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Descotes-Genon, L. Hofer, J. Matias, J. Virto}. \item The data can be explained by modifying the $C_9$ Wilson coefficient. -\item Overall there is $>4~\sigma$ discrepancy wrt. SM prediction. +\item Overall there is $>4~\sigma$ discrepancy wrt. the SM prediction. \end{itemize} \includegraphics[width=0.9\textwidth]{images/C9.png} @@ -1113,6 +1113,7 @@ \item Measurements cluster in the same direction. \item We are not opening the champagne yet! \item Still need improvement both on theory and experimental side. +\item More data will shade a light on the matter. \item Time will tell if this is QCD+fluctuations or new Physics: \end{itemize} \pause diff --git a/NuFact_2016/LongLive/HNL.png b/NuFact_2016/LongLive/HNL.png new file mode 100644 index 0000000..2620f8f --- /dev/null +++ b/NuFact_2016/LongLive/HNL.png Binary files differ diff --git a/NuFact_2016/LongLive/cleo.pdf b/NuFact_2016/LongLive/cleo.pdf new file mode 100644 index 0000000..3208956 --- /dev/null +++ b/NuFact_2016/LongLive/cleo.pdf Binary files differ diff --git a/NuFact_2016/LongLive/eventdisplay.png b/NuFact_2016/LongLive/eventdisplay.png new file mode 100644 index 0000000..00bf6f0 --- /dev/null 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\flushright\fontspec{Trebuchet MS}\bfseries \LARGE {Sterile neutrino and other long lived particle searches at LHCb} + \flushright\fontspec{Trebuchet MS}\bfseries \LARGE {Search for massive neutrinos at LHCb and discovery potential of the FCC} \end{column} \begin{column}{0.02\textwidth} {~} @@ -279,7 +279,9 @@ \begin{column}{0.23\textwidth} % \hspace*{-1.cm} \vspace*{-3mm} - \includegraphics[width=0.6\textwidth]{lhcb-logo} + \includegraphics[width=0.6\textwidth]{lhcb-logo}\\ + \includegraphics[width=0.7\textwidth]{fcclogo} + \end{column} \end{columns} @@ -597,7 +599,7 @@ % \textref{M.Chrz\k{a}szcz 2014} \end{frame} -\iffalse + \begin{frame} \frametitle{Summary on Majorana neutrinos in $\textbf{B}$ decays} \vspace{0.5cm} @@ -631,7 +633,7 @@ %\textref{M.Chrz\k{a}szcz 2014} \end{frame} -\fi + @@ -1028,6 +1030,147 @@ \end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Future Circular Collider (FCC) } +\begin{columns} +\column{0.5\textwidth} +\begin{itemize} +\item $p - p$ collider $\mathcal{O}(100{\rm TeV})$: +\begin{itemize} +\item $16~T$ in $100~\rm km$ tunnel!!! +\end{itemize} +\item The collider would benefit form existing CERN infrastructure. +\item Before one reaches the technology for $\mathcal{O}(100{\rm TeV})$: +\begin{itemize} +\item Collide $e^+ e^-$ with energy $90-400~{\rm GeV}$. +\item The third option is the $p-e$ is also on the table. +\end{itemize} +\end{itemize} + + +\column{0.5\textwidth} +\includegraphics[width=1.0\textwidth]{tunel} + +\end{columns} +\includegraphics[width=0.2\textwidth]{tunel2.png} +\includegraphics[width=0.8\textwidth]{geo.png} + +\textref{M.Benedikt, J. Osborne, C. Cook} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Why FCCee?} +\begin{columns} +\column{0.35\textwidth} +\begin{itemize} +\item FCCee is also a $Z$-factory! +\item Current design produces $2.5 \times 10^{12}$ $Z$ peer year! +\item We all love $Z$: +\begin{itemize} +\item LFV: $Z \to \ell \ell^{\prime}$. +\item $\mathcal{O}(10^{12}) \rm{ b\bar{b}}$, flavour factory. +\end{itemize} +\end{itemize} + + +\column{0.65\textwidth} +\includegraphics[width=1.0\textwidth]{lumi} + +\end{columns} +\textref{A. Blondel} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Sterile neutrinos} + +\ARROW There are 3 missing pieces missing:\\ +\begin{center} +\includegraphics[width=0.95\textwidth]{netrino.png} + +\end{center} +\ARROW The neutrinos have masses (no one knows from where).\\ +\ARROW New degrees of freedom needed! + +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{RHNS, at $Z$ threshold} + +\ARROW Production: +\begin{small} +\begin{align*} +BR(Z \to \nu \nu_m) = 2 \times BR(Z \to \nu \bar{\nu}) \sum_i \vert U_{im} \vert^2 \left(1- \frac{m^2_{\nu_m}}{m^2_Z} \right)^2 \left(1 + \frac{1}{2} \frac{m^2_{\nu_m}}{m^2_Z} \right)^2 +\end{align*} +\end{small} +\pause +\begin{exampleblock}{Decays} +\begin{columns} +\column{0.5\textwidth} +\begin{center} +\includegraphics[width=0.9\textwidth]{HNL.png} + +\end{center} +\column{0.5\textwidth} +Decay Lenght: +\begin{align*} +L=\frac{3~{\rm cm}}{ \vert U \vert^2 \left( m_{\nu_m} [{\rm GeV/c^2}] \right)^6} +\end{align*} + +\end{columns} + +\end{exampleblock} +\ARROW Possible backgrounds: +\begin{align*} +e^+ e^- \to W^{\ast +} W^{\ast -}, Z(\nu\nu) + Z^{\ast}/\gamma +\end{align*} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{RHNS, at $Z$ threshold} +\ARROW Expected sensitivity: +{~}\\ + +\begin{columns} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{exclusion} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{eventdisplay2} + + +\end{columns} + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{FCCee conclusions} + +\ARROW FCCee is one of the future colliders that are on the table.\\ +\ARROW I deal environment to do flavour physics!\\ +\ARROW Can reach the $\vert U \vert^2$ up to $10^{-11}$.\\ +\ARROW Now is the right time to plan physics of 2035-2040: + +\begin{center} +\includegraphics[width=0.8\textwidth]{time.png} + +\end{center} + +\end{frame} + + + + + + + + \backupbegin @@ -1130,6 +1273,15 @@ \includegraphics[width=0.8\textwidth]{susy/sps7.png} \end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{} + +\begin{center} +\includegraphics[width=0.9\textwidth]{newlimits} +\end{center} + +\end{frame} + diff --git a/NuFact_2016/LongLive/mchrzasz2.pdf b/NuFact_2016/LongLive/mchrzasz2.pdf new file mode 100644 index 0000000..515c4fb --- /dev/null +++ b/NuFact_2016/LongLive/mchrzasz2.pdf Binary files differ diff --git a/NuFact_2016/LongLive/netrino.png b/NuFact_2016/LongLive/netrino.png new file mode 100644 index 0000000..66931cc --- /dev/null +++ b/NuFact_2016/LongLive/netrino.png Binary files differ diff --git a/NuFact_2016/LongLive/newlimits.png b/NuFact_2016/LongLive/newlimits.png new file mode 100644 index 0000000..50d3b3c --- /dev/null +++ b/NuFact_2016/LongLive/newlimits.png Binary files differ diff --git a/NuFact_2016/LongLive/time.png b/NuFact_2016/LongLive/time.png new file mode 100644 index 0000000..143bdf9 --- /dev/null +++ b/NuFact_2016/LongLive/time.png Binary files differ diff --git a/NuFact_2016/LongLive/tunel.png b/NuFact_2016/LongLive/tunel.png new file mode 100644 index 0000000..a2cca0b --- /dev/null +++ b/NuFact_2016/LongLive/tunel.png Binary files differ diff --git a/NuFact_2016/LongLive/tunel2.png b/NuFact_2016/LongLive/tunel2.png new file mode 100644 index 0000000..1160954 --- /dev/null +++ b/NuFact_2016/LongLive/tunel2.png Binary files differ