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\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich)}
\institute{UZH}
\title[Electroweak Run2 prospects]{Electroweak Run2 prospects}
\date{1-2 September 2015}


\begin{document}
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{
\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 {Electroweak\\ Run2 prospects}
		\end{column}
                \begin{column}{0.02\textwidth}
                  {~}
                  \end{column}
                \begin{column}{0.23\textwidth}
                 % \hspace*{-1.cm}
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                  \includegraphics[width=0.6\textwidth]{lhcb-logo}
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	\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}}

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\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, Churwalden\\September 1-2, 2015}
\end{center}
\end{frame}
}


\begin{frame}\frametitle{Higher energy!}
\begin{columns}
\column{0.1\textwidth}
{~}
\column{0.5\textwidth}
$7~\TeV$
\column{0.4\textwidth}
$14~\TeV$
\end{columns}


\includegraphics[width=0.95\textwidth]{images/Q_x.png}

\begin{itemize}
\item LHCb cover a very unique region of the phase space that is not accessible for any other experiments.
\item One could measure in this regime:
\begin{itemize}
\item $\PW$, $\PZ$ cross section.
\item Drell-Yan cross section.
\end{itemize}
\item These measurements would strongly constrain the PDF in the fits.
\end{itemize}


\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{frame}\frametitle{Cross section}
$\Rrightarrow$ Higher energy $\Rightarrow$ Higher cross section:
\includegraphics[width=0.95\textwidth]{images/xsection.png}

$\Rrightarrow$ In contrast to RD the EW measurements should start much sooner as they are not statistically dominated!


\end{frame}

\begin{frame}\frametitle{What could we do?}

$\Rrightarrow$ For starters we should start by measurement of $\PZ$ cross section (already ongoing in the group).\\
$\Rightarrow$ Relativity simple, you don't need much data.\\
$\Rightarrow$ Important for MC tuning.\\
$\Rrightarrow$ More interesting: Tripple Gauge Boson Couplings:\\{~}\\
\begin{columns}

\column{3in}
\begin{itemize}
\item Clear SM prediction.
\item Sensitive to anomalous couplings!
\item ATLAS observed a small but consistent deviation in this measurement.
\end{itemize}

\column{2in}
\includegraphics[width=0.9\textwidth]{{images/DibosonGeneric.eps}.jpg}

\end{columns}


\end{frame}

\begin{frame}\frametitle{Drell-Yan}
\begin{columns}
\column{0.05\textwidth}


\column{0.45\textwidth}
\begin{itemize}
\item Very clean theoretical prediction!
\item Effectively you are probing the proton PDF. 
\item Remember that the theory error for all the Higgs calculations comes from PDFs.
\item One could improve really the PDFs thanks to special kinematic region of LHCb.
\item We could reach lower $x$ region of $10^{-6}$, trigger is there! Background needs to be understood.
\end{itemize}

\column{0.5\textwidth}
\includegraphics[width=0.9\textwidth]{{images/450px-Drell-Yan.svg}.png}\\
\includegraphics[angle=-90,width=0.9\textwidth]{{images/13000_14000_y_bin_2_4.5}.pdf}

\end{columns}


\end{frame}

\begin{frame}\frametitle{Central Exclusive Production}
\begin{columns}
\column{0.05\textwidth}


\column{0.65\textwidth}
\begin{itemize}
\item Super clean theoretically.
\item Signature: protons interact and go to the beam pipe undetected, in the detector you are left with couple of particles.
\item Probing PDF and also thanks to DPE we have a link to Higgs Physics.
\item Getting sensitive to saturation effects?
\end{itemize}

\column{0.3\textwidth}
\includegraphics[width=0.6\textwidth]{{images/2gamma}.png}\\
\includegraphics[width=0.6\textwidth]{{images/gammapomeron}.png}\\
\includegraphics[width=0.6\textwidth]{{images/2pomeron}.png}\\
\end{columns}


\end{frame}

\begin{frame}\frametitle{Central Exclusive Production- detector upgrade}
\begin{itemize}
\item For Run2 LHCb installed:HeRSCheL: High Rapidity Shower Counters 
\item They cover $5<\eta<8$.
\item Rejecting the main background for CEP.
\item Allows to measure $p_T^2$ distribution for inelastic events.
\item Dedicated \texttt{L0} trigger for CEP.
\end{itemize}


\includegraphics[width=0.9\textwidth]{{images/upgrade}.png}\\

\end{frame}
  

\begin{frame}\frametitle{Ion-Ion run}
\begin{columns}
\column{0.03\textwidth}
{~}
\column{0.7\textwidth}
\begin{itemize}
\item Tests of all QGP effects:
\begin{itemize}
\item Colour screening.
\item Melting states.
\item Jet quenching.
\item $\PJpsi$ suppression.
\item Elliptic flow.
\end{itemize}
\item Cold and hot matter effects.
\item SMOG.
\item etc.
\end{itemize}

\column{0.27\textwidth}
\includegraphics[width=0.95\textwidth]{images/melt.png}\\

\end{columns}
\includegraphics[width=0.85\textwidth]{images/smog.png}
\end{frame}



\begin{frame}\frametitle{CP-odd Higgs}
\includegraphics[width=0.95\textwidth]{images/diagrams.png}
\begin{itemize}
\item Competitive with ATLAS and CMS
\item We have excellent resolution.
\item Can probe mass around the $\Upsilon$s region.
\end{itemize}


\end{frame}
\begin{frame}\frametitle{top physics}
\begin{itemize}
\item Katharina already presented our recent measurement of top measurement in the forward region.
\item with Run2 data ($5~\rm fb^{-1}$):
\begin{itemize}
\item $[\Plepton, \Pbeauty]$: expect $\sim$  $8300~\Ptop \APtop$ , $5000~\Ptop$-channel, $600~\Pstrange$ -channel, and $180~\PW \Ptop$.
\item $[ \Plepton, \Plepton , \Pbeauty, \Pbeauty]$: expect $\sim$ $530~\Ptop \APtop$.
\end{itemize}
\end{itemize}


\end{frame}

\begin{frame}\frametitle{How about some precision?}

\begin{columns}
\column{0.05\textwidth}
{~}

\column{0.5\textwidth}
\begin{itemize}
\item One can measure the $A_{FB}$ in the $\PZ \to \Pmu \Pmu$ decays:
\begin{align*}
A_{FB}=\dfrac{\sigma(\cos \theta >0) - \sigma(\cos \theta <0) }{\sigma(\cos \theta >0) + \sigma(\cos \theta <0) }
\end{align*}
\item This is dependent on the vector and axial couplings $\Rightarrow$ $\sin \theta_W^{eff}$.
\item Since LEP time there is a small tension in this measurement.
\item With full Run2 data and some smart ideas we might be close to LEP!
\item ATLAS and CMS will not not be able to compete.
\end{itemize}

\column{0.45\textwidth}
\includegraphics[width=0.95\textwidth]{images/AFB_11.png}\\
\includegraphics[width=0.95\textwidth]{images/chi2.png}
\end{columns}

\end{frame}


\begin{frame}\frametitle{Summary}
\begin{itemize}
\item Reach Run2 program in QEE WG measurements:
\begin{enumerate}
\item Drell-Yan
\item Ion-Ion physics
\item Cross section measurements
\item Triple Gauge Couplings
\item top physics
\item CEP
\item $\sin \theta_W^{eff}$
\end{enumerate}
\end{itemize}



\end{frame}






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\end{document}