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\section{First Section}

\subsection{First subsection is related with $\hbar$}
Hello world..

Turkish letters:
\begin{verbatim}
\c{c} \c{C} \u{g} \u{G} {\i} \.{I} \"{o} \"{O} \c{s} \c{S} \"{u} \"{U}
\end{verbatim}
\c{c} \c{C} \u{g} \u{G} {\i} \.{I} \"{o} \"{O} \c{s} \c{S} \"{u} \"{U}


This is an {\bf in-line equation}: ($a_1 = a^2$)

And this is a {\large numbered} equation~\cite{Cemal}:

\begin{equation}
 A(x) = \sum_{i=1}^N \int_0^{\infty} x^{i+1} dx
\label{my_integral}
\end{equation}

This is an unnubered {\Huge equation} (completely unrelated
to Eqn.\ref{my_integral}but see reference \cite{hwang}):

\[
\Psi(x) = \sum_{i=1}^N \int_0^{\infty} x^{i+2} dx
\]
 
tiny small large Large huge Huge

\begin{thebibliography}{9}
\bibitem{hwang} K.~Hwang, B.~Schmittmann, and R.K.P.~Zia, Phys.~Rev.~E, {\bf 48}, 800 (1993).
\bibitem{Cemal} K. Hwang, B. Schmittmann, and R.K.P. Zia, Phys. Rev. E, {\bf 48}, 800 (1993).
\end{thebibliography}

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