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+\ARROW $9~\%$ of the $\tau$ that are produced in LHCb acceptance ($\eta <5$) have a muon that ends in the magnet tracking stations! {~}\\{~}\\ + \only<1>{ \begin{columns} \column{0.5\textwidth} \includegraphics[width=0.9\textwidth]{images/tauxy.png} @@ -359,9 +360,22 @@ \end{columns} \ARROW Rather uniform distribution. + } + \only<2>{ + \begin{columns} + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/taupz.png} + + + + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/taupy.png} + + \end{columns} + {~}\\ +\ARROW If we exclude the $\pm 150 \rm cm$ regions we loose $14\%$. - - + } \end{minipage} \vspace*{2.cm} @@ -391,6 +405,7 @@ \begin{minipage}{\textwidth} \ARROW $10~\%$ of the $\tau$ that are produced in LHCb acceptance have a muon that ends in the tracking stations! {~}\\{~}\\ + \only<1>{ \begin{columns} \column{0.5\textwidth} \includegraphics[width=0.9\textwidth]{images/Dstarxy.png} @@ -403,8 +418,22 @@ \end{columns} \ARROW Clearly different behaviour than $\mu$. + } + \only<2>{ + \begin{columns} + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/Dstarpz.png} + + + + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/Dstarpy.png} + + \end{columns} + {~}\\ +\ARROW If we exclude the $\pm 150 \rm cm$ regions we loose $17\%$. - + } \end{minipage} @@ -420,6 +449,7 @@ {~}\\ \ARROW $19~\%$ of the $\tau$ that are produced in LHCb acceptance have a muon that ends in the tracking stations! {~}\\{~}\\ + \only<1>{ \begin{columns} \column{0.5\textwidth} \includegraphics[width=0.9\textwidth]{images/Lcxy.png} @@ -434,9 +464,21 @@ \ARROW Clearly different behaviour than $\mu$.\\ \ARROW We have two slow pions. The efficiency looks like factorizes :) - - - + } + \only<2>{ + \begin{columns} + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/Lcpz.png} + + + + \column{0.5\textwidth} + \includegraphics[width=0.9\textwidth]{images/Lcpy.png} + + \end{columns} + {~}\\ +\ARROW If we exclude the $\pm 150 \rm cm$ regions we loose $16\%$. + } \end{minipage} \vspace*{2.cm} \end{frame} @@ -449,6 +491,8 @@ \ARROW Using 3 benchmark channels we see there is quite a lot to be gain!\\ \ARROW This is just tip of the ice berg. \\ \ARROW We need to strengthen the physics program: ex. $\PLambdac(2595)$ decays via intermediate states like $\PSigmac$ which allows polarization measurements.\\ +\ARROW Will add multi bodies to the studies.\\ +\ARROW $\PB^{\ast \ast} \to \PK \PB$ will allow constrained the final state measurements.\\ \ARROW The length of this detector can be optimised based on our ''golden channels''. \end{minipage}