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Table 1.

Input parameters and output diagnostics of the numerical simulation runs (see main text for definitions).

Name δ0 Lu0 Pr ⋅ 102 t1ωA0 δ ¯ 1 $ \overline{\delta}_1 $ Lu ¯ 1 $ \overline{\mathrm{Lu}}_1 $ σ / ω ¯ A 1 $ \sigma/\overline{\omega}_{\mathrm{A}1} $
TU0(1) 0 917 26.6 0 677 1.09
TU1 0 611 50.6 0 406 1.09
TU2 0 367 31.5 0 242 1.06
TU3 0 244 51.4 0 122 0.90
TU4 0 122 61.6 0 30 0.28
TU5 0 61 40.9 0 10 Stable
TU6 0 31 26.1 0 3 Stable
TS1(1) 8 917 1 24.3 3.5 681 0.94
TS2(1) 63 917 1 24.2 27 682 0.77
TS3(1) 126 917 1 26.0 54 680 0.60
TS4(1) 209 917 1 25.2 90 681 0.43
TS5(1) 300 917 1 26.9 130 678 0.28
TS6(1, 2) 419 917 1 24.5 180 682 0.16
TS7(1) 628 917 1 27.7 272 678 0.07
TS8(1) 900 917 1 27.3 321 678 0.04
TS9(2) 419 458 2 11.6 180 342 Stable
TS10(2) 419 1833 0.5 46.0 180 1367 0.47
TS11(2) 419 3667 0.25 91.2 180 2735 0.68
TS12(2) 419 7333 0.125 173.2 180 5481 0.85
TS13 628 458 2 13.8 272 339 Stable
TS14 739 306 3 9.3 321 226 Stable
TS15 739 397 2.31 12.1 321 293 Stable
TS16 739 611 1.5 18.3 321 452 Stable
TS17 63 57 16 1.7 27 42 Stable
TS18 63 458 2 12.7 27 340 0.55

Notes. Superscripts (1) and (2) in the run names indicate a run pertaining to the simulation subsets 1 and 2, respectively (see Fig. 9). The time at which the nonaxisymmetric perturbations are introduced is t1. The final column reports the growth rate of the m = 1 mode, with “Stable” indicating decaying perturbations. All runs have a magnetic Prandtl number of Pm = 1. For all stratified runs, the ratio of the thermal diffusion rate to the mean Alfvén frequency at the perturbation time is ϵ ¯ 1 = 0.15 $ \overline{\epsilon}_1 = 0.15 $.

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