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\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  
      $12<P_{T}^{X}<25$~GeV & 1 & 1.96 $\pm$ 0.27  & 1.45 $\pm$ 0.24  & 0.51 $\pm$ 0.12  \\
      \hline
      $25<P_{T}^{X}<40$~GeV & 1 & 0.95 $\pm$ 0.14  & 0.82 $\pm$ 0.13  & 0.13 $\pm$ 0.04  \\
      \hline
      $P_{T}^{X}>40$~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  
      $12<P_{T}^{X}<25$~GeV & 2 & 1.11 $\pm$ 0.19  & 0.94 $\pm$ 0.18  & 0.17 $\pm$ 0.05  \\
      \hline
      $25<P_{T}^{X}<40$~GeV & 3 & 0.89 $\pm$ 0.14  & 0.77 $\pm$ 0.14  & 0.12 $\pm$ 0.03  \\
      \hline
      $P_{T}^{X}>40$~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  
      $12<P_{T}^{X}<25$~GeV & 3  & 3.08 $\pm$ 0.43  & 2.40 $\pm$ 0.40  & 0.68 $\pm$ 0.14  \\
      \hline
      $25<P_{T}^{X}<40$~GeV & 4  & 1.83 $\pm$ 0.27  & 1.59 $\pm$ 0.26  & 0.24 $\pm$ 0.06  \\
      \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}
\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}