Table A.1.
Properties of the HHS22 modes in our nonlinear rotating convection simulations for 1 ≤ m ≤ 15. The values in parentheses show the results from our linear model 3-sub (δcz = −5 × 10−7 and δsf = 10−3). The frequencies are measured in the Carrington frame. The peak frequencies and linewidths (FWHM) are obtained by Lorentzian fits. The quantity max(vhori) represents the maximum surface horizontal velocity amplitude of the mode eigenfunction extracted using the singular-value-decomposition (SVD).
| m | Frequency | Linewidth | max(vhori) |
|---|---|---|---|
| [nHz] | [nHz] | [m s−1] | |
| 1 | -394.3 (-437.6) | 90.3 (166.7) | 0.4 |
| 2 | -360.8 (-399.9) | 104.4 (144.7) | 0.8 |
| 3 | -328.7 (-368.4) | 161.5 (124.8) | 0.7 |
| 4 | -316.4 (-341.2) | 133.2 (108.5) | 0.4 |
| 5 | -317.0 (-318.5) | 128.4 (96.1) | 1.9 |
| 6 | -296.2 (-299.8) | 133.0 (87.3) | 0.7 |
| 7 | -293.7 (-284.6) | 111.1 (81.9) | 1.9 |
| 8 | -285.4 (-272.7) | 121.8 (79.0) | 1.0 |
| 9 | -260.9 (-263.3) | 156.3 (78.2) | 2.1 |
| 10 | -256.0 (-256.1) | 205.5 (79.3) | 2.3 |
| 11 | -220.7 (-250.3) | 225.4 (81.9) | 1.1 |
| 12 | -216.7 (-245.6) | 237.8 (85.6) | 3.2 |
| 13 | -198.8 (-241.8) | 158.2 (89.9) | 1.3 |
| 14 | -195.0 (-238.8) | 181.7 (94.7) | 3.4 |
| 15 | -194.7 (-236.3) | 151.5 (99.8) | 3.5 |
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