\documentclass[12pt,landscape]{article}

\usepackage{portland}

\begin{document}


\landscape



\setlength{\textwidth}{16.5cm}
\setlength{\textheight}{22.5cm}
%\setlength{\oddsidemargin}{3.cm}
\setlength{\oddsidemargin}{1.cm}
%\setlength{\headheight}{0.5cm}
\setlength{\headsep}{1.0cm}
\setlength{\topmargin}{0.0cm}
\setlength{\topskip}{0.1cm}
%\setlength{\footheight}{0.5cm}
\renewcommand{\baselinestretch}{1.1}
%\setlength{\changebarsep}{0mm}
%%%\setlength{\mathindent}{0mm}
%\setlength{\overfullrule}{5pt}

\setlength{\footskip}{1.5cm}
\frenchspacing
\newcommand{\ep}{\epsilon}
\newcommand{\la}{\lambda}
\newcommand{\La}{\Lambda}
\newcommand{\prd}{\partial}

\large

In the file  \verb+sqmass_data.m+   three functions 
are defined:

\noindent
\verb+ db[i,j],  bb[i,j]+  and  \verb+ rw[i,j]+.
\\
The relations between these functions and  eqs. (8-11), (17-22) and (25-28) of the work \cite{Chetyrkin:2005kn}
are:
\[
\verb+ db[i,j]+ = \bar{d}_{i,j},
\ \ 
\verb+ bb[i,j]+ = \bar{b}_{i,j},
\verb+ rw[i,j]+ = \tilde{r}_{i,j}.
\]

\vspace{6mm}

\noindent
Notations are  as follows. 
\vspace{6mm}

\begin{table}[here]
\begin{tabular}{|c|c|c|c|c|c|c|c|c|c|}
\hline
\texttt{LQM} & \texttt{LMM} & \texttt{LSM} & \texttt{GE} &  \texttt{Pi}  &  \texttt{z3} & \texttt{z4}  & \texttt{z5}
&  \texttt{z6} & \texttt{z7} 
\\ \hline\hline
$\log\frac{Q^2}{\mu^2}$ & $\log\frac{M^2}{\mu^2}$  & $\log\frac{s}{\mu^2}$  & $\gamma_E$ &  $\pi$ &
$\zeta_3$ & $\zeta_4$  & $\zeta_5$   & $\zeta_6$ & $\zeta_7$
\\
\hline
\end{tabular}
\vspace{6mm}

\end{table}




\begin{thebibliography}{100}





%\cite{Chetyrkin:2005kn}
\bibitem{Chetyrkin:2005kn}
K.~G.~Chetyrkin and A.~Khodjamirian,
``Strange Quark Mass from Pseudoscalar Sum Rule with ${\cal O}(\alpha_s^4)$ Accuracy,''
arXiv:hep-ph/0512295.
%%CITATION = HEP-PH 0512295;%%


\end{thebibliography}
\end{document}

