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Table 1

Recovered XRT spectral resolution.

Source Mode Epoch Exposure Line FWHMobserved FWHMcorrected ΔR

Cas A PC 2005/02 24.5 Si 108 ±    4
S 133 ±    6
Fe 268 ±    8
Cas A PC 2007/09 38.1 Si 138 ±    7 114 ±    2 0.17 ±    0.05
S 200 ±    11 146 ±    6 0.27 ±    0.06
Fe 318 ±    22 286 ±    21 0.10 ±    0.09
Cas A PC 2009/02 128.5 Si 154 ±    8 122 ±    2 0.21 ±    0.05
S 251 ±    18 163 ±    7 0.35 ±    0.08
Fe 372 ±    25 321 ±    14 0.14 ±    0.08
Tycho PC 2009/10 75.1 Si 179 ±    8 132 ±    3 0.26 ±    0.05
S 267 ±    14 182 ±    8 0.32 ±    0.06
Fe 381 ±    45 299 ±    31 0.21 ±    0.14
Tycho PC 2010/03 73.6 Si 177 ±    7 138 ±    3 0.22 ±    0.04
S 256 ±    10 184 ±    8 0.28 ±    0.05
Fe 381 ±    39 307 ±    32 0.19 ±    0.13
Tycho PC 2010/10 71.5 Si 192 ±    7 139 ±    7 0.28 ±    0.05
S 269 ±    11 192 ±    11 0.29 ±    0.06
Fe 387 ±    34 304 ±    27 0.21 ±    0.11
Cas A WT 2005/02 18.7 Si 101 ±    3
S 128 ±    6
Fe 263 ±    8
Cas A WT 2007/10 37.7 Si 159 ±    13 106 ±    3 0.33 ±    0.09
S 244 ±    15 138 ±    7 0.43 ±    0.07
Fe 383 ±    16 304 ±    15 0.21 ±    0.06
Cas A WT 2008/07 49.2 Si 161 ±    14 113 ±    4 0.30 ±    0.09
S 274 ±    17 154 ±    9 0.44 ±    0.08
Fe 393 ±    22 325 ±    17 0.17 ±    0.07
Cas A WT 2009/10 27.4 Si 177 ±    16 120 ±    3 0.32 ±    0.10
Tycho WT 2009/11 24.2 Si 196 ±    15 136 ±    7 0.31 ±    0.09
Tycho WT 2010/10 41.9 Si 219 ±    12 148 ±    5 0.32 ±    0.06

Notes. XRT instrumental full width half maximum (FWHM) ineV of the silicon, sulphur and iron Kα lines in the observed and the corrected spectra of each calibration epoch (specified as YYYY/MM). The total exposure time of the observations used for the trap analysis for each epoch is reported in kiloseconds (ks). The FWHM values at sulphur and iron are only reported when enough counts in the lines allowed a reliable fit. The Cas A lines are at energies ESi = 1.863   keV, ES = 2.456   keV, EFe = 6.626   keV, while for Tycho ESi = 1.856   keV, ES = 2.450   keV, EFe = 6.430   keV, as derived from our fits to XMM spectra; the differences in the line energies originate from the dynamics of the expanding SNR shells. The last column quantifies the improvement in the energy resolution ΔR defined as , where .

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