Table 2
Best-fit parameters for the emission lines for the 20 phases.
Phase | E1 | K1 | E2 | K3 | E3 | σ3 | K3 | ||||
---|---|---|---|---|---|---|---|---|---|---|---|
keV | 10−4 cts cm−2 s−1 | keV | 10−4 cts cm−2 s−1 | keV | keV | 10−4 cts cm−2 s−1 | |||||
Averagea | 0.51 ± 0.02 | 3.02![]() |
0.96 ± 0.02 | 3.55![]() |
6.64![]() |
0.36![]() |
1.70![]() |
||||
0 | 0.49 ± 0.03 | 11.2![]() |
0.98 ± 0.03 | 2.79![]() |
6.76![]() |
0.25![]() |
2.43![]() |
||||
1 | 0.51![]() |
6.98![]() |
0.94![]() |
1.91 ± 1.13 | 6.44![]() |
<0.39 | 1.33![]() |
||||
2 | 0.53![]() |
<10.8 | 1.02![]() |
2.69![]() |
6.76![]() |
0.45* | 2.28![]() |
||||
3 | 0.50![]() |
<21.9 | 0.97 ± 0.03 | 2.75![]() |
6.49![]() |
<0.48 | 0.92![]() |
||||
4 | 0.48![]() |
16.8![]() |
– | – | – | – | – | ||||
5 | 0.55![]() |
4.96![]() |
0.98 ± 0.03 | 3.12 ± 1.13 | 6.61![]() |
0.41![]() |
3.06![]() |
||||
6 | – | – | – | – | – | – | – | ||||
7 | – | – | 0.94 ± 0.03 | 2.69 ± 1.23 | – | – | – | ||||
8 | – | – | – | – | 6.74![]() |
0.28![]() |
1.80![]() |
||||
9 | – | – | 0.98![]() |
3.09![]() |
6.81![]() |
0.45* | 2.93 ± 1.13 | ||||
10 | 0.46 ± 0.04 | 16.0![]() |
– | – | – | – | – | ||||
11 | 0.50![]() |
14.7![]() |
0.94 ± 0.03 | 3.12 ± 1.17 | 6.76![]() |
0.45* | 2.97![]() |
||||
12 | 0.46![]() |
<8.90 | 0.97 ± 0.03 | 2.30![]() |
6.70![]() |
0.45* | 3.60![]() |
||||
13 | – | – | 0.96![]() |
1.70![]() |
– | – | – | ||||
14 | 0.51![]() |
7.49![]() |
0.99![]() |
1.85![]() |
6.9* | 0.44![]() |
2.52![]() |
||||
15 | – | – | 0.95![]() |
1.13![]() |
6.87![]() |
0.30![]() |
2.32![]() |
||||
16 | – | – | 1.02![]() |
1.76![]() |
6.42![]() |
0.30![]() |
1.79![]() |
||||
17 | – | – | – | – | 6.58![]() |
<0.29 | 1.67![]() |
||||
18 | 0.53 ± 0.03 | 6.41![]() |
1.00![]() |
2.25![]() |
6.45 ± 0.06 | <0.14 | 1.06 ± 0.53 | ||||
19 | 0.49 ± 0.02 | 24.2![]() |
– | – | 6.60![]() |
<0.60 | 1.38![]() |
Notes. All errors are in the 90% confidence range. (a) The line widths E1 and E2 were frozen to the value of 1 ev in the phase-resolved analysis because they are too narrow to be resolved by the pn detector. Nevertheless, E2 in the phase-averaged spectra is broader and has a width value of eV. (*) Parameter frozen.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.