Table 2.
Magnetic energy from the decomposition in the first 11 spherical harmonics (0 ≤ l, m ≤ 10) of the near-surface (r = 0.98R) radial magnetic field.
Run |
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τcyc[yr] |
---|---|---|---|---|---|---|---|---|---|
R1 | 1.4(−2) | 4.9(−3) | 1.6(−3) | 8.2(−4) | 7.5(−4) | 8.0(−4) | 8.5(−4) | 4.5(−3) | 1.8(m = 0) |
R2 | 1.5(−2) | 9.9(−3) | 3.7(−4) | 3.9(−4) | 4.2(−4) | 4.1(−4) | 4.8(−4) | 2.9(−3) | 1.7(m = 0) |
R3 | 1.8(−2) | 5.4(−3) | 8.2(−3) | 1.2(−3) | 7.5(−4) | 5.2(−4) | 4.4(−4) | 1.0(−3) | 3.3(m = 0) |
R4 | 5.0(−2) | 1.2(−2) | 2.6(−2) | 3.4(−3) | 1.7(−3) | 1.2(−3) | 1.0(−3) | 4.2(−3) | 2.8(m = 1) |
Notes. The labels indicate the energy in the corresponding m mode, in units of 105 J m−3. We define 0 ≤ l, m ≤ 5 the large-scale field. The numbers in parenthesis represent the power of ten. The last column indicates the characteristic time of the dynamo, calculated on the dominant mode and indicated in the subscript.
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