{2in} +\begin{tiny} +\begin{description} + \item[i=1,2] Tree + \item[i=3-6,8] Gluon penguin + \item[i=7] Photon penguin + \item[i=9.10] EW penguin + \item[i=S] Scalar penguin + \item[i=P] Pseudoscalar penguin + \end{description} + +\end{tiny} +\end{columns} +where $C_i$ are the Wilson coefficients and $O_i$ are the corresponding effective operators. +\begin{center} +\includegraphics[width=0.85\textwidth,height=3cm]{images/all.png} + +\end{center} + + + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +\fi + + +\begin{frame}{Analysis of Rare decays} +\begin{footnotesize} + +%{\Large Since a long time ago...} \\ \medskip +%\hspace*{1.4cm}$\Rightarrow$ $b \to s \gamma$ and $b \to s \ell\ell $ {\bf Flavour Changing Neutral Currents} have been used as {\bf \cred Our Portal} \\ to explore the fundamental theory beyond SM. \\ +%\medskip +%\medskip +%\hfill....... with not much success till 2013.\hspace*{1cm} +%\bigskip + +Analysis of FCNC in a model-independent approach, effective Hamiltonian: +\vspace*{-0.1cm} +\begin{columns} +\begin{column}{1cm} +~ +\end{column} +\begin{column}{8cm} +\begin{equation*} +b\to s\gamma(^*): {\mathcal H}^{SM}_{\Delta F=1} \propto + \sum_{i=1}^{10} V_{ts}^* V_{tb} {\cgreen \C{i}} \alert{ {\cal O}_i} + \ldots +\end{equation*} + +\vspace{-0.2cm} + +\begin{itemize} +\item $\alert{ {\cal O}_7} = \frac{e}{16 \pi^2}m_b\, + (\bar s\sigma^{\mu\nu} P_R b) F_{\mu\nu}\,$ %\quad [real or soft photon] +\item $\alert{ {\cal O}_9}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b)\ (\bar\ell\gamma_\mu\ell)$ + %\quad [$b\to s\mu\mu$ via $Z$/hard $\gamma$] +\item $\alert{ {\cal O}_{10}}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b) \ (\bar\ell\gamma_\mu\gamma_5\ell)$, ... +%\quad [$b\to s\mu\mu$ via $Z$] +\end{itemize} +\end{column} +\begin{column}{5.5cm} +\includegraphics[width=3.5cm]{images/qum1.png} +%\includegraphics[width=3cm]{bsll.pdf} +\end{column} +\end{columns} + +%\hspace*{5cm} with no clear success yet... +%\bigskip + + +%\centerline{{\bf Goal}: \underline{Decode the short distance physics to find a smoking gun of BSM}\hspace*{2cm}} + + +\bigskip +\hspace*{0.0cm} $\bullet$ {\bf SM} Wilson coefficients up to NNLO + e.m. corrections at $\mu_{ref}=4.8$ GeV [{\cgreen Misiak et al.}]: $${\cal C}_7^{\rm SM}=-0.29,\, {\cal C}_9^{\rm SM}=4.1,\, {\cal C}_{10}^{\rm SM}=-4.3$$ +%BUT, like in the film there is always the good, the bad and the ugly. +\bigskip +$\bullet$ {\bf NP} changes short distance ${\cal C}_i-{\cal C}_i^{\rm SM}={\cal C}_i^{\rm NP}$ and induce new operators, like ${\cal O}^\prime_{7,9,10}={\cal O}_{7,9,10}\,\, (P_L \leftrightarrow P_R)$ ... also scalars, pseudoescalar, tensor operators...%\bigskip + + +\end{footnotesize} + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\iffalse +%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$, where it all begun} +{~} + \begin{minipage}{\textwidth} +\only<1>{ +\begin{columns} +\column{0.6\textwidth} + August 2013:\\ + + \includegraphics[width=0.95\textwidth]{images/P5prime.png} +\column{0.4\textwidth} +\begin{itemize} +\item LHCb observed a deviation in $4.3-8.68~\GeV^2$ using $1~\invfb$ of data. +\item It turned out that the discrepancy occurred in an observable that was not constrained. +\item $q^2$ is the dimuon invariant mass. + +\end{itemize} +\end{columns} + + +} + + + + +\only<2>{ + + +\begin{columns} +\column{0.6\textwidth} + August 2013:\\ + + \includegraphics[width=0.95\textwidth]{images/P5prime.png} +\column{0.4\textwidth} +\begin{itemize} +\item LHCb observed a deviation in $4.3-8.68~\GeV^2$ using $1~\invfb$ of data. +\item It turned out that the discrepancy occurred in an observable that was not constrained. + +\end{itemize} +\end{columns} + + +\begin{exampleblock}{} +Now let's move back and see the theory behind the $\PBzero \to \PKstar \Pmuon \APmuon$ and $P_5^{\prime}$. +\end{exampleblock} +} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +LHCb measurement of $\PBd \to \PKstar \Pmu \Pmu$ +\end{Huge} +\end{center} + + + + +\end{frame} + +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCbs $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{columns} +\column{0.2in} +{~} +\column{2in} +\ARROW Trigger +\begin{itemize} +\item Muon trigger. +\item Topological trigger. +\end{itemize} +\ARROW Good modelling with MC. \\ +\ARROW Selection: +\begin{itemize} +\item As loose as possible. +\item Based on the $\PBzero$ vertex quality, impact parameters, loose Particle identification for the hadrons. +\item The variables were chosen in a way we are sure the are correctly modelled in MC. +\end{itemize} +\column{2.8in} + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_pt}.pdf}\\ +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_costhetal}.pdf} +\end{columns} + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Peaking backgrounds} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW A number of peaking backgrounds that can mistaken as your signal.\\ +\ARROW There where a specially designed vetoes to fight each of them. +\begin{center} +\begin{tiny} +\hspace{-1cm}\begin{tabular}{ r | c c | c c } + \hline + & \multicolumn{2}{c|}{after preselection, before vetoes} & \multicolumn{2}{c }{after vetoes and selection}\\ + Channel & Estimated events & \% signal & Estimated events & \% signal \\ + \hline + \hline + $\PLambda_b \to \PLambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ + $\PLambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ + $\PBd \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ +$\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ +signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ +$\PBd \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ + + \hline + \end{tabular} +\end{tiny} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/h_Bd_Kstmm_vetoes}.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{{h_Lb_L1520mm_vetoes}.pdf} + +\end{center} + + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +\fi + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation} +{~} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\begin{footnotesize} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. +\item BDT with k-Folding technique. +\item Completely data driven. +\end{footnotesize} +\end{itemize} +\begin{center} +\includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf} +\end{center} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.82\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation, efficiency} +{~} + + \begin{minipage}{\textwidth} + \begin{footnotesize} + +\ARROW BDT was also checked in order not to bias our angular distribution: +\begin{center} +\includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} +\end{center} +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\begin{frame}{Mass modelling} +{~} +\begin{minipage}{\textwidth} +\begin{footnotesize} + +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\ARROW The signal is modelled by a sum of two Crystal-Ball functions with common mean.\\ +\ARROW The background is a single exponential.\\ +\ARROW The base parameters are obtained from the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ +\ARROW All the parameters are fixed in the signal pdf.\\ +\ARROW Scaling factors for resolution are determined from MC.\\ +\ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ +\ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. +\column{2.5in} +\begin{center} +\includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ + +\end{center} +\ARROW The S-wave fraction is extracted using a \texttt{LASS} model. +\end{columns} + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\iffalse +%%%%%%%%%%%%%%% +\begin{frame}{Monte Carlo corrections} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW No Monte Carlo simulation is perfect! One needs to correct for remaining differences.\\ +\ARROW We reweighted our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. +\only<1>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/pt.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/vertex.pdf}\\ +\includegraphics[angle=-90,width=0.38\textwidth]{images/nTracks.pdf} +\end{center} +} +\only<2>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/eta_logy.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/B0_p.pdf} \\ +\includegraphics[angle=-90,width=0.38\textwidth]{{images/bdt_data_mc_nominalMkpi}.pdf} +\end{center} +} + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Detector acceptance} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} + +\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} 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 $\cos \thetal, \cos \thetak, \phi, q^2$. +\item The coefficients were determined using Method of Moments, with a huge simulation sample. +\item The simulation was done assuming a flat phase space and reweighing the $q^2$ distribution to make is flat. +\item To make this work the $q^2$ distribution needs to be reweighted to be flat. +\end{itemize} +%\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} + + + +\column{0.4\textwidth} +%\only<1>{ +%\includegraphics[width=0.99\textwidth]{images/q2PHSP.png}\\ +%\includegraphics[width=0.99\textwidth]{images/q2PHSPw.png} +%} + +\only<1>{ +\includegraphics[width=0.99\textwidth]{images/det.png} +} +\end{columns} + + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Control channel} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\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} +\end{footnotesize} +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mlogjpsi.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mkpijpsi.pdf}\\ +\includegraphics[width=0.99\textwidth]{images/angles3.png} +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.94\textwidth]{images/columns.png} + + \end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} +\begin{enumerate} +\item Maximum likelihood fit: +\begin{itemize} +\item The most standard way of obtaining the parameters. +\item Suffers from convergence problems, under coverages, etc. in low statistics. +\end{itemize} +\item Method of moments: +\begin{itemize} +\item Less precise then the likelihood estimator ($10-15\%$ larger uncertainties). +\item Does not suffer from the problems of likelihood fit. +\end{itemize} +\item Amplitude fit: +\begin{itemize} +\item Incorporates all the physical symmetries inside the amplitudes! The most precise estimator. +\item Has theoretical assumptions inside! +\end{itemize} +\end{enumerate} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\ARROW In the maximum likelihood fit one could weight the events accordingly to the $\dfrac{1}{\varepsilon(\cos \thetal, \cos \thetak, \phi, q^2)}$\\ +\ARROW Better alternative is to put the efficiency into the maximum likelihood fit itself: +\begin{align*} +\mathcal{L}=\prod_{i=1}^N \epsilon_i(\Omega_i, q_i^2) \mathcal{P}(\Omega_i, q_i^2) / \int \epsilon(\Omega, q^2) \mathcal{P}(\Omega, q^2) d\Omega dq^2 +\end{align*} +\ARROW Only the relative weights matters!\\ +\ARROW The Procedure was commissioned with TOY MC study.\\ +\ARROW Use Feldmann-Cousins to determine the uncertainties. \\ +\ARROW Angular background component is modelled with $2^{\rm nd }$ order Chebyshev polynomials, which was tested on the side-bands.\\ +\ARROW S-wave component treated as nuisance parameter.\\ +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_Afb3}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P11}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P57}.pdf} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[angle=-90,width=0.65\textwidth]{images/P5pPadOverlay.pdf}\\ + \end{center} + +\begin{itemize} +\item Tension with $3~\invfb$ gets confirmed! +\item two bins both deviate by $2.8~\sigma$ from SM prediction. +\item Result compatible with previous result. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S9Pad.pdf} +} + + +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + + + + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Method of moments} +{~} +\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.\\ +\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} +\end{align*} +\begin{align*} +M_i = \int \left( \dfrac{1}{d(\Gamma+ \bar{\Gamma})/dq^2} \right) \dfrac{d^3(\Gamma+\bar{\Gamma})}{d \overrightarrow{\Omega}} f_i(\overrightarrow{\Omega})d \Omega +\end{align*} +\ARROW Don’t have true angular distribution but we ''sample'' it with our data.\\ +\ARROW Therefore: $\int \to \sum$ and $M_i \to \widehat{M}_i$ +\begin{align*} +\hat{M}_i=\dfrac{1}{\sum_e \omega_e} \sum_e \omega_e f_i(\overrightarrow{\Omega}_e) +\end{align*} +\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights does not matter. + + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Method of moments - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\only<3> +{ +\ARROW Method of Moments allowed us to measure for the first time a new observable: +} + +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S9Pad.pdf} +} +\only<3>{ +\includegraphics[angle=-90,width=0.75\textwidth]{images/S6cPad.pdf} +} + +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + + + +\begin{frame}{Amplitudes method} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Needs some Ansatz: +\begin{align*} +A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} +\end{align*} +\ARROW The assumption is tested extensively with toys.\\ +\ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} +\item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. +\item Scalar amplitudes: $+4$ DoF. +\item Symmetries of the amplitudes reduces the total budget to: $28$. +\end{itemize} +\ARROW The technique is described in \href{http://arxiv.org/pdf/1504.00574v2.pdf}{\color{blue}{JHEP06(2015)084}}, U. Egede, M. Patel, K.A. Petridis.\\ +\ARROW Allows to build the observables as continuous functions of $q^2$: +\begin{itemize} +\item At current point the method is limited by statistics. +\item In the future the power of this method will increase. +\end{itemize} +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\begin{center} +\begin{columns} +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_AFBOverlay}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S4Overlay}.pdf} + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S5Overlay}.pdf}\\ +{~}\\{~}\\{~}\\{~}\\ +\begin{large} +Zero crossing points: +\end{large} +\begin{align*} +q_0(S_4) & <2.65 & {\rm{~at~}} & 95\% ~CL \\ +q_0(S_5) & \in \left[ 2.49,3.95 \right] & {\rm{~at~}} & 68\% ~CL \\ +q_0(A_{FB}) & \in \left[ 3.40, 4.87 \right] & {\rm{~at~}} & 68\% ~CL +\end{align*} + + +\end{columns} +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{Compatibility with SM} +{~} + + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.1in} +{~} +\column{2in} +\ARROW Use \texttt{EOS} software package to test compatibility with SM.\\ +\ARROW Perform the $\chi^2$ fit to the measured: +\begin{center} +\begin{align*} +F_L, A_{FB}, S_{3,..., 9} . +\end{align*} +\end{center} +\ARROW Float a vector coupling: $\Re(C_9)$.\\ +\ARROW Best fit is found to be $3.4~\sigma$ away from the SM. + + +\column{3in} +\begin{align*} +\Delta \Re (C_9) \equiv \Re(C_9)^{{\rm fit}} - \Re(C_9)^{{\rm SM}} = -1.03 +\end{align*} +\includegraphics[angle=-90,width=0.95\textwidth]{images/wilsonchi2.pdf} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Other related LHCb measurements. + +\end{Huge} +\end{center} + + + + +\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 than 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}\nonumber +\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}{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}{Steps in the near future} +{~} + \begin{minipage}{\textwidth} + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Conclusions} +{~} + \begin{minipage}{\textwidth} +\begin{itemize} +\item LHCb is and still will provide the most precise measurements of EWP! +\item Many analysis in the pipe line! +\item Even more ideas to what to do with existing and further data. + +\end{itemize} + + \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} + + + +\backupend + +\end{document} diff --git a/b2sll_barcelona/mchrzasz.tex~ b/b2sll_barcelona/mchrzasz.tex~ new file mode 100644 index 0000000..85cc86a --- /dev/null +++ b/b2sll_barcelona/mchrzasz.tex~ @@ -0,0 +1,307 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + 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 + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \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{\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, IFJ PAN)} +\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}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\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/b2sll_barcelona/mchrzasz.toc b/b2sll_barcelona/mchrzasz.toc new file mode 100644 index 0000000..429917f --- /dev/null +++ b/b2sll_barcelona/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/b2sll_barcelona/pt.pdf b/b2sll_barcelona/pt.pdf new file mode 100644 index 0000000..9d347bf --- /dev/null +++ b/b2sll_barcelona/pt.pdf Binary files differ diff --git a/b2sll_barcelona/tikzfeynman.sty b/b2sll_barcelona/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/b2sll_barcelona/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}, +} +