Open Access
Table 8.
Best-fitting partial-covering obscuration models to XM1, XM2, and XM4.
XM1 (2020 Dec. 26) | |||
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M2 (PC*(SXCOM+HXPL)+UXCL): | Obscurer | Soft comptonization | Hard comptonization |
χ2/d.o.f. = 625.28/644 = 0.971 |
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Tseed = 20 eV* |
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F0.5 − 2 = (1.13 ± 0.03)×10−13 erg cm−2 s−1 | CF = ![]() |
Te = 0.1 keV* | F1 − 10(a) = (3.77 ± 0.16)×10−13 erg cm−2 s−1 |
F0.2 − 5 = (3.79 ± 0.10)×10−13 erg cm−2 s−1 |
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NSC(b) = 3.97![]() |
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M2-alt (PC*(SXCOM+HXCOM)+UXCL): | Tseed = 20 eV*, Te = 100 keV* | ||
χ2/d.o.f. = 626.61/644 = 0.973 |
![]() ![]() |
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XM2 (2021 Jan. 28) | |||
M2 (PC*(SXCOM+HXPL)+UXCL): | Obscurer | Soft comptonization | Hard comptonization |
χ2/d.o.f. = 302.13/292 = 1.035 |
![]() |
Tseed = 20 eV* |
![]() |
F0.5 − 2 = (1.10 ± 0.04)×10−13 erg cm−2 s−1 | CF = ![]() |
Te = 0.1 keV* | F1 − 10(a) = (2.93 ± 0.22)×10−13 erg cm−2 s−1 |
F0.2 − 5 = (3.46 ± 0.12)×10−13 erg cm−2 s−1 |
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||
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NSC(b) = ![]() |
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M2-alt (PC*(SXCOM+HXCOM)+UXCL): | Tseed = 20 eV*, Te = 100 keV* | ||
χ2/d.o.f. = 302.96/292 = 1.038 |
![]() ![]() |
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XM4 (2022 Apr. 25) | |||
M2 (PC*(SXCOM+HXPL)+UXCL): | Obscurer | Soft comptonization | Hard comptonization |
χ2/d.o.f. = 177.07/175 = 1.012 |
![]() |
Tseed = 20 eV* |
![]() |
F0.5 − 2 = (2.5 ± 0.2)×10−14 erg cm−2 s−1 | CF = ![]() |
Te = 0.1 keV* | F1 − 10(a) = 1.54![]() |
F0.2 − 5 = (8.0 ± 0.5)×10−14 erg cm−2 s−1 |
![]() |
||
![]() |
NSC(b) = ![]() |
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M2-alt (PC*(SXCOM+HXCOM)+UXCL): | Tseed = 20 eV*, Te = 100 keV* | ||
χ2/d.o.f. = 176.50/175 = 1.009 |
![]() ![]() |
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