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100644 --- a/SM@LHC/mchrzasz.pdf +++ b/SM@LHC/mchrzasz.pdf Binary files differ diff --git a/SM@LHC/mchrzasz.snm b/SM@LHC/mchrzasz.snm index fdd20d8..f85d7b6 100644 --- a/SM@LHC/mchrzasz.snm +++ b/SM@LHC/mchrzasz.snm @@ -1,2 +1,2 @@ -\beamer@slide {Js}{40} -\beamer@slide {LargeRecoilAs}{41} +\beamer@slide {Js}{57} +\beamer@slide {LargeRecoilAs}{58} diff --git a/SM@LHC/mchrzasz.synctex.gz b/SM@LHC/mchrzasz.synctex.gz index 2ab35a6..34ebb88 100644 --- a/SM@LHC/mchrzasz.synctex.gz +++ b/SM@LHC/mchrzasz.synctex.gz Binary files differ diff --git a/SM@LHC/mchrzasz.tex b/SM@LHC/mchrzasz.tex index c8f8fde..c62f316 100644 --- a/SM@LHC/mchrzasz.tex +++ b/SM@LHC/mchrzasz.tex @@ -507,6 +507,7 @@ \item CP violation in kaons. \item $V_{ub}$. \end{itemize} +\item Tetra\&Pentaquarks \end{itemize} @@ -1246,25 +1247,44 @@ \begin{frame}{Mixing induced CPV in $\PBs$} {~} -\begin{small} +\begin{footnotesize} + \begin{minipage}{\textwidth} -\ARROW Interference between $\PBs$ decaying to $\PJpsi \Pphi$ either directly or by oscillations gives rise to CP violation phase: $\phi_s^{\PJpsi \Pphi}$ +\ARROW Unbinned maximum likelihood fit (time, mass, angles, initial flavour): \begin{center} -\includegraphics[width=0.85\textwidth]{images/phis.png} +\includegraphics[width=0.6\textwidth]{images/Bsmix.png} \end{center} -\ARROW In the Sm $\phi_s \approx -2 \beta+s = -(0.0376^{+0.0007}_{-0.0008})~\rm rad$, where $\beta_s=\arg \left(- \frac{V_{ts}V_{tb}^{\ast}}{V_{cs} V_{cb}^{\ast}} \right)$\\ -\ARROW At the leading order the same phase is expected $\PBs \to \PDs \PDs$ and $\PB \to \PJpsi \Ppi \Ppi$.\\ -\ARROW NP can enter in the $\PBs$ mixing!\\ -\ARROW Measured by simultaneous fit to $\PBs$ and $\bar{\PBs}$ decay rates: -\begin{center} -\includegraphics[width=0.9\textwidth]{images/phis2.png} - -\end{center} +\begin{itemize} +\item $\phi_s=-0.058 \pm 0.049 \pm 0.006$ rad. +\item $\Gamma_s=(\Gamma_L+\Gamma_H)/2=0.6603\pm 0.0027 \pm 0.0015~ {\rm ps}^{-1}$ +\item $\Delta \Gamma_s=\Gamma_L-\Gamma_H=0.0805 \pm 0.0091 \pm 0.0032~ {\rm ps}^{-1}$ +\item Combined with $\PBs \to \PJpsi \pi \pi$: $\phi_s=-0.010 \pm 0.039$ rad. +\end{itemize} \end{minipage} - \end{small} +\end{footnotesize} +\textref{PRL 114, 041801 (2015)} + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{Mixing induced CPV in $\PBs$} +{~} +\begin{footnotesize} + +\begin{center} +\includegraphics[width=0.7\textwidth]{images/hfagccs.png} +\end{center} +\ARROW LHCb is dominating the world average!\\ +\ARROW $\phi_s^{ \rm HFAG}=-0.034 \pm 0.033$.\\ +\ARROW Compatible with SM, but there is still plenty room for NP!\\ +\ARROW Penguin pollution constrained from $\PBzero \to \PJpsi \Prho$ and $\PBs \to \PJpsi \bar{\PKstar}$ + +\end{footnotesize} \vspace*{2.1cm} \end{frame} @@ -1272,6 +1292,342 @@ +\begin{frame}{$V_{ub}$} +{~} +\begin{footnotesize} + +\ARROW Since a long time the smallest of the CKM matrix elements $V_{ub}$ has been determined in two ways: +\begin{itemize} +\item inclusively: $\Pbeauty \to \Pup \ell \nu$, $\vert V_{ub} \vert=(4.41 \pm 0.15^{+0.15}_{-0.17})\times 10^{-3}$ +\item exclusively: $\PB \to \pi \ell \nu$, $\vert V_{ub} \vert=(3.28 \pm 0.29)\times 10^{-3}$ +\item $3~\sigma$ tensions! +\end{itemize} +\ARROW LHCb perspectively enters the game with baryons decay: $\PLambdab \to \Pproton \mu \nu$. +\begin{center} +\includegraphics[width=0.45\textwidth]{images/vub.png} +\end{center} +where $R_{FF}$ is a ratio of form factors, that can be calculated using lattice QCD [rxiv:1503.01421]. +\end{footnotesize} + +\textref{Nature Physics 11, 743-747 (2015)} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{$V_{ub}$} +{~} +\begin{footnotesize} + +\ARROW $\vert V_{ub}\vert = (3.27 \pm0.15 \pm 0.16 \pm 0.06(V_{cb})) \times 10^{-3}$ + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/vub2.png} +\end{center} + +\begin{itemize} +\item LHCbs measurement makes the discrepancy larger and is spot on the Exclusive B-factories results. +\item Disfavor NP models with significant right handed current +\item Debatable world averages, depending on the input used (theory, BR of control mode, ...) +\end{itemize} + + + +\end{footnotesize} + +\textref{Nature Physics 11, 743-747 (2015)} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{CP violation in charm} +{~} +\begin{footnotesize} + +\ARROW The $A_{CP}$ asymmetry is defined as: +\begin{align*} +A_{CP}(\PDzero \to f) = \frac{\Gamma(\PDzero \to f)-\Gamma(\bar{\PDzero} \to f) }{\Gamma(\PDzero \to f)+\Gamma(\bar{\PDzero} \to f) },~~~f=\PK^+ \PK^- ,\Ppi^+ \Ppi^- +\end{align*} +\begin{center} +\includegraphics[width=0.65\textwidth]{images/charmCP.png} +\end{center} +\ARROW New world average: +\begin{align*} +a_{CP}^{ \rm ind}=(0.056 \pm 0.040)\% \\ +a_{CP}^{ \rm dir}=(-0.137 \pm 0.070)\% +\end{align*} +\ARROW Results consistent with no CPV at $6.5~\%$ CL. +\end{footnotesize} + +\textref{LHCb-PAPER-2015-055, PLB 753 (2016) 412} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Direct CPV in kaons} +{~} +\begin{small} +\ARROW 1999: Discovery of CP violation in $\PK \to \pi \pi$ (NA48, KTeV).\\ +\ARROW 2001: Combined experimental average of the two above experiments: $\Re (\epsilon^{\prime}/ \epsilon )=(16.6\pm 2.3)~\%$, compatible with SM. Experimental precision much better than the theoretical prediction.\\ +\ARROW 2015: Fantastic progresses in lattice QCD. Can now compute all relevant long-distance effects that used to dominate the theoretical uncertainty: + +\begin{align*} +\Re (\epsilon^{\prime}/ \epsilon )=(1.9 \pm 4.5)\times 10^{-4} +\end{align*} + +\ARROW A brand new $2.9~\sigma$ tension arrives!\\ +\ARROW A.Buras, et.al. [JHEP03(2016)010] This discrepancy can be linked to aforementioned $\Pbeauty \to \Pstrange \ell \ell$ anomalies. \\ +\ARROW Good lattice prospects to improve even further the theoretical uncertainty + +\end{small} +\textref{A. Buras et al, arXiv:1507.06345} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{Global CKM fit} +{~} +\begin{center} +\includegraphics[width=0.95\textwidth]{images/CKMfit.png} +\end{center} + +\ARROW Excellent consistency of the various CKM measurements so far! + + +\textref{\url{http://ckmfitter.in2p3.fr}} + + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame} +\begin{center} +\begin{Huge} +Tetra\&Petraquarks + +\end{Huge} +\end{center} + + \vspace*{2.1cm} +\end{frame} + + + + + +\begin{frame}{Tetra\&Petraquarks} +{~} +\ARROW Idea of this multi quark states started in the $1960$s: +\begin{center} +\includegraphics[width=0.7\textwidth]{images/gelman.png} +\end{center} +\ARROW Searches for years and many “discoveries” not confirmed + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{X(3872)} +{~} +\begin{footnotesize} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{2.5in} +\ARROW First observed by Belle in $\PB^+ \to X(\PJpsi \pi \pi) \PK^+$, above the $\PUpsilon(2S)$. [PRL 91 (2003) 262001]\\ +\ARROW Confirmed by several experiments: BaBar, CDF, D0, LHCb, CMS.\\ +\ARROW LHCb determined its quantum numbers: $J^{PC}=1^{++}$ using angular analysis [PRL 110, 222001 (2013)].\\ +{~}\\ +\ARROW The nature of this state is still unclear. It is compatible with a tetraquark, $\PD\PDstar$ molecule or a $\chi_{c1}(2^3P_1)$ hypothesis.\\ +\ARROW Never LHCb measurements disfavour the $\PD\PDstar$ molecule by $4.4~\sigma$ [Nucl. Phys. B886 (2014) 665]. + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{images/x3872.png} +\end{columns} +\end{footnotesize} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{$Z(4430)^-$} +{~} +\begin{footnotesize} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{2.5in} +\ARROW $Z(4430)^-$ special “tetraquark candidate”,because charged: cannot be a $\Pcharm \bar{\Pcharm}$ state!\\ +\ARROW Belle discovered it in $\PBzero \to \PUpsilon(2S)\PK \Ppi$, with evidence of $J^{P}=1^+$ [PRD 88 (2013) 074026]. \\ +\ARROW Using method of moments, Babar claimed they do not need the $Z(4430)^-$ to described their data [PRD 79 (2009) 112001].\\ +\ARROW LHCb reproduced BaBar moments analysis with the full Run1 sample ($3~\invfb$) and clearly something mote was needed to describe the data [PRL 112, 222002 (2014)].\\ + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{images/Z4430.png} +\end{columns} +\end{footnotesize} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{$Z(4430)^-$} +{~} +\begin{footnotesize} +\ARROW LHCb unbinned amplitude analysis of $\PBzero \to \Ppsi(2S) \PK^+ \Ppi^-$, $m=4475 \pm 7 ^{+15}_{-25}~\MeV/c^2$, $\Gamma=172 \pm 13^{37}_{34}~\MeV/c^2$\\ +\ARROW $J^P$ is confirmed to be $1^+$ and Argand plot shows the typical pattern for resonances.\\ +\ARROW Minimal quark content $\Pcharm \APcharm \Pdown \APup$. + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Z44301.png} +\end{center} + + +\end{footnotesize} +\textref{LHCb, PRL 112, 222002 (2014)} + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\ARROW $\PLambdab \to \PJpsi \Pproton \PK$ was studied initially for a precise $\PLambdab$ lifetime .\\ +\ARROW Close look at the Dalitz: $m(\PK\Pproton)-m(\PJpsi \Pproton)$ +\begin{itemize} +\item $m(\PK\Pproton)$ has a rich structure of excited $\PLambda$ states. +\item $m(\PJpsi \Pproton)$ has something inside! +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/penta.png} +\end{center} + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\ARROW Super complex fit needed to describe the data: $5$ decay angles, $14$ possible $\PLambda^{\ast}$ resonances for $m(\PK \Ppi)$ and two brand new pentaquarks for $m(\PJpsi \Pproton)$: +\begin{itemize} +\item $P_c(4380)^+$: $4380\pm 8 \pm 29~\MeV/c^2$, $\Gamma=205 \pm 18 \pm 86~\MeV/c^2$, $J^P=\frac{3}{2}^-$ +\item $P_c(4450)^+$: $4449,8\pm 1.7 \pm 2.5~\MeV/c^2$, $\Gamma=39 \pm 5 \pm 19~\MeV/c^2$, $J^P=\frac{5}{2}^+$ +\end{itemize} + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/penta2.png} +\end{center} + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + + + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\begin{columns} +\column{3in} +\begin{itemize} +\item Angrad plots show the phase motion for the resonances. +\item The $P_c(4380)$ has one point off by a $2\sigma$. +\end{itemize} + +\column{2in} +\begin{itemize} +\item The interference patterns confirm the opposite parities. +\end{itemize} + +\end{columns} +\begin{center} +\includegraphics[width=0.99\textwidth]{images/penta3.png} +\end{center} + +\ARROW The significance was evaluated with a TOY MC: +\begin{itemize} +\item $P_c(4380)^+:~9\sigma$ +\item $P_c(4450)^+:~12\sigma$ +\end{itemize} +\ARROW The states are consistent with $\Pcharm \APcharm \Pup \Pup \Pdown$.\\ + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{Conclusions} +{~} +\begin{small} + +\ARROW Flavour physics is still playing an important role for hunting new physics!\\ +\ARROW Anomalies in the electroweak penguin and lepton universality combine to over $4\sigma$ significance discrepancy for NP.\\ +\ARROW The dominant anomaly was recently confirmed by Belle experiment.\\ +\ARROW $\gamma$ angle combination from LHCb is now two times more precise then the B-factories.\\ +\ARROW After $50$ years after the first prof. Gelman paper the pentraquark states have been observed.\\ +\ARROW Stay tuned as there are plenty of more results in the pipe line! + + + +\end{small} + + \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