Table 1
XMM-Newton observations of HD 168112 and HD 167971.
Obs. | Obs. ID. | Duration (ks) | JD-2450000 | EPIC filter | Target on axis | ϕHD 168112 | HD 16797 | ||
---|---|---|---|---|---|---|---|---|---|
Putkuri | Blomme | ϕinner | ϕouter | ||||||
1 | 0008820301 | 9.1 | 2372.56 | Thick | – | 0.096 | 0.063 | 0.49 | 0.697 |
2 | 0008820601 | 13.4 | 2526.78 | Thick | – | 0.396 | 0.364 | 0.92 | 0.717 |
3 | 0740990101 | 23.8 | 6909.73 | Medium | HD 167971 | 0.931 | 0.921 | 0.45 | 0.278 |
4 | 0920040401 | 12.5 | 10009.81 | Thick | HD168112 | 0.968 | 0.974 | 0.75 | 0.676 |
5 | 0920040501 | 11.5 | 10025.98 | Thick | HD168112 | 0.000 | 0.006 | 0.62 | 0.678 |
6 | 0920040601 | 11.5 | 10042.45 | Thick | HD168112 | 0.032 | 0.038 | 0.58 | 0.680 |
Notes. The durations indicated in the third column correspond to the effective exposure time of the EPIC-MOS camera (i.e. after removing the time interval affected by a flare in the first and third observation). The Julian day given in Col. 4 is evaluated at mid-exposure. The last four columns yield the orbital phases respectively for HD 168112 (Putkuri et al. 2023; Blomme et al. 2024), the eclipsing inner binary of HD 167971 (Ibanoglu et al. 2013) and the orbit of the outer component of HD 167971 (Le Bouquin et al. 2017).
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