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{\bfseries TITLE OF THE ARTICLE (IN CAPITAL LETTERS)}

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A.A. Author$^{1 \dag}$, \underline{B.B. Author-Speaker}$^{2}$ and
C.C. Author$^{2}$

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{\small
(1) {\it
First Organization
}\\
(2) {\it
Second Organization
}\\
$\dag$ {\it
E-mail: author@somewhere.org
}}
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\vskip 5mm
\begin{abstract}
Text of the abstract.
\end{abstract}

\vskip 8mm Text of report................... 
For figures we recommend to use wrapfigure. Pay attention to the 
name of eps file!
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\begin{wrapfigure}[21]{R}{5cm}
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\mbox{\epsfig{figure=yourname_fig1.eps,width=5cm,height=5cm}}
\end{center}
{\small{\bf Figure 1.} Figure caption aaaaaaa aaa aaa aaa aaa}
\label{yourname_fig1}
\end{wrapfigure}


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To insert figure (with the help of wrapfig.sty)

In the HERMES and COMPASS experiments the cross sections
$\sigma_N^{\uparrow\downarrow}$ for the process
$lN^{\uparrow\downarrow}\rightarrow l'h X$ will be measured, where
$N^{\uparrow\downarrow}$ denotes the transversely with respect to
the beam polarized target, see Fig.~1.

With $P$, $l$ and $l'$ denoting the momenta of the target, incoming and
outgoing lepton the kinematic variables are defined as $s:=(P+l)^2$,
$q:= l-l'$ with $Q^2:= - q^2$,  and $W^2:= (P+q)^2$, and
\begin{equation}\label{notation-1}
        x := \frac{Q^2}{2Pq}    \;,\;\;\;
        y := \frac{Pq}{Pl}      \;,\;\;\;
        z := \frac{PP_h}{Pq\;}  \;.
\end{equation}
Let $S^{\uparrow\downarrow}$ denote the modulus of the polarization
vector.
To insert figures in one row (with the help of epsfig.sty)
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\mbox{\epsfig{figure=yourname_fig2a.eps,width=4cm,height=2cm}}&
\mbox{\epsfig{figure=yourname_fig2b.eps,width=4cm,height=2cm}}&
\mbox{\epsfig{figure=yourname_fig2c.eps,width=4cm,height=2cm}}\\
{\bf(a)}& {\bf(b)}& {\bf(c)}
\end{tabular}
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{\small{\bf Figure 2a.} Figure caption aaaaaaa aaa aaa aaa aaa
aaaaaa aaaaaaaaaaa aaa bbbbbbbbbbbbbbbbbbbb.}\\
{\small{\bf Figure 2b.} Figure caption aaaaaaa aaa aaa aaa aaa
aaaaaa aaaaaaaaaaa aaa bbbbbbbbbbbbbbbbbbbb.}\\
{\small{\bf Figure 2c.} Figure caption aaaaaaa aaa aaa aaa aaa
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The component of the target polarization vector which is
transverse with respect to the hard photon is characterized
by the angle $\Theta_S$, see Fig.~2a.

\begin{thebibliography}{99}
\bibitem{bib1}
A.A.~Author, Phys. Rep. {\bfseries 01}, 1 (1901).
\bibitem{bib2}
A.A.~Author, Nucl. Phys. {\bfseries A01}, 1 (1901).
\bibitem{rad-j} A.V. Radyushkin, Phys.Rev, D {\bf 56}, 5524 (1997);\\
%\phantom{7}
X. Ji, Phys.Rev. D {\bf 55} (1997) 7114.
\bibitem{rysk}
 M.G.Ryskin, Z.Phys C {\bf 57}, 89 (1993).
\bibitem{kroll-da}
M. Diehl, T. Feldmann, R. Jakob, P. Kroll, Eur.Phys.J.
C {\bf 8}, 409  (1999).
\bibitem{krish-f}
D. C. Peaslee et al, Phys. Rev. Lett. {\bf 51}, 2358 (1983).
\bibitem{gol_j} S.V. Goloskokov, Proc. of the
14th International Spin Physics Symposium, SPIN2000,
AIP Conference  Proc. {\bf V.570}, 541

\end{thebibliography}
\end{document}