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Fig. 4

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Case of ϵ = 0.2 and St = 0.01 (model E0v02S0v01c), showing the time evolution of the dimensionless diffusion coefficients, αg,i, in each direction (top). The lower panel shows the expected linear growth rates for the same model in the inviscid case (left) and for αg,i = 5 × 10−6 (right). These have been obtained from linear theory (see Appendix A) using D = ν = αg,icsHg. Here, K~x,z=kx,zηR0$\[\tilde{K}_{x, z}=k_{x, z} \eta R_{0}\]$ are the dimensionless wavenumbers.

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