Table 5: Anisotropy function $h^{\rm F}$ for fast magnetosonic waves.
$1 \over 2$ Anisotropy parameter $\Lambda$ $h^{\rm F}(\Lambda, \epsilon, s)$

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

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

$1 \over 2$ $\Lambda \gg 1$ ${1 \over s} - {1 \over s+2}$

**Table 5:** Anisotropy function $h^{\rm F}$ for fast magnetosonic waves.
$1 \over 2$ Anisotropy parameter $\Lambda$	$h^{\rm F}(\Lambda, \epsilon, s)$
$1 \over 2$ ${\epsilon ^2 \ll \Lambda \ll 1}$	$c_3 (s) \Lambda^{-1/2} \left[ \ln \epsilon ^{-1} + \ln \Lambda ^{1/2} \right]$
$1 \over 2$ ${\Lambda = 1}$	$c_1 (s) \ln \epsilon^{-1}$
$1 \over 2$ $\Lambda \gg 1$	${1 \over s} - {1 \over s+2}$

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