Table 6.

$Q$ values for all the applied magnetic field cases, obtained by the different procedures shown in this study.

$\mathit{H}\left(\mathit{O}\mathit{e}\right)$	${\mathit{Q}}_0=\frac{{\mathit{f}}_{\mathit{r}}}{\mathsf{\Delta }\mathit{f}}$	${\mathit{Q}}_1\approx \frac{{\mathit{f}}_{\mathit{r}}}{{\mathit{f}}_{\mathit{m}}^{\text{'}}-{\mathit{f}}_{\mathit{M}}^{\text{'}}}$	${\mathit{Q}}_{\mathit{f}\mathit{i}\mathit{t}1}$	${\mathit{Q}}_{\mathit{f}\mathit{i}\mathit{t}2}$	${\mathit{Q}}_{\mathit{c}\mathit{a}\mathit{l}}=\frac{{\mathit{f}}_{\mathit{m}}^2+{\mathit{f}}_{\mathit{M}}^2}{{\mathit{f}}_{\mathit{m}}^2-{\mathit{f}}_{\mathit{M}}^2}$
$0.6$	$333$	$290$	$208$	$283$	290
$2$	$285$	$243$	$178$	$229$	$243$
$16$	$1762$	$1410$	$1067$	$1321$	$1410$