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Table 1

X-ray spectral fitting results for the combined spectrum.

Model NHlocal$N\rm{_{H}^{local}}$ kT norm τ χν2$\chi^2_{\nu}$2/d.o.f.) FX[FXISMcor]$F_X$[$F\mathrm{_X^{ISMcor}}$] LX[LXISMcor]$L_X$[$L\mathrm{_X^{ISMcor}}$]
(1022 cm−2) keV cm−5 (1010 s cm−3 (10−13 erg cm−2 s−1) (1032erg s−1)
Aa 1.460.18+0.231.46$_{-0.18}^{+0.23}$ 0.67±0.09 (0.810.19+0.37)e3(0.81$_{-0.19}^{+0.37}$)e$-$3 1.08 (273.22/253) 1.450.05+0.01[2.8]1.45$_{-0.05}^{+0.01}$[2.8] 3.110.11+0.02[5.99]3.11$_{-0.11}^{+0.02}$[5.99]
2.970.35+0.512.97$_{-0.35}^{+0.51}$ (1.750.32+0.35)e4(1.75$_{-0.32}^{+0.35}$)e$-$4
Bb 4.260.27+0.314.26$_{-0.27}^{+0.31}$ 0.850.16+0.190.85$_{-0.16}^{+0.19}$ (1.070.21+0.44)e3(1.07$_{-0.21}^{+0.44}$)e$-$3 17.824.79+7.9617.82$_{-4.79}^{+7.96}$ 1.0 (251.78/253) 1.450.22+0.04[2.06]1.45$_{-0.22}^{+0.04}$[2.06] 3.110.48+0.09[4.41]3.11$_{-0.48}^{+0.09}$[4.41]
3.190.74+3.013.19$_{-0.74}^{+3.01}$ (1.710.96+1.0)e4(1.71$_{-0.96}^{+1.0}$)e$-$4

Notes. Model A corresponds to tbabs× phabs× Σvapec, and Model B corresponds to tbabs × phabs× Σvpshock. The plasma temperature is expressed in kilo-electronvolts, with a normalisation parameter defined as 10144πD2nenH,dV$\frac{10^{-14}}{4\pi D^2}\int n_e n_H , dV$, where ne and nH denote the electron and hydrogen densities, integrated across the emitting volume, V. Here, D represents the distance to the source in centimetres (Smith et al. 2001). τ is the upper limit on the ionisation timescale. We show the absorbed 0.5–8 keV flux, the corresponding luminosity, and in brackets the ISM-corrected values. All uncertainties are quoted at the 1σ confidence level. Abundances of specific elements that were varied are as follows: (a)S=2.03±0.30, Ar=2.68±0.9(b)Fe=3.520.96+1.25$_{-0.96}^{+1.25}$.

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