Open Access
Table 1
The new spectroscopic and polarimetric data used in our analysis.
Instrument | HJD | Phase | SNR | ⟨ Bz ⟩ | ⟨ B ⟩ (G) | Window | RV | ||
(G) | Fe ii λ6149 | Nd iii λ5050 | Nd iii λ6145 | (Å) | (km s-1) | ||||
|
|||||||||
ESPaDOnS | 2 454 553.119 | 0.991 | 250 | 4900 ± 45 | 13 900 ± 380 | 12 600 ± 340 | 12 400 ± 280 | 3690–10 481 | −9 |
ESPaDOnS | 2 454 553.150 | 0.995 | 250 | 4856 ± 42 | 3690–10 481 | −9 | |||
ESPaDOnS | 2454 652.793 | 0.258 | 320 | 1985 ± 31 | 15 400 ± 380 | 16 300 ± 340 | 16 800 ± 280 | 3690–10 481 | −9 |
HARPS | 2 453 463.898 | 0.803 | 80 | 13 600 ± 420 | 14 900 ± 410 | 15 100 ± 420 | 3783–6914 | −9 | |
HARPS | 2 453 582.645 | 0.034 | 90 | 13 600 ± 500 | 11 900 ± 680 | 12 000 ± 670 | 3783–6914 | −9 | |
HARPS | 2 453 583.693 | 0.142 | 40 | 13 900 ± 420 | 14 100 ± 550 | 14 200 ± 570 | 3783–6914 | −9 | |
HARPS | 2 454 223.642 | 0.056 | 70 | 13 200 ± 310 | 12 300 ± 510 | 13 000 ± 410 | 3783–6914 | −9 | |
HARPS | 2 454 633.613 | 0.283 | 55 | 14 700 ± 250 | 16 400 ± 410 | 16 400 ± 340 | 3783–6914 | −8 | |
HARPS | 2 454 869.850 | 0.615 | 70 | 13 800 ± 420 | 15 700 ± 680 | 15 300 ± 570 | 3783–6914 | −8 | |
HARPS | 2 454 870.879 | 0.721 | 60 | 13 600 ± 420 | 14 700 ± 680 | 15 900 ± 570 | 3783–6914 | −8 | |
UVES | 2 451 692.894 | 0.390 | 220 | 15 900 ± 210 | 17 000 ± 280 | 16 400 ± 380 | 4795-6745 | ||
FLAMES–UVES | 2 454 256.625 | 0.453 | 150 | 16 500 ± 340 | 16 400 ± 510 | 16 900 ± 420 | 4200-6200 | −8 |
Notes. Recorded are the HJD and derived phases for each spectra. The values of ⟨ Bz ⟩ for the ESPaDOnS spectra are shown followed by ⟨ B ⟩ values for all spectra measured from three spectral lines: Fe ii λ6149, Nd iii λ5050 and λ6145.
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