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differ diff --git a/Implication_workshop/11_12_2016/mchrzasz.tex b/Implication_workshop/11_12_2016/mchrzasz.tex index 9c9041f..179716b 100644 --- a/Implication_workshop/11_12_2016/mchrzasz.tex +++ b/Implication_workshop/11_12_2016/mchrzasz.tex @@ -255,6 +255,7 @@ + {\fontspec{Trebuchet MS} \Large Marcin ChrzÄ…szcz}\\ University of Zurich \& Polish Academy of Sciences\\ \vspace{1em} @@ -277,10 +278,10 @@ \ARROW Theoretical framework for $B$ decays\\[3.mm] \ARROW $B \to K^* \ell^+ \ell^-$ observables and calculations\\[3.mm] -\ARROW Numerical approach\\[3.mm] \ARROW Which data do Flavour factories publish\\[3.mm] \ARROW New Physics searches\\[3.mm] \ARROW What would be the best way to exchange the information?\\[3.mm] +\ARROW Wilson Coefficients fits with \textbf{GAMBIT}\\[3.mm] \ARROW Questions for discussion \end{minipage} @@ -290,6 +291,16 @@ %%%%%%%%%%%%%%%%%%%%% % Nazila %%%%%%%%%%%%%%%%%%%%% +\begin{frame} + +\begin{center} +\begin{Huge} +Theoretical framework for $\PB$ decays. +\end{Huge} +\end{center} + +\end{frame} + %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Theoretical framework for $B$ decays} @@ -518,8 +529,8 @@ \vspace*{0.1cm} \visible<3>{% \begin{center} -{\small Anomalies can be explained with 20-50\% non-factorisable power corrections at the -observable level in the critical bins {\tiny \bf \color{vert}(Ciuchini et al., 1512.07157)}\\[0.2cm] +{\small The observed deviations from the SM can be explained with 20-50\% non-factorisable power corrections at the +observable level {\tiny \bf \color{vert}(Ciuchini et al., 1512.07157)}\\[0.2cm] This corresponds to more than 150\% error at the amplitude level for the critical bins!} \end{center} } @@ -527,17 +538,65 @@ \end{footnotesize} } + + +\frame { \frametitle{$B \to K^* \mu^+ \mu^-$ -- Optimized observables} +\begin{align*} +% +\av{P_1}_{\rm bin}&= \frac12 \frac{\int_{{\rm bin}} dq^2 [J_3+\bar J_3]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]} +& +% \av{P_1^{CP} }_{\rm bin}&= \frac12 \frac{\int_{{\rm bin}} dq^2 [J_3-\bar J_3]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\label{p1}\\ +% +\av{P_2}_{\rm bin} &= \frac18 \frac{\int_{{\rm bin}} dq^2 [J_{6s}+\bar J_{6s}]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\\ +% & \av{P_2^{CP} }_{\rm bin} &= \frac18 \frac{\int_{{\rm bin}} dq^2 [J_{6s}-\bar J_{6s}]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\\ +% +% \av{P_3}_{\rm bin} &= -\frac14 \frac{\int_{{\rm bin}} dq^2 [J_9+\bar J_9]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ , +% & \av{P_3^{CP} }_{\rm bin} &= -\frac14 \frac{\int_{{\rm bin}} dq^2 [J_9-\bar J_9]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\\ +% +\av{P'_4}_{\rm bin} &= \frac1{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_4+\bar J_4] +& +% \av{{P'_4}^{CP} }_{\rm bin} &= \frac1{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_4-\bar J_4]\ ,\\ +% +\av{P'_5}_{\rm bin} &= \frac1{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_5+\bar J_5]\\ +% & \av{{P'_5}^{CP} }_{\rm bin} &= \frac1{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_5-\bar J_5]\ ,\\ +% +\av{P'_6}_{\rm bin} &= \frac{-1}{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_7+\bar J_7] +& +% \av{{P'_6}^{CP} }_{\rm bin} &= \frac{-1}{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_7-\bar J_7]\ ,\\ +% +\av{P'_8}_{\rm bin} &= \frac{-1}{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_8+\bar J_8] +% & \av{{P'_8}^{CP} }_{\rm bin} &= \frac{-1}{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_8-\bar J_8]\ . +% +\end{align*} +% +% where the normalization ${\cal N}_\bin^\prime$ is defined as +% +with {\footnotesize \[{\cal N}_\bin^\prime = {\textstyle \sqrt{-\int_\bin dq^2 [J_{2s}+\bar J_{2s}] \int_{{\rm bin}} dq^2 [J_{2c}+\bar J_{2c}]}}\]}\\[6mm] +$+$ CP violating clean observables and other combinations\\[2mm] +{\vspace*{-0.cm}\hspace*{5.cm}\tiny \bf \color{vert}U.~Egede et al., JHEP {\bf 0811} (2008) 032, JHEP {\bf 1010} (2010) 056}\\ +{\vspace*{-0.1cm}\hspace*{5.cm}\tiny \bf \color{vert}J.~Matias et al., JHEP {\bf 1204} (2012) 104}\\ +{\vspace*{-0.1cm}\hspace*{5.cm}\tiny \bf \color{vert}S.~Descotes-Genon et al., JHEP 1305 (2013) 137}\\ +% Sebastien Descotes-Genon (Orsay, LPT), Tobias Hurth (Mainz U., Inst. Phys.), Joaquim Matias, Javier Virto, JHEP 1305 (2013) 137 +} + %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%% % Marcin %%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Flavour measurements +\end{Huge} +\end{center} +\end{frame} \begin{frame}\frametitle{Detector effects 1/2} {~}\\ \ARROW In Flavour factories because we usually measure the properties of a $\PB$ meson decay we can -provided the measurements that are corrected for the detector effects!\\ +provide the measurements that are corrected for the detector effects!\\ \begin{center} \includegraphics[width=0.95\textwidth]{images/andy.png}\let\thefootnote\relax\footnote {Thanks to Andy Buckley for the plot.} @@ -585,7 +644,9 @@ \begin{footnotesize} \ARROW There are number of ways the B-factories publish their results.\\ -\ARROW Most of the time the information to links are on the collaboration web pages: +\ARROW Most of the time the information to links are on the collaboration web pages:\\ + + \begin{columns} \column{0.5\textwidth} \includegraphics[width=0.95\textwidth]{images/bellepub.png} @@ -594,6 +655,13 @@ \end{columns} +\href{http://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/Summary_all.html}{\url{http://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/Summary_all.html}}\\ + +\href{http://belle.kek.jp/belle/publications.html}{\url{http://belle.kek.jp/belle/publications.html}}\\ + +\href{http://www.slac.stanford.edu/BFROOT/www/pubs/babarpubs.html} +{\url{http://belle.kek.jp/belle/publications.html}} + \end{footnotesize} \end{minipage} @@ -604,10 +672,16 @@ {~}\\ \begin{minipage}{\textwidth} \begin{footnotesize} - +\only<1>{ \begin{center} \includegraphics[width=0.95\textwidth]{images/cds.png} \end{center} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.95\textwidth]{images/cds2.png} +\end{center} +} \ARROW Figure on \texttt{CDS} and \texttt{LHCb publications page} available in many formats: \texttt{.pdf}, \texttt{.eps}, \texttt{.png}, \texttt{ROOT\_.C}\\ \ARROW No need to read the numbers from the plot any more!\\ \ARROW Supplementary material not included in the paper\\ @@ -623,7 +697,7 @@ {~}\\ \begin{minipage}{\textwidth} \begin{footnotesize} -\ARROW More and more results are being published on HepData make them ''one clic away'' to get. +\ARROW More and more results are being published on HepData make them ''one click away'' to get. \begin{center} \includegraphics[width=0.95\textwidth]{images/hepdata.png} \end{center} @@ -783,7 +857,15 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % GAMBIT %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Global fits +\end{Huge} +\end{center} + +\end{frame} \begin{frame} @@ -816,9 +898,9 @@ 11 Experiments, 4 major theory codes\\ \vspace{2mm} \scriptsize \begin{tabular}{l l} -\textbf{ATLAS} & A.\ Buckley, P.\ Jackson, C.\ Rogan,\\ +\textbf{ATLAS} & A.\ Buckley, C.\ Rogan,\\ & M.\ White, \vspace{0.5mm}\\ -\textbf{Flavour exp.} & F.\ Bernlochner, M.\ Chrzaszcz, N.\ Serra\vspace{0.5mm}\\ +\textbf{Flavour exp.} & F.\ Bernlochner, M.\ Chrzaszcz, P.\ Jackson, N.\ Serra\vspace{0.5mm}\\ \textbf{Fermi-LAT} & J.\ Conrad, J.\ Edsj\"o, G.\ Martinez\\ & P.\ Scott\vspace{0.5mm}\\ \textbf{CTA} & C. Bal\'azs, T.\ Bringmann, \\ @@ -861,10 +943,18 @@ {\hspace*{3.cm}\tiny \bf \color{vert}Mahmoudi, CPC 178 (2008) 745; CPC 180 (2009) 1579, CPC 180 (2009) 1718}\\[-0.1cm] {\hspace*{3.cm}\tiny \bf \color{vert} available from http://superiso.in2p3.fr/}\\[0.4cm] \item {\bf\color{brique}SuperIso} interfaced into {\bf\color{brique}GAMBIT} through the flavour physics module {\bf\color{brique}FlavBit}\\[0.2cm] -{\hspace*{3.cm}\tiny \bf \color{vert}{\bf\color{brique}GAMBIT}: The Global And Modular BSM Inference Tool}\\[-0.1cm] + {\hspace*{3.cm}\tiny \bf \color{vert}Web page: http://gambit.hepforge.org/}\\[0.4cm] \item {\bf\color{brique}FlavBit} determines the likelihoods by comparing the theoretical evaluations and the experimental results taking into account the experimental and theoretical correlations. +\item In this study we used: +\begin{itemize} +\item $\PB \to \PKstar \Pmu \Pmu$ with all the $q^2$ bins and correlations matrices from HepData! +\item $\PB _{s/d} \to \Pmu \Pmu$ +\item $\Pbeauty \to \Pstrange \gamma$ +\end{itemize} + + \end{itemize} \end{column} @@ -874,8 +964,22 @@ \end{minipage} \end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\iffalse +\begin{frame}\frametitle{Global Analysis with Gambit - Results} +{~}\\ + \begin{minipage}{\textwidth} +\begin{footnotesize} + +\end{footnotesize} +\end{minipage} + +\end{frame} +\fi +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + \begin{frame}\frametitle{Global Analysis with Gambit - Results} {~}\\ \begin{minipage}{\textwidth} @@ -887,8 +991,10 @@ \includegraphics[width=0.85\textwidth]{{plots/plot_WC_2_like1D_WC_MN}.pdf} \end{column} -\begin{column}[c]{5.2cm} -\includegraphics[width=0.95\textwidth]{{plots/plot_WC_2_3_like2D_WC_MN}.pdf}\\ +\begin{column}[c]{6.0cm} +\includegraphics[angle=-90,width=0.45\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/P5pPadOverlay.pdf}\\ +\includegraphics[width=0.9\textwidth]{{plots/plot_WC_2_3_like2D_WC_MN}.pdf}\\ \ARROW Tension if $\Delta C_9$ observed!\\ \ARROW Other coefficients within SM predictions.\\ \ARROW $C_{10}$ still has a big uncertainty. @@ -931,44 +1037,6 @@ \end{frame} -\frame { \frametitle{$B \to K^* \mu^+ \mu^-$ -- Optimized observables} -\begin{align*} -% -\av{P_1}_{\rm bin}&= \frac12 \frac{\int_{{\rm bin}} dq^2 [J_3+\bar J_3]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]} -& -% \av{P_1^{CP} }_{\rm bin}&= \frac12 \frac{\int_{{\rm bin}} dq^2 [J_3-\bar J_3]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\label{p1}\\ -% -\av{P_2}_{\rm bin} &= \frac18 \frac{\int_{{\rm bin}} dq^2 [J_{6s}+\bar J_{6s}]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\\ -% & \av{P_2^{CP} }_{\rm bin} &= \frac18 \frac{\int_{{\rm bin}} dq^2 [J_{6s}-\bar J_{6s}]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\\ -% -% \av{P_3}_{\rm bin} &= -\frac14 \frac{\int_{{\rm bin}} dq^2 [J_9+\bar J_9]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ , -% & \av{P_3^{CP} }_{\rm bin} &= -\frac14 \frac{\int_{{\rm bin}} dq^2 [J_9-\bar J_9]}{\int_{{\rm bin}} dq^2 [J_{2s}+\bar J_{2s}]}\ ,\\ -% -\av{P'_4}_{\rm bin} &= \frac1{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_4+\bar J_4] -& -% \av{{P'_4}^{CP} }_{\rm bin} &= \frac1{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_4-\bar J_4]\ ,\\ -% -\av{P'_5}_{\rm bin} &= \frac1{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_5+\bar J_5]\\ -% & \av{{P'_5}^{CP} }_{\rm bin} &= \frac1{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_5-\bar J_5]\ ,\\ -% -\av{P'_6}_{\rm bin} &= \frac{-1}{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_7+\bar J_7] -& -% \av{{P'_6}^{CP} }_{\rm bin} &= \frac{-1}{2{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_7-\bar J_7]\ ,\\ -% -\av{P'_8}_{\rm bin} &= \frac{-1}{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_8+\bar J_8] -% & \av{{P'_8}^{CP} }_{\rm bin} &= \frac{-1}{{\cal N}_\bin^\prime} \int_{{\rm bin}} dq^2 [J_8-\bar J_8]\ . -% -\end{align*} -% -% where the normalization ${\cal N}_\bin^\prime$ is defined as -% -with {\footnotesize \[{\cal N}_\bin^\prime = {\textstyle \sqrt{-\int_\bin dq^2 [J_{2s}+\bar J_{2s}] \int_{{\rm bin}} dq^2 [J_{2c}+\bar J_{2c}]}}\]}\\[6mm] -$+$ CP violating clean observables and other combinations\\[2mm] -{\vspace*{-0.cm}\hspace*{5.cm}\tiny \bf \color{vert}U.~Egede et al., JHEP {\bf 0811} (2008) 032, JHEP {\bf 1010} (2010) 056}\\ -{\vspace*{-0.1cm}\hspace*{5.cm}\tiny \bf \color{vert}J.~Matias et al., JHEP {\bf 1204} (2012) 104}\\ -{\vspace*{-0.1cm}\hspace*{5.cm}\tiny \bf \color{vert}S.~Descotes-Genon et al., JHEP 1305 (2013) 137}\\ -% Sebastien Descotes-Genon (Orsay, LPT), Tobias Hurth (Mainz U., Inst. Phys.), Joaquim Matias, Javier Virto, JHEP 1305 (2013) 137 -} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \frame { \frametitle{Numerical approach} @@ -979,7 +1047,6 @@ - \backupend \end{document}