Table 2.

Best-fitting parameters for the soft proton background power-law model, where |$\alpha _1$| is the power-law index before the break and |$\alpha _2$| is the index after the break. All parameters listed were allowed to vary, apart from |$\alpha _2$| in PN.

Detector|$\alpha _1$||$\alpha _2$|Break energy (keV)Normalization (10|$^{-4}$| arcmin|$^{-2}$|⁠)
MOS10.53 |$\pm$| 0.050.22 |$\pm$| 0.063.0|$^{+0.5}_{-0.2}$|3.0 |$\pm$| 0.2
MOS20.56 |$\pm$| 0.040.17 |$\pm$| 0.063.5|$^{+0.2}_{-0.3}$|2.7 |$\pm$| 0.1
PN0.4 |$\pm$| 0.42.50.98|$^{+0.05}_{-0.05}$|6 |$\pm$| 1
Detector|$\alpha _1$||$\alpha _2$|Break energy (keV)Normalization (10|$^{-4}$| arcmin|$^{-2}$|⁠)
MOS10.53 |$\pm$| 0.050.22 |$\pm$| 0.063.0|$^{+0.5}_{-0.2}$|3.0 |$\pm$| 0.2
MOS20.56 |$\pm$| 0.040.17 |$\pm$| 0.063.5|$^{+0.2}_{-0.3}$|2.7 |$\pm$| 0.1
PN0.4 |$\pm$| 0.42.50.98|$^{+0.05}_{-0.05}$|6 |$\pm$| 1
Table 2.

Best-fitting parameters for the soft proton background power-law model, where |$\alpha _1$| is the power-law index before the break and |$\alpha _2$| is the index after the break. All parameters listed were allowed to vary, apart from |$\alpha _2$| in PN.

Detector|$\alpha _1$||$\alpha _2$|Break energy (keV)Normalization (10|$^{-4}$| arcmin|$^{-2}$|⁠)
MOS10.53 |$\pm$| 0.050.22 |$\pm$| 0.063.0|$^{+0.5}_{-0.2}$|3.0 |$\pm$| 0.2
MOS20.56 |$\pm$| 0.040.17 |$\pm$| 0.063.5|$^{+0.2}_{-0.3}$|2.7 |$\pm$| 0.1
PN0.4 |$\pm$| 0.42.50.98|$^{+0.05}_{-0.05}$|6 |$\pm$| 1
Detector|$\alpha _1$||$\alpha _2$|Break energy (keV)Normalization (10|$^{-4}$| arcmin|$^{-2}$|⁠)
MOS10.53 |$\pm$| 0.050.22 |$\pm$| 0.063.0|$^{+0.5}_{-0.2}$|3.0 |$\pm$| 0.2
MOS20.56 |$\pm$| 0.040.17 |$\pm$| 0.063.5|$^{+0.2}_{-0.3}$|2.7 |$\pm$| 0.1
PN0.4 |$\pm$| 0.42.50.98|$^{+0.05}_{-0.05}$|6 |$\pm$| 1
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