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\documentclass{article}  
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%     Proceedings of the 24th Winter Workshop on Nuclear Dynamics        %|
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%              South Padre, Texas, April 5--12, 2008                     %|
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% Communicating author:                                                  %|
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\def\rightmark{(Short) Title of the Article}
\def\leftmark{A. One et al.}
 
\title{Title of the Article (Sometimes Extending over Two or\\ 
More Lines)} 
\authors{
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{Author One$^1$ and Author Two$^{2,a}$ %
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{\normalsize
\hspace*{-8pt}$^1$ Institute of Author One, \\ 
123456 City, Country\\[0.2ex] 
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\hspace*{-8pt}$^2$ Institute of Author Two, (if not the same)\\ 
456789 City, Country
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\abstract{This is a template article, to be used along with the style
  {\tt spadre2008.sty}, prepared for manuscripts to the Proceedings
  of the {\it 24th \mbox{Winter} Workshop on Nuclear Dynamics}, South Padre,
  Texas, April 5--12, 2008. {Articles} so prepared are suitable
  for submissions to e.g.\ the LANL preprint server as well.}

\keyword{list of keywords, relevant to the article} 
\PACS{specifications see, e.g.\ {\tt http://www.aip.org/pacs/}}
 
\begin{document}
 
\maketitle
\setcounter{page}{1}

\section{Introduction}\label{intro}

A historical, methodological or logical scope outlined in the
Introduction helps the readers place the subject of the article or it
enables to guess the present stage of the subject. Ample citation
\cite{bib1,bib2,bib3,bib4,bib5,bib6,bib7,bib8,bib9} of literature 
that deals with the subject in question is also given in this section, 
as a source of information.  In a second part, the Introduction tells 
the readers more details about the structure of the article. It often 
serves as a guide to introduce the sections that build up the article.
 
At the beginning of the \LaTeX\ template file {\tt
  spadre2008-template.tex}, there is a header in which certain {\it
  data are asked to submit for communication purposes}.

 
\section{Technical--Preparatory Section}\label{techno}  

The technical or methodological preparatory section of the article
should commence the row of the sections. The experimental description
of measurements or the mathematical introduction of the problem, the
definitions of the concepts or the descriptions of the methods,
procedures applied in the investigations should be treated in this
section to start with the problem \cite{bib1,bib6,bib7,bib8,bib9}.
 
{\it Citation of references} mentioned in the article will be done as
seen in the previous sentence. Citations referring to some journals
should be given, for example, as in Ref.~\cite{bib4}, using the
`protocol' shown in the References.
 
 
\subsection{Subsections dealing with details}\label{details}

Subsections (maybe, the deeper {\tt $\backslash$subsubsection}s) will be
arranged so that they appear as discernible distinct parts within the
whole structure of the article. For too wide tables or figures it may
happen that a ``landscape page'' will be setup.
 
\subsection{Mathematics}\label{maths}
 
Mathematics can be e.g.\ embedded $P_1({\bf p})=E_p(dN/d^3p)$ as in
this case, or displayed separately from text rows as (the boldface
letter {\bf p} denotes a vector):
\begin{equation}
   n_\mu(x)=
\int_\Sigma d^3\sigma_\mu(x^\prime)\,\delta^{(4)}(x-x^\prime) \,. 
\label{eq1}
\end{equation} 
 
Not strange if formulae are arranged in an (vertical or horizontal)
array of terms/factors or equations or in matrices, e.g.\ if a single
row is too short to accommodate a formula:
\begin{eqnarray}
   \tilde{C}({\rm\bf q},{\rm\bf K}) = 1 \pm \Bigl\{1
   &-&
   q_s^2\langle y^2\rangle
   -\left\langle[q_\perp(x-\beta_\perp t) +
   q_L(z-\beta_L t)]^2\right\rangle
 \nonumber \\
   &+&
   \langle q_\perp(x-\beta_\perp t) +
   q_L(z-\beta_L t)\rangle^2
+ {\cal O}\left[\left\langle(q{\cdot}x)^4\right\rangle\right] \Bigr\} \,.
\label{eq2} 
\end{eqnarray}
{\it Cross references to formulae} will be given as ``as in
Eq.~(\ref{eq2})'' or ``given by (\ref{eq1})'', etc.
 
\subsection{Tables}\label{tabs}
 
An example of a simply built table we give below. 
\begin{table}[hb] 
\vspace*{-12pt}
\caption[]{Title of the table (usually, the first sentence). 
An explanatory on the data text may follow; it ranges in the full 
width of the table, similarly as for figures.}\label{tab1}
\vspace*{-14pt}
\begin{center}
\begin{tabular}{lllll}
\hline\\[-10pt]
Projectile & Energy & $\bar{E}$ & $\sigma_{KLL}^{\rm rel}$ &
$\sigma_{KLM}/\sigma_{KLL}$\\ 
&(MeV) & (eV) & (\%) & (\%)\\
\hline\\[-10pt]
Ne$^{3+}$ & 110 & 756.6 $\pm$ 0.3 & {\phantom{$0$}}71.6 $\pm$ 3.8 & 
{\phantom{$00$}}8.1 $\pm$ 1.2 \\
Ne$^{10+}$ & 110 & 742.8 $\pm$ 0.2 & 100 & {\phantom{$0$}}10.3 $\pm$ 4.5 \\ 
Ar$^{6+}$ & 220 & 743.7 $\pm$ 0.3 & 153.5 $\pm$ 10.7 & $<9.2$ \\ 
Ar$^{17+}$ & 220 & 719.8 $\pm$ 0.4 & 269.2 $\pm$ 21.3 & 
{\phantom{$00$}}9.84 $\pm$ 0.35\\
\hline 
\end{tabular}
\end{center}
\end{table}
 
\newpage
 
\subsection{Figures}\label{figs}
 
Figure \ref{fig1} shows a typical presentation of data or results. The
figure caption is an inevitable part of the figure (see Fig.\ \ref{fig1}).
 
\begin{figure}[htb]
\vspace*{-.8cm}
                 \insertplot{fig1.ps}
\vspace*{-2cm}
\caption[]{The figure caption contains an explanatory text for the 
  figure, the meaning of the applied signs, references, explicit data
  for parameters}
\label{fig1}
\end{figure} 

{\it Plots} are expected to be submitted in Encapsulated PostScript.
The {\tt epsf.sty} style file is used in {\tt spadre2008.sty} to help
you place and size your figures into the ma\-nu\-script. Please submit
each figure as a fig-n\-.eps(f) file separately. If the file is
exceptionally large or in other exceptional cases the {\it compression
  of files\/} is desirable, however, in this case include instructions
for decompressing on a unix computer. {\it Figures will be printed
  generally in \framebox{\selectfont\itshape{\bfseries black-{\rm
        \&}-white}} in the journals}, so please use {\it
  distinguishable colors, marks and line styles\/} in your
figures. {\it Photos} should be converted to EPS files; for color
separation purposes, please keep the TIF (or good quality JPG) file
format if they are colorful photos.
 
\section{Other Sections}\label{others}
Further sections explaining the subject of the article follow the
starting ones. At the end, Special Sections may follow as below.

\section{Conclusions}\label{concl}
As usual, the Conclusions contain the results achieved and presented
in the article.
 
\section*{Appendix}\label{app}
Details of mathematical derivations, other technical descriptions are
deferred here from the main text. If more than a single appendix will
be included, they will be enumerated by using capital Latin letters:
Appendix A, Appendix B, etc.

 
\section*{Acknowledgments}
A section devoted for personal gratitude and/or offered grant
identifications.
 
\section*{Note(s)} (footnotes will be typeset in this way) 
\begin{notes}
\item[a]
Permanent address: Institute, City, Country;\\ 
E-mail: author@host.domain.name
\end{notes}
 
 
\begin{thebibliography}{9}  
  
\bibitem{bib1}A.B. Coalman, D.E. Fiedler and G. Hughes, {\it Rev. Mod.
    Phys.}  {\bf 63} (1991) 545.
 
\bibitem{bib2}G.J. Banderer and S.M. Mikhalchuk, {\it Phys. Lett.}
  {\bf B54} (1983) 387; {\it Sov. J. Nucl. Phys.} {\bf 19} (1979) 197.
 
\bibitem{bib3}D. Heinemann and U. S\o renmann, Bergensburg preprint
  BPR-94-31, submitted to {\it Phys. Lett. B.} [hep-ph/0123456].
  
\bibitem{bib4}T. Czukor and J. Zel\'enyi, {\it Acta Phys. Hung. A} {\bf
    24} (2005) 345.
 
\bibitem{bib5}I.V. Mileev, K. Plummer and M.M. Gorentchev, {\it Int.
    J. Mod.  Phys.} {\bf A11} (1995) 77.
 
\bibitem{bib6}S. Trottman and G. Karib, {\it Proceedings of the 5th
    Workshop on High Energy Collision Phenomena}, eds. J.-P. Condrieu
  and P.  Ch\^{a}teau-Simone, Paris, August 2--6, 1993, Springer,
  Heidelberg, 1994, p.  324.
 
\bibitem{bib7}W.T. Fogg, Talk presented at {\it Advanced Research
    Workshop on Hot Hadronic Matter: Theory and Experiment},
  Barcelona, June 29 -- July 1, 1994; to be published in the
  Proceedings by Plenum Press.
 
\bibitem{bib8}This was not seen in \cite{bib6}.
 
\bibitem{bib9}From Eq.~(\ref{eq2}) one sees that in the original frame
  the cross term is given by:
$$
Q_{\perp L}^2 =  \left( <x\;\tau\;{\rm sh}\eta'>-
<x><\tau\;{\rm sh}\eta'>\right) 
$$
up to small logarithmic corrections. This clearly vanishes as soon
as the source becomes reflection symmetric under $\eta' = - \eta'$.

\end{thebibliography}
\vfill\eject
\end{document}
