\begin{table}%t3
%\centering
\par
\caption{Anisotropy function $h^{\rm T}$ for fast magnetosonic waves. In 
this table we introduced the functions
$\xi (s) = {c_1 (s) \Gamma (1+s/2) \over \sqrt{\pi} \Gamma ((s+1)/2)} 
B({s+4 \over 2},{s+2 \over 2})$ with 
the generalized $\beta$-function $B(x,y)$ and $c_3 (s)= {\Gamma (1-s/2) 
\over \pi \Gamma (2+s/2)}$.}\label{t3}
\begin{tabular}{l|l}\hline\hline
\vphantom{$1 \over 2$} \ Anisotropy parameter $\Lambda 	$ & $ 
h^{\rm T}(\Lambda, \epsilon, s)									$ \\
\hline
\vphantom{$1 \over 2$} $ \Lambda \ll \epsilon ^2 \ll 1 	$ & $ \xi (s) 
\Lambda^{s+1 \over 2} \epsilon^{-(s+2)}						$ \\
\vphantom{$1 \over 2$} $ \epsilon ^2 \ll \Lambda \ll 1 	$ & $ c_3 (s) 
\Lambda^{-1/2} \left[ \ln \epsilon ^{-1} + \ln \Lambda ^{1/2} \right]	$ 
\\
\vphantom{$1 \over 2$} $ \Lambda = 1 				$ & $ c_1 (s) \ln 
\epsilon^{-1} 									$ \\
\vphantom{$1 \over 2$} $ \Lambda \gg 1 				$ & $ c_1 (s) s 
\Lambda^{-s/2} \ln \epsilon ^{-1} 						$ \\
\hline
\end{tabular}
\end{table}