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%  \usepackage[CP866]{inputenc}
%  \usepackage[russiane]{babel}
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\begin{document}



\begin{flushright}
“„Š 539.12: 539.171 \end{flushright}
\vskip 15mm

\begin{center}
{\Large \bf Title of article in Russian}
\end{center}
\vspace*{.5cm}

\begin{center}
A. B. Author1$^{1}$, \underline{C.D. Author2}$^{1,2}$ and
V.A. Author3$^{1,3}$ %(in Russian)
\vskip 5mm

{\small
(1) {\it Institute1, address1 (in Russian)}
\\
(2) {\it Institute2, address2 (in Russian)}
\\
(3) {\it Institute3, address3 (in Russian)}
}
\end{center}
\vspace*{.5cm}

\centerline{\small \bf €­­®â æ¨ï}
\vskip 4mm
\hspace*{1cm}
\begin{minipage}{14cm}
{\small \hspace*{5mm}
This is where the abstract in Russian language should be placed.
}
\end{minipage}



\begin{center}
\section*{Title of article in English}


\vskip 5mm
A. B. Author1$^{1}$, \underline{C.D. Author2}$^{1,2}$ and
V.A. Author3$^{1,3}$
\vskip 5mm

{\small
(1) {\it Institute1, address1}
\\
(2) {\it Institute2, address2}
\\
(3) {\it Institute3, address3}

}
\end{center}
\vskip 5mm

\begin{abstract}
This is where the abstract should be placed. It should consist
of one paragraph giving a concise summary of the material in
the article below.  Replace the title, authors, and addresses
within the curly brackets with your own title, authors, and
addresses. You may have as many authors and addresses as you
like. It is preferable not to use footnotes in the abstract or
the title; the acknowledgments for funding bodies etc. are to
be placed in a separate section at the end of the text.
\end{abstract}
\vskip 8mm


\subsection*{1. Guidelines}

You can delete our sample text and replace it with your own
contribution to the volume, however we recommend that you keep an
initial version of the file for reference. These file will work
with standard latex2e. A guide to authors
also can be found on the web site:
http://thsun1.jinr.ru/\~ \,bog2004/proceedings.html
The deadline for submission of the talk is December 1, 2004.
The sizes of the contributions are:\\
\hspace*{2cm}plenary talk -- 10 pages,\\
\hspace*{2cm}orginal talk -- 6 pages.\\
The e-mail address for sending of the manuscripts is:
bog2004@thsun1.jinr.ru

\subsection*{2. Headings, Text, Equations and Figures/Illustrations/Images}
Please preserve the style of the headings, text font and line
spacing in order to provide a uniform style for the
proceedings volume.

Equations should be centered and numbered consecutively, as in
Eq.~(\ref{eq:murn}), and the {\em eqnarray} environment may be
used to split equations into several lines, for example in
Eq.~(\ref{eq:sp}), or to align several equations.

In latex, it is simplest to give the equation a label, as in
Eq.~(\ref{eq:murn}) where we have used
{\em $\backslash$label\{eq:murn\}} to identify the equation.
You can then use the reference {\em $\backslash$ref\{eq:murn\}}
when citing the equation in the text which will avoid
the need to manually renumber equations due to later changes.

The same method can be used for referring to subsections and subsubsections.

Authors are advised to prepare their figures in eps format.
Please prepare the figures in high resolution (300 dpi) for half-tone
illustrations or images. Half-tone pictures must be sharp enough
for reproduction. To insert figure you can use\\
\centerline{$\backslash$includegraphics[width=8cm,]{Fig1.eps}}

\subsection*{3. Sample Mathematical Text}
The following may be (and has been) described as `dangerously
irrelevant' physics. The Lorentz-invariant phase space integral for a
general n-body decay from a particle with momentum $P$ and mass $M$
is given by:
\noindent
\begin{equation}
I((P - k_i)^2, m^2_i, M) = \frac{1}{(2 \pi)^5}
\int \frac{d^3 k_i}{2 \omega_i} \delta^4(P - k_i)\,.
\label{eq:murn}
\end{equation}
There are two
necessary conditions required for any acceptable parametrization of
the quark mixing matrix. The first is that the matrix must be unitary,
and the second is that it should contain a CP violating phase
$\delta$. The connection between invariants
(of form similar to J) and unitarity relations will be examined
further for the more general $ n \times n $ case. The reason is that
such a matrix is not a faithful representation of the group, i.e.~it
does not cover all of the parameter space available
\begin{eqnarray}
T &=& {\rm Im}[V_{11} {V_{12}}^* {V_{21}}^* V_{22}]\nonumber \\[4pt]
&&{}+ {\rm Im}[V_{12} {V_{13}}^* {V_{22}}^* V_{23}]\nonumber \\[4pt]
&&{}- {\rm Im}[V_{33} {V_{31}}^* {V_{13}}^* V_{11}]\, ,
\label{eq:sp}
\end{eqnarray}
where $k=j$ or $j+1$ and $\beta = \alpha$ or $\alpha+1$, but if
$k=j+1$, then $\beta \neq \alpha + 1$ and similarly, if $\beta =
\alpha + 1$ then $ k \neq j + 1$.\footnote{An example of a matrix
which has elements containing the phase variable $e^{i \delta}$ to
second order, i.e.~elements with a phase variable $e^{2i \delta}$ is
given at the end of this section.}


\begin{thebibliography}{99}
\itemsep=-2pt
\bibitem{Ge66}
S.B.~Gerasimov, ZhETF {\bf 50}, 1559 (1966).

\bibitem{DvH}
R.H.~Dalitz and F.~von Hippel,
Phys. Lett. {\bf 10}, 153 (1964).

\bibitem{CSW03}
N.~Cabibbo, E.C.~Swallow and R.~Winston, arXiv: hep-ph/0307298

\end{thebibliography}
\end{document}