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Table 3

Mode frequencies (kilohertz) from the B sequence simulations in CFC.

Model F H1 2f0 2p1 2f2 2f−2 δF δH1 δ2f0 δ2p1 tax t3D
B0 1.443 3.953 1.595 3.714 1.564 1.564 1.06 0.46 0.58 0.31 25.0 25.0
B1 1.429 3.915 1.634 3.701 1.118 1.945 1.57 0.32 0.34 0.32 25.0 25.0
B2 1.392 3.914 1.674 3.647 0.881 2.072 1.37 0.33 0.27 0.52 25.0 25.0
B3 1.359 3.953 1.718 3.572 0.681 2.159 1.99 0.27 0.51 0.33 25.0 25.0
B4 1.327 4.003 1.759 3.482 0.514 2.216 3.12 0.27 0.70 0.22 25.0 25.0
B5 1.287 4.073 1.800 3.395 0.320 2.276 4.03 0.02 0.63 0.14 25.0 25.0
B6 1.246 4.122 1.840 3.292 0.138 2.312 5.74 0.10 1.18 0.35 25.0 24.4
B7 1.210 4.193 1.881 3.199 −0.055 2.353 12.36 0.33 1.48 0.36 25.0 19.3
B8 1.172 4.224 1.921 2.990 −0.235 2.392 8.54 0.28 1.10 3.65 24.1 17.1
B9 1.130 4.177 1.960 2.912 −0.471 2.459 19.60 6.54 2.23 3.83 20.4 14.9

Notes. The axisymmetric frequencies (F, H1, 2f0, 2p1) correspond to perturbed axisymmetric simulations, while the nonaxisymmetric ones (2f2, 2f−2) are extracted from the nonaxisymmetric simulations. The relative errors (%) of the axisymmetric modes with respect to the results in Dimmelmeier et al. (2006), as well as the total simulation times (in milliseconds) for each type of simulation, are displayed in the right-hand part of the table.

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