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Table 2.

Properties of the magnetic maps.

Star Epoch ⟨|BV|⟩ |Bmax| B2 fpol ftor fdip fquad foct faxi faxi, pol faxi, tor
[rad s−1] [G] [G] [×102 G2] [%] [%] [%] [%] [%] [%] [%] [%]
HD 1835 2018.77 0.018 ± 0.008 7.4 29.3 0.78 91.1 8.9 32.1 28.4 27.4 6.4 6.9 1.2
HD 43162 2019.01 11.0 23.3 1.50 63.8 36.2 84.0 11.1 3.5 63.9 45.7 96.0
HD 43162 2019.22 16.4 36.1 3.33 36.9 63.1 62.5 25.8 7.9 83.9 61.8 96.8
HD 82443 2019.22 0.114 ± 0.022 23.6 65.1 7.05 63.9 36.1 34.3 46.8 9.2 36.1 4.6 92.0
HD 114710 2019.23 1.3 3.4 0.02 88.6 11.4 59.9 25.4 9.8 31.4 25.0 80.9
HD 189733 2018.89 0.110 18.8 56.5 5.50 52.1 47.9 67.7 16.1 8.2 43.6 1.5 89.5
HD 206860 2018.57 0.109 ± 0.004 20.8 47.7 5.10 85.5 14.5 46.8 16.8 13.5 64.6 61.0 85.7
HD 206860 2019.55 0.051 ± 0.042 15.8 35.3 2.80 69.2 30.8 59.4 21.0 10.5 73.4 65.2 91.9

Notes.

The following quantities are listed: star’s name, epoch of observations, differential rotation rate, mean unsigned magnetic strength, maximum unsigned magnetic strength, total reconstructed magnetic energy, poloidal and toroidal magnetic energy as a fraction of the total energy, dipolar, quadrupolar, and octupolar magnetic energy as a fraction of the poloidal energy, axisymmetric magnetic energy as a fraction of the total energy, poloidal axisymmetric energy as a fraction of the poloidal energy, and toroidal axisymmetric energy as a fraction of the toroidal energy. The symbol † indicates that the value from Fares et al. (2017) was used.

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