%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\documentclass[11pt,twoside]{article}
\usepackage{epsfig}
\usepackage{here}
\usepackage{amsmath}
 
\begin{document}
 

\begin{center}{\bf\Large  Title of my talk is for example 
  study of the $\boldsymbol{\eta}^{\boldsymbol{\prime}}$ meson in the reaction 
  $\mbox{p}\mbox{n} \boldsymbol{\rightarrow} 
  \mbox{p}\mbox{n}\boldsymbol{\eta}^{\boldsymbol{\prime}}$}
\end{center}
\vspace{0.5cm}
\begin{center}
   A. Name$^{a,b}$ \\[0.1cm]
   {\small \em 
         $^a$Institute of Physics, Jagellonian University, Krak\'ow, Poland \\
         $^b$Institut f\"ur Kernphysik, Forschungszentrum J\"ulich, Germany
   }
\end{center}
\vspace{0.5cm}
\begin{center}
 \parbox{0.9\textwidth}{
  \small{
    {\bf Abstract:}\
     This is example of the abstract:
     The feasibility of an investigation of the $pn \rightarrow 
     p n \eta^{\prime}$ reaction by means of the COSY-11 internal target 
     facility is discussed. Appraisals are based on the assumption of the 
     quasi-free reactions of beam protons, circulating in the cooler 
     synchrotron COSY, with neutrons from a windowless deuteron cluster 
     target.}
 }
\end{center}

\vspace{0.5cm}
\section{Introduction}

In 1984 Maltman and Isgur~\cite{maltmanisgur} have argued on the basis of 
simple geometrical considerations (see figure~\ref{cartoon}) that at the 
distances smaller than $2\,\mbox{fm}$ the internucleon potential should begin 
to be free of meson exchange effects and may be dominated by the residual 
colour forces. 

\begin{figure}[H]
\parbox{0.4\textwidth}
   {\epsfig{file=figure1.eps,width=0.4\textwidth}}
\hfill
\parbox{0.5\textwidth}
  {\caption{\label{cartoon} \small A cartoon illustrating in naive geometrical 
   terms that for $r < 2r_{N} + 2r_{M}$ meson exchange is unlikely to be 
   appropriate to the description of the internucleon potential. Figure and 
   caption are taken from reference~\cite{maltmanisgur}.}}
\end{figure}

\section{Next section ...Experiment}

 The detection setup consists of .....

\begin{figure}[H]
\epsfig{file=figure2.eps,width=0.5\textwidth}
    \caption{\label{detectionsystem} \small Schematic view of the COSY-11 
      detection setup\cite{brau96}. Only detectors needed for the measurements 
      of the reaction $pd \rightarrow p_{sp} pn \eta (\eta^\prime)$ are 
      shown.\newline
      D1, D2 denote the drift chambers; S1, S2, S3, S4 and V1 the 
      scintillation detectors; N1 the neutron detector and $\mbox{Si}_{\,mon}$ 
      and $\mbox{Si}_{\,spec}$ silicon strip detectors to detect elastically 
      scattered and spectator protons, respectively.}
\end{figure}

\section{Next section ... Formulae}
Equations~\ref{eq1} and~\ref{eq2} are given here as an example:
\begin{equation}
\frac{dN}{dm}(m,\mbox{Q}) =
  \frac{d\sigma}{dm}(m,\mbox{Q}) \cdot L \cdot Eff(\mbox{Q}),
  \label{eq1}
\end{equation}

\begin{equation}
 \sigma(\mbox{Q})=\!\displaystyle\int_{2m_{p}}^{\infty}
 \frac{d\sigma}{dm}(m\!=\!\sqrt{s}-2\,m_{p}-\mbox{Q},\mbox{Q}) \;d\sqrt{s}
 \label{eq2}
\end{equation}




\begin{thebibliography}{9}
\bibitem{maltmanisgur} K. Maltman, N. Isgur, Phys.\ Rev.~{\bf D~29} (1984) 952.
\bibitem{brau96} S. Brauksiepe et al., Nucl.\ Instr.~\&~Meth.~{\bf A~376}
                 (1996) 397.
\end{thebibliography}
\end{document}
