Table 7: Joint fits to EPIC-pn FF mode observations for a quadrupole dominated magnetic field ( $\beta _{\rm d}=0.05$ ) with $\mu =3.87$ and $\mathcal{O}= 11^{\circ}$ , forcing the hydrogen column density, the normalization constant and the magnetic field intensity to be the same for all observations. The best fit yields $\chi ^{2}=1192$ for 819 d.o.f.
Rev. $n_{\rm H}$ ${\cal B}$ $kT_{\rm pole}$ R/D₃₀₀ $B_{\rm p}$

(10²⁰ cm^-2) (eV) (10¹² G)

175 $\rm 1.23^{+0.04}_{-0.04}$ $\rm 73.9^{+6.0}_{-14.1}$ $\rm 104.6^{+0.4}_{-0.4}$ $\rm 12.7^{+1.0}_{-2.1}$ $\rm 18.2^{+1.6}_{-1.5}$

533 = $\rm 58.6^{+2.0}_{-2.4}$ $\rm 107.5^{+0.2}_{-0.3}$ = =

534 = $\rm 57.6^{+2.0}_{-2.4}$ $\rm 107.5^{+0.4}_{-0.3}$ = =

815 = $\rm 26.9^{+1.7}_{-0.6}$ $\rm 118.2^{+0.5}_{-0.2}$ = =

1086 = $\rm 31.8^{+0.9}_{-1.1}$ $\rm 116.3^{+0.5}_{-0.3}$ = =

**Table 7:** Joint fits to EPIC-pn FF mode observations for a quadrupole dominated magnetic field ( $\beta _{\rm d}=0.05$ ) with $\mu =3.87$ and $\mathcal{O}= 11^{\circ}$ , forcing the hydrogen column density, the normalization constant and the magnetic field intensity to be the same for all observations. The best fit yields $\chi ^{2}=1192$ for 819 d.o.f.
Rev.	$n_{\rm H}$	${\cal B}$	$kT_{\rm pole}$	R/D₃₀₀	$B_{\rm p}$
	(10²⁰ cm^-2)		(eV)		(10¹² G)
175	$\rm 1.23^{+0.04}_{-0.04}$	$\rm 73.9^{+6.0}_{-14.1}$	$\rm 104.6^{+0.4}_{-0.4}$	$\rm 12.7^{+1.0}_{-2.1}$	$\rm 18.2^{+1.6}_{-1.5}$
533	=	$\rm 58.6^{+2.0}_{-2.4}$	$\rm 107.5^{+0.2}_{-0.3}$	=	=
534	=	$\rm 57.6^{+2.0}_{-2.4}$	$\rm 107.5^{+0.4}_{-0.3}$	=	=
815	=	$\rm 26.9^{+1.7}_{-0.6}$	$\rm 118.2^{+0.5}_{-0.2}$	=	=
1086	=	$\rm 31.8^{+0.9}_{-1.1}$	$\rm 116.3^{+0.5}_{-0.3}$	=	=

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