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Figure 6 - Phase and amplitude evolution in the network of triadic interactions of the Hasegawa-Wakatani system

Figure 6. Time derivatives of the phases ϕ ± k for C = 1 case with k = (0, 1.125) and p = (−0.5, −1.0), corresponding to nonlinear frequencies. Notice that while dϕ − q /dt appears to oscillate wildly, since its amplitude χ − q is vanishingly small, as can be seen in figure 4, these oscillations are not important for the rest of the dynamics.
Time derivatives of the phases ϕ ± k for C = 1 case with k = (0, 1.125) and p = (−0.5, −1.0), corresponding to nonlinear frequencies. Notice that while dϕ − q /dt appears to oscillate wildly, since its amplitude χ − q is vanishingly small, as can be seen in figure 4, these oscillations are not important for the rest of the dynamics.
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