Table 2
Summary of the diagnostic quantities of Runs A–E.
| Run | P1 [yr] (N) | P2 [yr] (N) | P1 [yr] (S) | P2 [yr] (S) | Beq [G] |
|
|
|
|
|
|
Pasym | ||||||||
|
|
||||||||||||||||||||
| A | 2.96 ± 0.22 | 4.04 ± 0.70 | 2.85 ± 0.25 | 4.05 ± 0.24 | 3931 | 11 412 | 0.119 | 0.066 | 0.052 | 12.1 | 92.4 | no | ||||||||
| B | 5.45 ± 0.20 | 7.88 ± 0.57 | 6.5 ± 1.5 | 8.7 ± 1.4 | 2956 | 11 339 | 0.068 | 0.038 | 0.030 | 16.1 | 114.8 | no | ||||||||
| BC | 10.6 ± 0.33 | – | 10.8 ± 0.66 | – | 2724 | 11 150 | 0.060 | 0.033 | 0.026 | – | – | no | ||||||||
| C | 7.0 ± 1.1 | – | – | – | 1789 | 10 686 | 0.028 | 0.017 | 0.012 | 37.6 | 36.9 | yes | ||||||||
| D | 6.9 ± 1.1 | – | 9.4 ± 1.3 | – | 3152 | 9220 | 0.120 | 0.064 | 0.053 | 2.2 | 1.2 | yes | ||||||||
| E | 4.49 ± 0.38 | 2.60 ± 0.67 | 2.58 ± 0.88 | – | 3472 | 8792 | 0.156 | 0.080 | 0.076 | 1.9 | 2.2 | yes | ||||||||
Notes. Here, Emag = ⟨ B2 ⟩ /2μ0 is the total magnetic energy, 
and 
are the poloidal and toroidal components of the energy of the azimuthally averaged magnetic field. All quantities are averaged over volume and in time over the thermally relaxed state. The last two columns show the ratios of the meridional circulation and rotational energies from hydrodynamic to the magnetic simulations.The first four columns list the candidate periods detected with the D2 statistics separately for the northern and southern hemispheres. In a multi-periodic case, the boldface font indicates the most significant period. The last column marks cycle period asymmetry between the two hemispheres.
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