\documentclass[11pt]{scrbook} %\documentclass[12pt]{article} \usepackage{graphicx} \usepackage{amsmath} \usepackage{hhline} \usepackage{amssymb} \usepackage{times} \usepackage{cite} \usepackage{array} \usepackage{multirow} \usepackage{float} \usepackage{latexsym} \usepackage{epsfig} \usepackage{rotating} \usepackage{graphics} %\usepackage{francais} %\usepackage{french} \usepackage{mathrsfs} \usepackage{setspace} \usepackage{subfigure} %\usepackage{babel} \newcommand{\eVdist}{\kern-0.06667em} \newcommand{\gev}{{\,\text{Ge}\eVdist\text{V\/}}} \usepackage{color} \definecolor{rltred}{rgb}{0.75,0,0} \definecolor{rltgreen}{rgb}{0,0.5,0} \definecolor{rltblue}{rgb}{0,0,0.75} \newif\ifpdf \ifx\pdfoutput\undefined \pdffalse % we are not running PDFLaTeX \else \pdfoutput=1 % we are running PDFLaTeX \pdftrue \fi \ifpdf \usepackage{thumbpdf} \usepackage[pdftex, colorlinks=true, urlcolor=rltblue, % \href{...}{...} external (URL) filecolor=rltgreen, % \href{...} local file linkcolor=rltred, % \ref{...} and \pageref{...} pdftitle={Example File for pdflatex}, pdfauthor={H1}, pdfsubject={Template file}, pdfkeywords={High-Energy Physics, Particle Physics}, % pagebackref, pdfpagemode=None, bookmarksopen=true]{hyperref} \fi \renewcommand{\topfraction}{1.0} \renewcommand{\bottomfraction}{1.0} \renewcommand{\textfraction}{0.0} \newlength{\dinwidth} \newlength{\dinmargin} \setlength{\dinwidth}{21.0cm} \textheight23.5cm \textwidth16.0cm \setlength{\dinmargin}{\dinwidth} \setlength{\unitlength}{1mm} \addtolength{\dinmargin}{-\textwidth} \setlength{\dinmargin}{0.5\dinmargin} \oddsidemargin -1.0in \addtolength{\oddsidemargin}{\dinmargin} \setlength{\evensidemargin}{\oddsidemargin} \setlength{\marginparwidth}{0.9\dinmargin} \marginparsep 8pt \marginparpush 5pt \topmargin -42pt \headheight 12pt \headsep 30pt \footskip 24pt \parskip 3mm plus 2mm minus 2mm \newcommand{\myref}[2]{% \ifpdf \href{#1}{#2}\else #2 \fi% } %\input{notations} \begin{document} \rm \normalsize \thispagestyle{empty} \begin{table}[htb] \renewcommand{\arraystretch}{1.1} \begin{center} \begin{tabular}{|r||c|c||c|c|} \hline Electron & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline $P_T^X<12$~GeV & 5 & 6.40 $\pm$ 0.79 & 4.45 $\pm$ 0.70 & 1.95 $\pm$ 0.36 \\ \hline $1240$~GeV & 3 & 0.54 $\pm$ 0.11 & 0.45 $\pm$ 0.11 & 0.09 $\pm$ 0.04 \\ \hline \end{tabular} \end{center} \caption{Observed and predicted numbers of events in the electron channel for all $e^+p$ data.} \end{table} \begin{table}[htb] \renewcommand{\arraystretch}{1.1} \begin{center} \begin{tabular}{|r||c|c||c|c|} \hline Muon & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline $1240$~GeV & 3 & 0.55 $\pm$ 0.12 & 0.51 $\pm$ 0.12 & 0.04 $\pm$ 0.01 \\ \hline \end{tabular} \end{center} \caption{Observed and predicted numbers of events in the muon channel for all $e^+p$ data.} \end{table} \begin{table}[htb] \renewcommand{\arraystretch}{1.1} \begin{center} \begin{tabular}{|r||c|c||c|c|} \hline Electron and Muon & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline $P_{T}^{X}<12$~GeV & 5 & 6.40 $\pm$ 0.79 & 4.45 $\pm$ 0.70 & 1.95 $\pm$ 0.36 \\ \hline $1240$~GeV & 6 & 1.08 $\pm$ 0.22 & 0.96 $\pm$ 0.22 & 0.12 $\pm$ 0.04 \\ \hline \end{tabular} \end{center} \caption{Observed and predicted numbers of events in the electron and muon channels combined for all $e^+p$ data. Only the electron channel contributes for $P_{T}^{X}<12$ GeV.} \end{table} \newpage \begin{table}[htb] \renewcommand{\arraystretch}{1.1} \begin{center} \begin{tabular}{|r||c|c||c|c|} \hline {\bf Electron }& H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 10 & 9.85 $\pm$ 1.27 & 7.17 $\pm$ 1.17 & 2.68 $\pm$ 0.49 \\ \hline $P_{T}^{X}<25$~GeV & 6 & 8.36 $\pm$ 1.04 & 5.90 $\pm$ 0.94 & 2.46 $\pm$ 0.45 \\ \hline $P_{T}^{X}>25$~GeV & 4 & 1.48 $\pm$ 0.25 & 1.27 $\pm$ 0.24 & 0.22 $\pm$ 0.06 \\ \hline $P_{T}^{X}>40$~GeV & 3 & 0.54 $\pm$ 0.11 & 0.45 $\pm$ 0.11 & 0.09 $\pm$ 0.04 \\ \hline \hline {\bf Muon } & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 8 & 2.55 $\pm$ 0.44 & 2.23 $\pm$ 0.43 & 0.33 $\pm$ 0.08 \\ \hline $P_{T}^{X}<25$~GeV & 2 & 1.11 $\pm$ 0.19 & 0.94 $\pm$ 0.18 & 0.17 $\pm$ 0.05 \\ \hline $P_{T}^{X}>25$~GeV & 6 & 1.44 $\pm$ 0.25 & 1.29 $\pm$ 0.25 & 0.15 $\pm$ 0.04 \\ \hline $P_{T}^{X}>40$~GeV & 3 & 0.55 $\pm$ 0.12 & 0.51 $\pm$ 0.12 & 0.04 $\pm$ 0.01 \\ \hline \hline {\bf Electron and Muon }& H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 18 & 12.40 $\pm$ 1.69 & 9.40 $\pm$ 1.60 & 3.00 $\pm$ 0.53 \\ \hline $P_{T}^{X}<25$~GeV & 8 & 9.48 $\pm$ 1.21 & 6.85 $\pm$ 1.12 & 2.64 $\pm$ 0.48 \\ \hline $P_{T}^{X}>25$~GeV & 10 & 2.92 $\pm$ 0.49 & 2.55 $\pm$ 0.49 & 0.37 $\pm$ 0.09 \\ \hline $P_{T}^{X}>40$~GeV & 6 & 1.08 $\pm$ 0.22 & 0.96 $\pm$ 0.22 & 0.12 $\pm$ 0.04 \\ \hline \end{tabular} \end{center} \caption{Observed and predicted numbers of events in the electron and muon channels combined for all $e^+p$ data. Only the electron channel contributes for $P_{T}^{X}<12$ GeV.} \end{table} \begin{table}[htb] \renewcommand{\arraystretch}{1.1} \begin{center} \begin{tabular}{|r||c|c||c|c|} \hline {\bf Electron } & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 1 & 1.69 $\pm$ 0.22 & 1.00 $\pm$ 0.16 & 0.69 $\pm$ 0.15 \\ \hline $P_{T}^{X}<25$~GeV & 0 & 1.41 $\pm$ 0.18 & 0.82 $\pm$ 0.13 & 0.59 $\pm$ 0.12 \\ \hline $P_{T}^{X}>25$~GeV & 1 & 0.28 $\pm$ 0.04 & 0.18 $\pm$ 0.04 & 0.10 $\pm$ 0.03 \\ \hline $P_{T}^{X}>40$~GeV & 0 & 0.12 $\pm$ 0.02 & 0.07 $\pm$ 0.02 & 0.05 $\pm$ 0.01 \\ \hline \hline {\bf Muon } & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 0 & 0.37 $\pm$ 0.06 & 0.29 $\pm$ 0.06 & 0.08 $\pm$ 0.02 \\ \hline $P_{T}^{X}<25$~GeV & 0 & 0.13 $\pm$ 0.02 & 0.11 $\pm$ 0.02 & 0.02 $\pm$ 0.01 \\ \hline $P_{T}^{X}>25$~GeV & 0 & 0.24 $\pm$ 0.04 & 0.18 $\pm$ 0.04 & 0.06 $\pm$ 0.01 \\ \hline $P_{T}^{X}>40$~GeV & 0 & 0.09 $\pm$ 0.02 & 0.08 $\pm$ 0.02 & 0.02 $\pm$ 0.01 \\ \hline \hline {\bf Electron and Muon} & H1 Data & SM expectation & SM Signal & Other SM processes\\ \hline \hline Total & 1 & 2.06 $\pm$ 0.28 & 1.30 $\pm$ 0.23 & 0.76 $\pm$ 0.16 \\ \hline $P_{T}^{X}<25$~GeV & 0 & 1.54 $\pm$ 0.20 & 0.93 $\pm$ 0.16 & 0.61 $\pm$ 0.13 \\ \hline $P_{T}^{X}>25$~GeV & 1 & 0.52 $\pm$ 0.08 & 0.37 $\pm$ 0.07 & 0.15 $\pm$ 0.04 \\ \hline $P_{T}^{X}>40$~GeV & 0 & 0.21 $\pm$ 0.04 & 0.14 $\pm$ 0.03 & 0.07 $\pm$ 0.02 \\ \hline \end{tabular} \end{center} \caption{Observed and predicted numbers of events in the electron and muon channels combined for all $e^-p$ data. Only the electron channel contributes for $P_{T}^{X}<12$ GeV.} \end{table} \newpage \begin{table} \renewcommand{\arraystretch}{1.6} \begin{center} \begin{tabular}{|c|c|c|c|} \hline \multicolumn{2}{|c|}{ } & Electron & Muon \\ \multicolumn{2}{|c|}{1994-2000 $e^\pm p$} & obs./exp. & obs./exp. \\ \multicolumn{2}{|c|}{ } & {\footnotesize($W^\pm$ contribution)} & {\footnotesize ($W^\pm$ contribution) } \\ \hline & Full sample & 11 / $11.54~\pm1.50~(71\%)$ & 8 / $2.94~\pm0.50~(86\%)$ \\ \cline{2-4} {\large \bf H1} & $p_T^\mathrm{X}~>~25\gev$ & 5 / $1.76~\pm0.30~(82\%)$ & 6 / $1.68~\pm0.30~(88\%)$ \\ \cline{2-4} {\footnotesize $118.4$~pb$^{-1}$}& $p_T^\mathrm{X}~>~40\gev$ & 3 / $0.66~\pm0.13~(80\%)$ & 3 / $0.64~\pm0.14~(92\%)$ \\ \hline \hline \end{tabular} \end{center} \caption{Summary of the H1 results of searches for events with isolated leptons, missing transverse momentum and large $p_T^\mathrm{had}$ at HERA. The number of observed events is compared to the SM prediction. The $W^\pm$ component is given in parentheses in percent. The statistical and systematic uncertainties added in quadrature are also indicated.} \label{tab:heraisolep} \end{table} \end{document}