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Table 3.

Parameters related to the study of the longitudinal field measurements from various LSD line masks.

Parameter Complete He excluded Balmer Fe II Si II He I
g 1.1906 1.1877 1.5000 1.1939 1.1446 1.2474
λ (nm) 505.99 508.79 486.13 516.79 508.46 478.18
⟨EW⟩ (km s−1) 2.96 ± 0.10 1.83 ± 0.11 1.34 ± 0.10 3.41 ± 0.30 8.74 ± 0.21
Int. range (km s−1) ±65 ±60 ±100 ±60 ±60 ±65
B0 (G) 344 ± 6 821 ± 11 531 ± 32 1679 ± 31 724 ± 22 27 ± 9
B1 (G) 568 ± 9 1340 ± 15 913 ± 45 2905 ± 43 1053 ± 30 82 ± 14
B2 (G) 61 ± 8 168 ± 13 64 ± 46 383 ± 37 57 ± 29 1 ± 12
ϕ1 0.719 ± 0.002 0.722 ± 0.002 0.741 ± 0.007 0.722 ± 0.002 0.735 ± 0.004 0.676 ± 0.022
ϕ2 0.46 ± 0.02 0.45 ± 0.01 0.77 ± 0.10 0.43 ± 0.01 0.36 ± 0.08 0.70 ± 0.14

Notes. We provide the mean Landé factor g and the mean wavelength λ from the LSD calculation, as well as the resulting mean equivalent width (EW) of the LSD Stokes I profiles. The integration range around the line centroid for the calculation of the longitudinal magnetic field (see Eq. (2)) and determination of the FAP is given, as well as the resulting parameters of the dipole with a quadrupole contribution model (i.e., Eq. (4)) fitted to the measured longitudinal field. The detection status following the computed FAP value for a specific observation and LSD line mask is provided in Table A.2, when not all observations had a definite detection for that specific line mask.

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