Table 6: Anisotropy function $g^{\rm F}$ for fast magnetosonic turbulence.
$1 \over 2$ Anisotropy parameter $\Lambda$ $g^{\rm F}(\Lambda, \epsilon, s)$ $g^{\rm F}(\Lambda, \epsilon, s=5/3)$

$1 \over 2$ ${\epsilon ^2 \ll \Lambda \ll 1}$ ${\pi \over \zeta (s+1)} \epsilon^{1-s}$ $2.446 \epsilon^{1-s}$

$1 \over 2$ ${\Lambda = 1}$ ${4 \over 3 \zeta (s+1)} \epsilon^{1-s}$ $1.038 \epsilon^{1-s}$

$1 \over 2$ ${ \epsilon ^{-2} \gg \Lambda \gg 1}$ ${1 \over s c_2} \epsilon^{1-s} \Lambda^{-1/2}$ $0.872 \epsilon^{1-s} \Lambda^{-1/2}$

$1 \over 2$ ${\Lambda \gg \epsilon ^{-2} \gg 1}$ ${2 \over (2-s)(4-s)}$ 2.57

**Table 6:** Anisotropy function $g^{\rm F}$ for fast magnetosonic turbulence.
$1 \over 2$ Anisotropy parameter $\Lambda$	$g^{\rm F}(\Lambda, \epsilon, s)$	$g^{\rm F}(\Lambda, \epsilon, s=5/3)$
$1 \over 2$ ${\epsilon ^2 \ll \Lambda \ll 1}$	${\pi \over \zeta (s+1)} \epsilon^{1-s}$	$2.446 \epsilon^{1-s}$
$1 \over 2$ ${\Lambda = 1}$	${4 \over 3 \zeta (s+1)} \epsilon^{1-s}$	$1.038 \epsilon^{1-s}$
$1 \over 2$ ${ \epsilon ^{-2} \gg \Lambda \gg 1}$	${1 \over s c_2} \epsilon^{1-s} \Lambda^{-1/2}$	$0.872 \epsilon^{1-s} \Lambda^{-1/2}$
$1 \over 2$ ${\Lambda \gg \epsilon ^{-2} \gg 1}$	${2 \over (2-s)(4-s)}$	2.57

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