Table 6: Characteristics of the source term derived in the local analysis at 1420 MHz for $\vert b_{\rm gal}\vert {\protect\ga} 45^{\circ}$ ( $c^{\rm src}_{1}$ ) and $\vert b_{\rm gal}\vert {\protect\la} 45^{\circ}$ ( $c^{\rm src}_{2}$ ).
Parameter, x $x_{\rm min}$ $x_{\rm max}$ $\langle x \rangle$ $\sigma_{x}$ $\%~(x \in \langle x \rangle \pm \sigma_{x})$

${\rm log}~(c^{\rm src}_{1}/{\rm mK}^2)$ -2.30 -0.75 -1.50 0.42 66

${\rm log}~(c^{\rm src}_{2}/{\rm mK}^2)$ -2.00 0.18 -0.86 0.53 72

**Table 6:** Characteristics of the source term derived in the local analysis at 1420 MHz for $\vert b_{\rm gal}\vert {\protect\ga} 45^{\circ}$ ( $c^{\rm src}_{1}$ ) and $\vert b_{\rm gal}\vert {\protect\la} 45^{\circ}$ ( $c^{\rm src}_{2}$ ).
Parameter, x	$x_{\rm min}$	$x_{\rm max}$	$\langle x \rangle$	$\sigma_{x}$	$\%~(x \in \langle x \rangle \pm \sigma_{x})$
${\rm log}~(c^{\rm src}_{1}/{\rm mK}^2)$	-2.30	-0.75	-1.50	0.42	66
${\rm log}~(c^{\rm src}_{2}/{\rm mK}^2)$	-2.00	0.18	-0.86	0.53	72

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