Table 2
Evolution timesteps of the peaks.
| t [s] |
|
|
|
|
|
|||
| t1 ≡ tstart | 0 | 0 | SI |
| t2 ≡ tmid | 51 (25.5) | 8.5 | |
| t3 ≡ tend | 102 (51) | 17 | |
|
|
|||
| t1 ≡ tstart | 0 | 0 | SII |
| t2 ≡ tmid | 20.4 | 1.28 | |
| t3 ≡ tend | 40.8 | 2.55 | |
|
|
|||
| t1 ≡ tstart | 0 | 0 | SIII |
| t2 ≡ tmid | 22.53 (21.42) | 2.04 | |
| t3 ≡ tend | 45.05 (42.84) | 4.08 | |
|
|
|||
| t1 ≡ tstart | 0 | 0 | SIV |
| t2 ≡ tmid | 54 (28.9) | 12.75 | |
| t3 ≡ tend | 108 (57.8) | 25.5 | |
Notes. The labels start, mid and end stand for the times of the decay until the final dissipation of the peak mode. The time tmid is defined as the half-time of the decay cycle. Note that the peak at smaller wavenumber 
remains visible significantly longer than the other peak. The values denoted in brackets are the middle and end of the simulations that were not performed until the final dissipation of the peak due to the long computational times. In these cases we estimated of the total decay by an exponential fit of the decay curve.
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