Table A.2
Energy conversion factors.
| Detector | Filter | f 1 | f 2 | f 3 | f 4 | f 5 |
|
|
||||||
| pn | thin | 11.150 | 8.132 | 5.839 | 1.943 | 0.463 |
| medium | 9.976 | 7.897 | 5.758 | 1.926 | 0.465 | |
| thick | 6.329 | 6.071 | 4.964 | 1.824 | 0.459 | |
| MOS1 | thin | 2.118 | 1.937 | 2.064 | 0.744 | 0.144 |
| medium | 1.891 | 1.883 | 2.029 | 0.735 | 0.144 | |
| thick | 1.273 | 1.530 | 1.807 | 0.705 | 0.142 | |
| MOS2 | thin | 2.117 | 1.938 | 2.070 | 0.748 | 0.152 |
| medium | 1.886 | 1.884 | 2.034 | 0.740 | 0.152 | |
| thick | 1.264 | 1.530 | 1.812 | 0.710 | 0.150 | |
Notes. Energy conversion factors fi in units of 1011 cts cm2 erg-1 for the standard bands 1−5, respectively: (0.2−0.5) keV, (0.5−1.0) keV, (1.0−2.0) keV, (2.0−4.5) keV, and (4.5−12.0) keV. A power law with photon index of Γ = 1.7 and foreground absorption of NH,Gal = 6 × 1020 cm-2 was used.
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