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\begin{document}  
% The rest
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%\newcommand{\gevsq}{\mathrm{GeV}^2}
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\newcommand{\n}{1.19\pm 0.06 (stat.) \pm0.07 (syst.)}
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%
% Some useful tex commands
%
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% Journal macro
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\def\NCA{\em Nuovo Cimento}
\def\NIM{\em Nucl. Instrum. Methods}
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\def\NPB{{\em Nucl. Phys.}   {\bf B}}
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\begin{titlepage}

\noindent
Submitted to the International Europhysics Conference on High Energy Physics
HEP99, \\
Tampere, Finland, July 1999

\vspace{2cm}

\begin{center}
\begin{Large}

{\bf your wonderful title ... at HERA}

\vspace{2cm}

H1 Collaboration

\end{Large}
\end{center}

\vspace{2cm}

\begin{abstract}
...your striking abstract
\end{abstract}

\vspace{1.5cm}

\begin{flushleft}
{\bf Abstract: } \\
{\bf Parallel sessions: } \\
{\bf Plenary sessions:  } \\ 
\vspace*{0.2cm}
{\bf Electronic Access: http://www-h1.desy.de/publications/ }
\end{flushleft}

\end{titlepage}


\newpage

\section{Introduction}

\noindent
...your clearly written text with figures 
(such as Fig.\ref{fig:diff}, from \cite{diff})
and important relations
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{equation}
x_\pom = \frac{\qsq+M_X^2-t}{\qsq+W^2+M_p^2} \; .
\label{eq:xpom}
\end{equation}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
Equation (\ref{eq:xpom}) gives ...

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[hhh]
\center
\epsfig{file=/h1/psfiles/figures/d98-029f6.eps,width=10.0cm}
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%\begin{picture}(15.0,10.0)
%\put(0.,0.0)
%{\epsfig{file=/h1/psfiles/figures/d98-029f6.eps,width=10.0cm}}
%\end{picture}
\caption{The average squared transverse momentum 
$\langle p_t^{*2} \rangle$ of hadrons is shown as 
a function of Feynman $x_F$.}
\label{fig:diff} 
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\section*{Acknowledgements}


\begin{thebibliography}{99}
\bibitem{diff} 
H1 Collab., C. Adloff et al., \Journal{\PLB}{428}{1998}{206}
\end{thebibliography}

\end{document}