Table 3: 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 $c_3 (s)= {\Gamma (1-s/2) \over \pi \Gamma (2+s/2)}$ .
$1 \over 2$ Anisotropy parameter $\Lambda$ $h^{\rm T}(\Lambda, \epsilon, s)$

$1 \over 2$ $\Lambda \ll \epsilon ^2 \ll 1$ $\xi (s) \Lambda^{s+1 \over 2} \epsilon^{-(s+2)}$

$1 \over 2$ ${\epsilon ^2 \ll \Lambda \ll 1}$ $c_3 (s) \Lambda^{-1/2} \left[ \ln \epsilon ^{-1} + \ln \Lambda ^{1/2} \right]$

$1 \over 2$ ${\Lambda = 1}$ $c_1 (s) \ln \epsilon^{-1}$

$1 \over 2$ $\Lambda \gg 1$ $c_1 (s) s \Lambda^{-s/2} \ln \epsilon ^{-1}$

**Table 3:** 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 $c_3 (s)= {\Gamma (1-s/2) \over \pi \Gamma (2+s/2)}$ .
$1 \over 2$ Anisotropy parameter $\Lambda$	$h^{\rm T}(\Lambda, \epsilon, s)$
$1 \over 2$ $\Lambda \ll \epsilon ^2 \ll 1$	$\xi (s) \Lambda^{s+1 \over 2} \epsilon^{-(s+2)}$
$1 \over 2$ ${\epsilon ^2 \ll \Lambda \ll 1}$	$c_3 (s) \Lambda^{-1/2} \left[ \ln \epsilon ^{-1} + \ln \Lambda ^{1/2} \right]$
$1 \over 2$ ${\Lambda = 1}$	$c_1 (s) \ln \epsilon^{-1}$
$1 \over 2$ $\Lambda \gg 1$	$c_1 (s) s \Lambda^{-s/2} \ln \epsilon ^{-1}$

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