Separation persists for the two θ₀-independent vanishing-viscosity families #
Step "separation persists" of the corrected no-selection argument.
p := 2β/(q+1); the two θ₀-independent diffusivity families κ_j^{(1)} = ½ ε_{2j+1}^p,
κ_j^{(2)} = 2 ε_{2j+1}^p. For infinitely many cosine modes the two vanishing-viscosity families
stay
separated in L² norm at a fixed time, uniformly in large j.
Equations
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