Table 2.
Summary of the spectral analysis of nine NuSTAR observations of Her X-1.
35 d | Max. flux | Observed | Line | Line | Ecyc | Ecut | Efold | Power- |
---|---|---|---|---|---|---|---|---|
cycle | of 35 d | line | width | strength (a) | norm. to 6.8 | law | ||
no. (e) | cycle | energy | σ | ASM-cts s−1 | index | |||
[ASM-cts s−1] | [keV] | [keV] | [keV] | [keV] | [keV] | [keV] | Γ | |
427 | 6.60 ± 0.37 | 37.40 ± 0.25 (b) | 5.76 ± 0.29 | 8.86 ± 0.87 | 37.54 ± 0.25 | 20.68 ± 0.27 | 9.95 ± 0.13 | 0.920 ± 0.004 |
457 | 2.96 ± 0.20 | 34.79 ± 0.22 | 4.46 ± 0.22 | 4.70 ± 0.70 | 37.38 ± 0.24 (c) | 19.86 ± 0.12 | 9.37 ± 0.09 | 0.929 ± 0.003 |
468 | 6.50 ± 0.20 | 37.18 ± 0.14 | 5.97 ± 0.18 | 8.83 ± 0.44 | 37.38 ± 0.14 (c) | 20.86 ± 0.15 | 10.16 ± 0.07 | 0.985 ± 0.001 |
478 | 4.10 ± 0.20 | 35.62 ± 0.18 | 4.94 ± 0.20 | 5.90 ± 0.40 | 37.44 ± 0.19 | 19.98 ± 0.16 | 9.79 ± 0.09 | 0.962 ± 0.002 |
484 | 4.09 ± 0.19 | 35.67 ± 0.29 | 4.84 ± 0.33 | 6.10 ± 0.70 | 37.50 ± 0.30 | 20.04 ± 0.11 | 10.16 ± 0.07 | 0.963 ± 0.002 |
490 | 5.60 ± 0.46 | 36.65 ± 0.16 | 5.61 ± 0.25 | 8.44 ± 0.59 | 37.46 ± 0.16 | 20.45 ± 0.23 | 9.79 ± 0.09 | 0.974 ± 0.002 |
494 | 5.02 ± 0.46 | 36.28 ± 0.22 | 5.26 ± 0.24 | 7.21 ± 0.53 | 37.48 ± 0.23 | 19.56 ± 0.12 | 9.65 ± 0.11 | 0.885 ± 0.002 (f) |
495 | 3.72 ± 0.56 | 35.36 ± 0.41 | 4.76 ± 0.45 | 6.38 ± 0.98 | 37.44 ± 0.43 | 19.62 ± 0.29 | 9.49 ± 0.24 | 0.934 ± 0.005 |
498 (d) | 4.00 ± 0.37 | 35.65 ± 0.21 | 5.01 ± 0.25 | 7.02 ± 0.50 | 37.54 ± 0.22 | 19.81 ± 0.16 | 9.38 ± 0.09 | 0.932 ± 0.001 |
Notes. The spectral parameters were found by applying the XSPEC-function highecut (see text). Uncertainties are at the 1 sigma (68%) level. The maximum flux of the respective 35-day cycle is given in units of (ASM-cts s−1), referring to the All Sky Monitor of RXTE. The corresponding physical flux in units of (keV cm−2 s) is found by multiplying with 0.2367. The flux was measured by Swift/BAT and converted according to (2–10 keV) (ASM-cts s−1) = 93.0 × (15–50 keV) (BAT-cts cm−2 s) (Staubert et al. 2016). The observed line energy was normalized to an ASM count rate of 6.8 cts s−1 using a slope of (0.675 ± 0.075) keV/(ASM-cts s−1) (see Fig. 1).
the values for the CRSF are from Fürst et al. (2013), Obs. II (Table 3, HighE);
in Staubert et al. (2016, 2017) the flux normalization was done with a slope of 0.44 (instead of 0.675);
35-day cycle numbering is according to Staubert et al. (1983);
observation at a high 35-day phase, Γ expected to be lower (Vasco 2012).
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