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Table 2

Similar to Table 1 but for Chandra and eROSITA spectra.

ID HJD ϕ NH norm χ2/d.o.f FXobs $\[F_{\mathrm{X}}^{\text {obs }}\]$ Ct rate (cts s−1)
−2.45e6 (1022 cm−2) (10−2 cm−5) (2–10 keV) 2–5 keV 5–8 keV
26239 9573.664 0.63 15.7 ± 2.0 2.38 ± 0.24 30.80/36 1.63 ± 0.10
eROSITA1-4 13.5 ± 2.1 1.64 ± 0.31 22.55/27 1.19 ± 0.16
eROSITA1 8935.809 0.84 13.3 (10.2–18.7) 2.77 (1.79–4.45) 21.69/22 2.03 ± 0.70 0.42 ± 0.08 0.16 ± 0.07
eROSITA2 9120.731 0.23 22.2 (14.6–35.7) 1.78 (1.00–3.04) 1.04± 0.38 0.22 ± 0.05 0.11 ± 0.05
eROSITA3 9297.519 0.56 13.0 (6.7–17.9) 2.23 (0.99–3.28) 1.65 ± 0.49 0.46 ± 0.08 0.18 ± 0.07
eROSITA4 9480.901 0.93 46.0 (30.8–66.6) 4.64 (2.49–7.88) 1.71 ± 0.69 0.09 ± 0.03 0.20 ± 0.06

Notes. The absorbed thermal model has the form phabs(ISM) × phabs × apec with NHISM=2.7×1020 cm2$\[N_{\mathrm{H}}^{\mathrm{ISM}}=2.7 \times 10^{20} \mathrm{~cm}^{-2}\]$ and kT = 9.1 keV. Fluxes are provided in units 10−11 erg cm−2 s−1. For individual eROSITA spectra, the errors on absorbing column and normalization factors were very asymmetric, hence the 1σ confidence interval is provided instead.

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