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Table 2.

Parameters resulting from four different height-dependent inversions which were applied to the two sets of observed Stokes profiles ((a) and (b)) and to their corresponding deconvolved Stokes profiles ((c) and (d)) from the two selected LFPs.

Height-dependent inversions

Inversion technique n P C log(τ) B [kG] γ [ ° ] vLOS [km s−1] χ2 α BIC
(a) SPINOR 2D (observed) 18 −2.0 6.4 141 5.6
1 1 −0.8 8.0 148 9.3 14 1 98
0.0 8.3 145 8.3
−2.0 7.0 139 7.9
2 1 −0.8 8.0 146 9.3 35 1 119
0.0 7.4 173 12.1

(b) SPINOR 1D (observed) 37 1 −2.0 3.6 166 0.2 8 181
1 −0.8 4.0 155 0.4 0.48
0.0 4.2 146 0.5
−2.0 2.9 163 15.5
2 −0.8 3.9 177 17.5 0.52
0.0 4.4 179 17.4
2 −2.0 3.6 159 0.1 12 185
1 −0.8 4.0 154 0.3 0.35
0.0 4.2 144 1.1
−2.0 2.3 152 14.3
2 −0.8 4.0 169 17.0 0.65
0.0 5.1 179 16.0

(c) SPINOR 1D (deconvolved) 18 −2.0 2.5 100 9.8
1 1 −0.8 7.4 179 12.7 44 1 128
0.0 7.2 169 4.7
−2.0 2.9 67 8.5
2 1 −0.8 5.2 178 11.4 47 1 131
0.0 6.6 132 6.7

(d) SPINOR 1D (deconvolved) 37 1 −2.0 3.0 159 0.0 14 187
1 −0.8 3.5 170 0.5 0.42
0.0 4.0 178 1.0
−2.0 2.8 144 14.4
2 −0.8 4.0 171 16.5 0.58
0.0 4.9 179 17.7
2 −2.0 3.2 157 0.2 18 191
1 −0.8 3.8 157 0.6 0.39
0.0 4.2 156 1.1
−2.0 1.7 165 15.6
2 −0.8 4.0 172 17.1 0.61
0.0 5.8 176 16.4

Notes. From left to right: number of free parameters n, pixel identification number P, atmospheric component C, optical depth node log(τ), field strength B, field inclination γ, LOS velocity vLOS, merit function χ2, filling factor α for each component, and Bayesian Information Criterion (BIC) value.

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