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Table 1.

Summary of NuSTAR observations of GX 301−2.

Date φorb(a) L 37 NS $ \mathcal{L}_{37}^\mathrm{NS} $(b) Observation ID Exposure [ks] ECRSF1 [keV] ECRSF2 [keV] Reference
2014-10-29 0.67 0.71 30001041002 38.2 34 . 7 1.4 + 2.1 $ 34.7^{+2.1}_{-1.4} $ 50 . 6 1.7 + 2.1 $ 50.6^{+2.1}_{-1.7} $ Fürst et al. (2018)
2015-10-04 0.87 1.08 30101042002 35.7 34 . 5 1.4 + 1.6 $ 34.5^{+1.6}_{-1.4} $ 49 . 6 1.2 + 1.3 $ 49.6^{+1.3}_{-1.2} $ Fürst et al. (2018)
2019-03-03 0.93 3.69 90501306002 23.0 36.7 ± 0.3 55 . 1 0.6 + 0.7 $ 55.1^{+0.7}_{-0.6} $ Nabizadeh et al. (2019)
2020-12-27 0.97 5.02 30601013002 48.5 37 . 4 1.0 + 1.1 $ 37.4^{+1.1}_{-1.0} $ 51 . 5 1.0 + 1.1 $ 51.5^{+1.1}_{-1.0} $ This work
2022-02-02 0.67 0.55 30701001002 35.6 35 . 4 0.2 + 0.6 $ 35.4^{+0.6}_{-0.2} $(c) 54 ± 2 (c) McCulloch et al. (in prep.)

Notes.

(a)

Orbital phase, which is calculated in the same manner as described in the caption of Fig. 1.

(b)

Absorbed luminosity in units of 1037 erg s−1 in the energy band 5–50 keV in the NS rest frame as obtained directly from the NuSTAR data. In order to transform the value from the observer’s frame to the NS frame, the obtained values are multiplied by (1 + z)4, where z = 0.3, which takes the gravitational red-shift, time dilatation, and surface magnification into account.

(c)

The cyclotron line parameters for the most recent observation are preliminary results and subject to further analysis.

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