The no-selection argument #
For the two θ₀-independent vanishing-viscosity families κ_j^{(1)} = ½ ε_{2j+1}^p,
κ_j^{(2)} = 2 ε_{2j+1}^p (p = 2β/(qβ+1)), with cosine data c cos(2π n x₀) for infinitely many
modes n, the two families have limits (transport weak solutions) which are HolderTimeL2Le ν η-close
for large j, and whose norms differ at some time in [0,1].
The no-selection statement (conditional-input form of the repaired no-selection argument).
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