Additional work on intro talk and changes latex generation to use rubber

CMakeLists.txt

@@ -70,7 +70,7 @@ IF(DOXYGEN_FOUND)
     )
 ENDIF(DOXYGEN_FOUND)
 
-ADD_SUBDIRECTORY(docs/intro/)
+ADD_SUBDIRECTORY(docs/)
 
 FIND_PACKAGE(ROOT REQUIRED)
 INCLUDE_DIRECTORIES( SYSTEM ${ROOT_INCLUDE_DIR} ${CMAKE_CURRENT_SOURCE_DIR})

docs/CMakeLists.txt

@@ -0,0 +1,6 @@
+
+ADD_CUSTOM_TARGET(intro
+                  rubber --into ${CMAKE_BINARY_DIR}/docs/intro/ intro.tex
+                  WORKING_DIRECTORY ${CMAKE_SOURCE_DIR}/docs/intro
+                  COMMENT "Build intro presentation with rubber"
+                  )

docs/intro/CMakeLists.txt

@@ -1,22 +0,0 @@
-# FIND_PACKAGE(LATEX)
-SET(LATEX_DEFAULT_BUILD pdf)
-SET(PDFLATEX_COMPILER xelatex)
-INCLUDE(${CMAKE_SOURCE_DIR}/cmake/UseLATEX.cmake)
-
-IF(LATEX_COMPILER)
-
-##############################################################################
-    SET(LATEX_OUTPUT_PATH ${CMAKE_BINARY_DIR}/intro)
-    ADD_LATEX_DOCUMENT(intro.tex
-                       INPUTS beamerthemebjeldbak.sty
-                       IMAGE_DIRS  . figures
-                       # Add the feynman diagrams manually because UseLATEX wants to 
-                       # generate the pngs if the eps files are included
-                       IMAGES figures/feynman-diagrams/T-b_W-ln.png
-                              figures/feynman-diagrams/T-b_W.png
-                              figures/feynman-diagrams/T-b_W-qq.png )
-##############################################################################
-
-ELSE(LATEX_COMPILER)
-    MESSAGE(STATUS "No LaTeX found, cannot compile LaTeX documents")
-ENDIF(LATEX_COMPILER)

docs/intro/beamerthemebjeldbak.sty

@@ -33,13 +33,13 @@
 % \fi%
 
 % Display a slide before the current section with overview inf
-\AtBeginSection[]
-{%
-   \begin{frame}
-       \frametitle{Overview}
-       \tableofcontents[currentsection,hideothersubsections]
-   \end{frame}
-}
+% \AtBeginSection[]
+% {%
+%    \begin{frame}
+%        \frametitle{Overview}
+%        \tableofcontents[currentsection,hideothersubsections]
+%    \end{frame}
+% }
 
 \setbeamerfont{title like}{shape=\scshape}
 \setbeamerfont{frametitle}{shape=\scshape}

docs/intro/intro.tex

@@ -1,194 +1,89 @@
+
+% rubber: module pdftex
+
 \documentclass[english,aspectratio=169]{beamer}
-\usepackage{fontspec}
 \usepackage{graphicx}
 \usepackage{amssymb}
 \usepackage{booktabs}
 \usepackage{siunitx}
+\usepackage{subcaption}
+\usepackage{marvosym}
+\usepackage[space]{grffile} % allows for spaces in filenames in \includegraphics
 
-% \setmainfont[Mapping=tex-text]{DejaVu Serif}
-% \setsansfont[Mapping=tex-text]{DejaVu Sans}
-% \setmonofont{DejaVu Sans Mono}
-
+\newcommand{\pb}{\si{\pico\barn}}%
 \newcommand{\fb}{\si{\femto\barn}}%
 \newcommand{\invfb}{\si{\per\femto\barn}}
 
 \newcommand{\GeV}{\si{\giga\electronvolt}}
 
+\newcommand{\specialcell}[2][c]{%
+  \begin{tabular}[#1]{@{}c@{}}#2\end{tabular}}
+
+\newcommand{\beginbackup}{%
+   \newcounter{framenumbervorappendix}
+   \setcounter{framenumbervorappendix}{\value{framenumber}}
+}
+\newcommand{\endbackup}{%
+   \addtocounter{framenumbervorappendix}{-\value{framenumber}}
+   \addtocounter{framenumber}{\value{framenumbervorappendix}}
+}
+
 \usetheme[]{bjeldbak}
 
 \begin{document}
 
 \title[4t X-Section]{Four Tops X Section Measurement}
-
-\subtitle{Trilepton Channel}
-
+\subtitle{Trilepton Channel ($\mu^+\mu^-e, e^+e^-\mu$) }
 \author[C. Fangmeier]{Caleb Fangmeier}
-
 \institute[UNL]{University of Nebraska \-- Lincoln}
-
 \date{\today}
 
 \titlegraphic{%
 \begin{figure}
-  \includegraphics[width=1in]{CMSlogo.png}\hspace{0.75in}\includegraphics[width=1in]{nebraska-n}
+  \includegraphics[width=1in]{CMSlogo.png}\hspace{0.75in}\includegraphics[width=1in]{nebraska-n.png}
 \end{figure}
 }
 
-\begin{frame}[plain]
+\begin{frame}[noframenumbering,plain]
   \titlepage%
 \end{frame}
 
 \section{Introduction}
-\begin{frame}{Production}
-  \begin{minipage}[c][\textheight]{0.45\textwidth}
-    \begin{itemize}
-      \item 4-top production can proceed through either
-        \begin{itemize}
-          \item<2,5-> $\mathcal{O}(\alpha_S^4)$ QCD Process
-          \item<3,5-> $\mathcal{O}(\alpha_S^2 y_t^2)$ Higgs Exchange
-          \item<4,5-> $\mathcal{O}(\alpha_S^2\alpha^2)$ Electroweak Process
-        \end{itemize}
-      \item<5-> Higgs Exchange + EW gives $\approx10\%$ contribution to total cross-section.
-    \end{itemize}
-  \end{minipage}
-  \begin{minipage}[c][\textheight]{0.45\textwidth}
-    \centering
-    \only<2>{%
-      \includegraphics[width=\textwidth]{figures/production-qcd}
-    }
-    \only<3>{%
-      \includegraphics[width=\textwidth]{figures/production-higgs}
-    }
-    \only<4>{%
-      \includegraphics[width=\textwidth]{figures/production-ew}
-    }
-    \only<5>{%
-      Standard Model cross-section at $\sqrt{s}=13\mathrm{TeV}$:
-      \begin{center}
-        \Huge{12.32\fb}
-      \end{center}
-    }
-    \only<6->{%
-      Standard Model cross-section at $\sqrt{s}=13\mathrm{TeV}$:
-      \vspace{-.15in}
-      \begin{center}
-        \Large{12.32\fb}
-      \end{center}
-      \includegraphics[width=\textwidth]{figures/lhc-luminosity-2016}
-      % IMGSRC: https://home.cern/cern-people/updates/2016/12/lhc-report-far-beyond-expectations
-      \vspace{-.15in}
-      \begin{equation*}
-        \mathrm{\#\ Signal\ Events}=12.32\fb * 40\invfb \approx 493
-      \end{equation*}
-    }
-  \end{minipage}
-\end{frame}
-
-\begin{frame}{Decay Channels}
-  \begin{minipage}[c][\textheight]{0.45\textwidth}
-    \begin{itemize}
-        %TODO: Check the limits on non-bW decays
-      \item<1-> All* tops will immediately decay to a b-quark and a W-boson
-      \item<2-> The W-boson will immediately decay either
-        \begin{itemize}
-          \item<2,4-> \textbf{Leptonically}
-          \item<3-> \textbf{Hadronically}
-        \end{itemize}
-      \item<4-> The b-quark will form some b hadron, travel some macroscopic distance, and then hadronize into a jet.
-    \end{itemize}
-  \end{minipage}
-  \begin{minipage}[c][\textheight]{0.54\textwidth}
-    \centering
-    \only<1>{%
-      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W.png}
-    }
-    \only<2>{%
-      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W-ln.png}
-    }
-    \only<3>{%
-      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W-qq.png}
-    }
-    \only<4>{%
-      \includegraphics[width=0.90\textwidth]{figures/b-tagging}
-    }
-  \end{minipage}
-\end{frame}
+\input{slides/introduction.tex}
+\input{slides/decay_channels_rates.tex}
 
 
-\begin{frame}{Decay Channels}
-  The Decay channels are enumerated based on the types of W-decays
-\begin{table}[]
-  \tiny
-  \begin{tabular}{@{}llccrrc@{}}
-    \textbf{Name}               & \textbf{Leptons}           & \textbf{B-Jets} & \textbf{LF-Jets} & \textbf{BR}     & \textbf{BR ($\mu$ and $e$ only)} & \textbf{Events @ 40\invfb}    \\ \midrule
-  Hadronic                    &                            & 4               & 8                & 20\%            & 20\%                             & 99                               \\ \midrule
-  Single Lepton               & $\ell^\pm$                 & 4               & 6                & 40\%            & 26.6\%                           & 131                              \\ \midrule
-  Same-Sign (SS) Dilepton     & $\ell^\pm \ell^\pm$        & 4               & 4                & 9.7\%           & 4.3\%                            & 21                               \\ \midrule
-  Opposite-Sign (OS) Dilepton & $\ell^\pm \ell^\mp$        & 4               & 4                & 19.3\%          & 8.6\%                            & 42                               \\ \midrule
-  Trilepton                   & $\ell^\pm\ell^\pm\ell^\mp$ & 4               & 2                & 9.8\%           & 2.9\%                            & 14                               \\ \midrule
-  Leptonic                    & $\ell^+\ell^+\ell^-\ell^-$ & 4               & 2                & 1.2\%           & 0.24\%                           & 1                                \\ \bottomrule
-  \end{tabular}
-\end{table}
-\vfill
-\footnotesize{$\ell \in \left(e,\mu,\tau\right)$}
-\end{frame}
 
-\section{Previous Measurements}
-\begin{frame}{Previous CMS Measurements @ 13TeV}
-\begin{table}[]
-  \begin{tabular}{@{}lcr@{}}
-  \textbf{Analysis}           & \textbf{Channel}            & \textbf{Limit}  \\ \midrule
-  CMS-TOP-16-016              & Single Lepton, OS Dilepton  & 94\fb          \\ \midrule%
-  CMS-SUS-15-008              & SS Dilepton                 & 119\fb         \\ \bottomrule%
-  \textbf{Combined}           &                             & 69\fb          \\%
-  \end{tabular}
-\end{table}
-\end{frame}
 
 \section{Strategy}
-\begin{frame}{Backgrounds (Irreducible)}
-  \begin{center}
-    \includegraphics[width=0.8\textwidth]{figures/irreducible-backgrounds}
-  \end{center}
-\end{frame}
+\input{slides/strategy.tex}
+\input{slides/irreducible_backgrounds.tex}
+\input{slides/reducible_backgrounds.tex}
 
-\begin{frame}{Backgrounds (Reducible)}
-  \begin{center}
-    \includegraphics[width=0.8\textwidth]{figures/reducible-backgrounds}
-  \\
-  Here, $\epsilon=10^{-4}$, but will need to be corrected to measured value for CMS
-  \end{center}
-\end{frame}
 
-\begin{frame}{Strategy}
-  \begin{minipage}[c][\textheight]{0.49\textwidth}
-    \small
-    \begin{itemize}
-      % \item Take advantage of the existing N-Tuples created by the TTH-Multilepton analysis
-      \item Use the baseline selection from\cite{}
-      \begin{itemize}
-        \item Exactly three charged leptons ($e$ or $\mu$) passing mini-isolation criteria ($R_0=0.5, p_{T_0}=7.5\GeV$)
-        \item Jet multiplicity $N_j \ge 4$
-        \item B-Jet multiplicity $N_j \ge 3$
-        \item Z-mass window veto: $M_{\ell^+\ell^-} \notin (70\GeV,105\GeV)$
-      \end{itemize}
-      \item Further breakdown into signal regions based on $N_j$
-    \end{itemize}
-  \end{minipage}
-  \begin{minipage}[c][\textheight]{0.49\textwidth}
-    \begin{center}
-      \includegraphics[width=\textwidth]{figures/event-yields}
-    \end{center}
-  \end{minipage}
-\end{frame}
 
+\section{Some Preliminary Plots}
+\input{slides/progress_and_status.tex}
+\input{slides/prelim_plots.tex}
 
-\section{Progress \& Status}
-\begin{frame}{Progress \& Status}
-\end{frame}
+\section{Timeline}
+\input{slides/timeline.tex}
+
+\input{slides/references.tex}
 
-\section{Conclusions}
-\begin{frame}{Conclusions}
+\beginbackup%
+\section{Backups}
+
+\begin{frame}
+  \huge
+  \centering
+  Backups
 \end{frame}
 
+\input{slides/production.tex}
+\input{slides/decay_channels.tex}
+\input{slides/previous_measurements.tex}
+
+\endbackup%
+
 \end{document}

docs/intro/live_figures

@@ -0,0 +1 @@
+../../python/figures

docs/intro/slides/decay_channels.tex

@@ -0,0 +1,30 @@
+
+\begin{frame}{Decay Channels}
+  \begin{minipage}[c][\textheight]{0.45\textwidth}
+    \begin{itemize}
+        %TODO: Check the limits on non-bW decays
+      \item<1-> All* tops will immediately decay to a b-quark and a W-boson
+      \item<2-> The W-boson will immediately decay either
+        \begin{itemize}
+          \item<2,4-> \textbf{Leptonically}
+          \item<3-> \textbf{Hadronically}
+        \end{itemize}
+      \item<4-> The b-quark will form some b hadron, travel some macroscopic distance, and then hadronize into a jet.
+    \end{itemize}
+  \end{minipage}
+  \begin{minipage}[c][\textheight]{0.54\textwidth}
+    \centering
+    \only<1>{%
+      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W.png}
+    }
+    \only<2>{%
+      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W-ln.png}
+    }
+    \only<3>{%
+      \includegraphics[width=\textwidth]{figures/feynman-diagrams/T-b_W-qq.png}
+    }
+    \only<4>{%
+      \includegraphics[width=0.90\textwidth]{figures/b-tagging}
+    }
+  \end{minipage}
+\end{frame}

docs/intro/slides/decay_channels_rates.tex

@@ -0,0 +1,18 @@
+
+\begin{frame}{Decay Channels}
+  The Decay channels are enumerated based on the types of W-decays
+\begin{table}[]
+  \tiny
+  \begin{tabular}{@{}llccrrc@{}}
+    \textbf{Name}               & \textbf{Leptons}           & \textbf{B-Jets} & \textbf{LF-Jets} & \textbf{BR}     & \textbf{BR ($\mu$ and $e$ only)} & \textbf{Events @ 40\invfb}    \\ \midrule
+  Hadronic                    &                            & 4               & 8                & 20\%            & 20\%                             & 99                               \\ \midrule
+  Single Lepton               & $\ell^\pm$                 & 4               & 6                & 40\%            & 26.6\%                           & 131                              \\ \midrule
+  Same-Sign (SS) Dilepton     & $\ell^\pm \ell^\pm$        & 4               & 4                & 9.7\%           & 4.3\%                            & 21                               \\ \midrule
+  Opposite-Sign (OS) Dilepton & $\ell^\pm \ell^\mp$        & 4               & 4                & 19.3\%          & 8.6\%                            & 42                               \\ \midrule
+  Trilepton                   & $\ell^\pm\ell^\pm\ell^\mp$ & 4               & 2                & 9.8\%           & 2.9\%                            & 14                               \\ \midrule
+  Leptonic                    & $\ell^+\ell^+\ell^-\ell^-$ & 4               & 2                & 1.2\%           & 0.24\%                           & 1                                \\ \bottomrule
+  \end{tabular}
+\end{table}
+\vfill
+\footnotesize{$\ell \in \left(e,\mu,\tau\right)$}
+\end{frame}

docs/intro/slides/introduction.tex

@@ -0,0 +1,6 @@
+\begin{frame}{Introduction}
+  \begin{itemize}
+    \item Beginning investigation of trilepton channel
+    \item Specifically the $\mu^+\mu^-e, e^+e^-\mu$ final states
+  \end{itemize}
+\end{frame}

docs/intro/slides/irreducible_backgrounds.tex

@@ -0,0 +1,6 @@
+
+\begin{frame}{Backgrounds (Irreducible)}
+  \begin{center}
+    \includegraphics[width=0.8\textwidth]{figures/irreducible-backgrounds}
+  \end{center}
+\end{frame}

docs/intro/slides/prelim_plots.tex

@@ -0,0 +1,27 @@
+
+\begin{frame}
+  \centering
+  % ROW 1
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+      \includegraphics[width=\textwidth]{live_figures/Jet Multiplicity N_lep3.png}
+  \end{minipage}
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+    \includegraphics[width=\textwidth]{live_figures/Jet Multiplicity e+e-mu.png}
+  \end{minipage}
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+    \includegraphics[width=\textwidth]{live_figures/Jet Multiplicity mu+mu-e.png}
+  \end{minipage}
+
+  % ROW 2
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+    \includegraphics[width=\textwidth]{live_figures/B-Jet Multiplicity N_lep3.png}
+  \end{minipage}
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+    \includegraphics[width=\textwidth]{live_figures/B-Jet Multiplicity e+e-mu.png}
+  \end{minipage}
+  \begin{minipage}[c][0.48\textheight]{0.32\textwidth}
+    \includegraphics[width=\textwidth]{live_figures/B-Jet Multiplicity mu+mu-e.png}
+  \end{minipage}
+  \footnotesize
+  Note that there is an overestimation of the jet counts as the lepton-tau-jet cross-cleaning still needs to be done.
+\end{frame}

docs/intro/slides/previous_measurements.tex

@@ -0,0 +1,11 @@
+
+\begin{frame}{Previous CMS Measurements @ 13TeV}
+\begin{table}[]
+  \begin{tabular}{@{}lcr@{}}
+  \textbf{Analysis}           & \textbf{Channel}            & \textbf{Limit}  \\ \midrule
+  CMS-TOP-16-016              & Single Lepton, OS Dilepton  & 94\fb          \\ \midrule%
+  CMS-SUS-15-008              & SS Dilepton                 & 119\fb         \\ \bottomrule%
+  \textbf{Combined}           &                             & 69\fb          \\%
+  \end{tabular}
+\end{table}
+\end{frame}

docs/intro/slides/production.tex

@@ -0,0 +1,45 @@
+
+\begin{frame}{Production}
+  \begin{minipage}[c][\textheight]{0.45\textwidth}
+    \begin{itemize}
+      \item 4-top production can proceed through either
+        \begin{itemize}
+          \item<2,5-> $\mathcal{O}(\alpha_S^4)$ QCD Process
+          \item<3,5-> $\mathcal{O}(\alpha_S^2 y_t^2)$ Higgs Exchange
+          \item<4,5-> $\mathcal{O}(\alpha_S^2\alpha^2)$ Electroweak Process
+        \end{itemize}
+      \item<5-> Higgs Exchange + EW gives $\approx10\%$ contribution to total cross-section.
+    \end{itemize}
+  \end{minipage}
+  \begin{minipage}[c][\textheight]{0.45\textwidth}
+    \centering
+    \only<2>{%
+      \includegraphics[width=\textwidth]{figures/production-qcd}
+    }
+    \only<3>{%
+      \includegraphics[width=\textwidth]{figures/production-higgs}
+    }
+    \only<4>{%
+      \includegraphics[width=\textwidth]{figures/production-ew}
+    }
+    \only<5>{%
+      Standard Model cross-section at $\sqrt{s}=13\mathrm{TeV}$:
+      \begin{center}
+        \Huge{12.32\fb{} \MVAt{} NLO}
+      \end{center}
+    }
+    \only<6->{%
+      Standard Model cross-section at $\sqrt{s}=13\mathrm{TeV}$:
+      \vspace{-.15in}
+      \begin{center}
+        \Large{12.32\fb{} \MVAt{} NLO}
+      \end{center}
+      \includegraphics[width=\textwidth]{figures/lhc-luminosity-2016}
+      % IMGSRC: https://home.cern/cern-people/updates/2016/12/lhc-report-far-beyond-expectations
+      \vspace{-.15in}
+      \begin{equation*}
+        \mathrm{\#\ Signal\ Events}=12.32\fb * 40\invfb \approx 493
+      \end{equation*}
+    }
+  \end{minipage}
+\end{frame}

docs/intro/slides/progress_and_status.tex

@@ -0,0 +1,26 @@
+
+\newcommand{\rarrow}{$\rightarrow$}
+\begin{frame}{Progress \& Status}
+  \centering
+  \footnotesize
+  \begin{itemize}
+    \item Acquired MC samples of signal and some relevant backgrounds
+    \item Basic framework written to easily make distributions of N-Tuple variables as well as values derived from them. \\
+      NTuple \rarrow{} (\texttt{filval} C++ Code) \rarrow{} \\
+      Root File with Histograms \rarrow{} (Python plotting routines) \rarrow{} \\
+      Plots in Jupyter Notebook
+  \end{itemize}
+
+  \tiny
+  \begin{tabular}{ll}
+  Sample Name                                                                                                    & X-section     \\
+  /TTTT\_TuneCUETP8M1\_13TeV-amcatnlo-pythia8/RunIISummer16MiniAODv2-PUMoriond17\_80X\                           & 0.009103\pb{} \\
+  \_mcRun2\_asymptotic\_2016\_TrancheIV\_v6-v1                                                                    &               \\
+  /TTWJetsToLNu\_TuneCUETP8M1\_13TeV-amcatnloFXFX-madspin-pythia8/RunIISummer16MiniAODv2-PUMoriond17\_80X\       & 0.2043\pb{}   \\
+  \_mcRun2\_asymptotic\_2016\_TrancheIV\_v6\_ext1-v3                                                              &               \\
+  /TTZToLLNuNu\_M-10\_TuneCUETP8M1\_13TeV-amcatnlo-pythia8/RunIISummer16MiniAODv2-PUMoriond17\_80X\              & 0.2529\pb{}   \\
+  \_mcRun2\_asymptotic\_2016\_TrancheIV\_v6\_ext1-v1                                                              &               \\
+  /ttHJetToNonbb\_M125\_13TeV\_amcatnloFXFX\_madspin\_pythia8\_mWCutfix/RunIISummer16MiniAODv2-PUMoriond17\_80X\ & 0.215\pb{}    \\
+  \_mcRun2\_asymptotic\_2016\_TrancheIV\_v6\_ext1-v1                                                              &               \\
+  \end{tabular}
+\end{frame}

docs/intro/slides/reducible_backgrounds.tex

@@ -0,0 +1,8 @@
+
+\begin{frame}{Backgrounds (Reducible)}
+  \begin{center}
+    \includegraphics[width=0.8\textwidth]{figures/reducible-backgrounds}
+  \\
+  Here, $\epsilon=10^{-4}$, but will need to be corrected to measured value for CMS
+  \end{center}
+\end{frame}

docs/intro/slides/references.tex

@@ -0,0 +1,6 @@
+\begin{frame}{References}
+  \begin{itemize}
+    \item \textbf{Analysis Code \& Results:}
+      \url{https://tttt.fangmeier.tech}
+  \end{itemize}
+\end{frame}

docs/intro/slides/strategy.tex

@@ -0,0 +1,15 @@
+
+\begin{frame}{Strategy}
+  \small
+  \begin{itemize}
+    \item Take advantage of the existing N-Tuples created by the TTH-Multilepton analysis
+    \item Use the following baseline selection
+    \begin{itemize}
+      \item Exactly three charged leptons $\in(\mu^+\mu^-e, e^+e^-\mu)$
+      \item Jet multiplicity $N_j \ge 4$
+      \item B-Jet multiplicity $N_j \ge 3$
+      \item Z-mass window veto: $M_{\ell^+\ell^-} \notin (70\GeV,105\GeV)$
+    \end{itemize}
+    \item Can then further breakdown into signal regions based on $N_j$ and other observables
+  \end{itemize}
+\end{frame}

docs/intro/slides/timeline.tex

@@ -0,0 +1,7 @@
+\begin{frame}{Timeline}
+  \begin{itemize}
+    \item Target Graduation: Spring 2019
+    \item $\rightarrow$ Primary Dataset 2016+2017(+top off with 2018)
+    \item I have comps starting next week and running for the next month
+  \end{itemize}
+\end{frame}