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Fig. 2

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Reference solution to the Kelvin–Helmholtz problem with initial Mach number M$\[\boldsymbol{\mathcal{M}}\]$0 = 10−2. The solution was computed using PSH reconstruction and the LHLLC flux function on an 8192 × 4096 grid. The mass fraction X of the passive scalar is shown at four points in time: late in the linear growth of the instability (t = 0.2 M$\[\boldsymbol{\mathcal{M}}\]$0−1), at an early stage of nonlinear evolution (t = 0.4 M$\[\boldsymbol{\mathcal{M}}\]$0−1), at a stage when the primary vortices have fully formed (t = 0.8 M$\[\boldsymbol{\mathcal{M}}\]$0−1; the final time for all of our other Kelvin–Helmholtz simulations), and at a late stage when fine threads have formed inside the primary vortices (t = 1.6 M$\[\boldsymbol{\mathcal{M}}\]$0−1). We use the same color scale as in Figs. 4, D.2, and D.1, although 0 ≲ X & ≲ 1 in the reference solution.

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