Documentation

LeanPool.EscauriazaSereginSverak.LPS.MixedCrossFiniteLimits

Finite Serrin cross-density limits #

The energy interpolation and the Serrin mixed norm provide the two oriented convection pairings needed for the finite-exponent cross identity.

theorem ESS.lps_mixed_cross_density_limits_finite {T : ℝ} {a : CKN.Foundation.Parabolic.Vec3 → CKN.Foundation.Parabolic.Vec3} {u v : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3} {Du Dv : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3} {pu pv : CKN.Foundation.Parabolic.ParabolicPoint → ℝ} {s : ℝ} (hULH : CKN.IsLerayHopfSolution T a u Du) (hVLH : CKN.IsLerayHopfSolution T a v Dv) (hU : IsSerrinWeakSolution T a u Du pu) (hV : IsSerrinWeakSolution T a v Dv pv) (hs : 3 < s) (hmix : ∫⁻ (t : ℝ) in Set.Ioo 0 T, (∫⁻ (x : CKN.Foundation.Parabolic.Vec3), ENNReal.ofReal (CKN.Foundation.Parabolic.vec3EuclideanNorm (u (x, t))) ^ s) ^ (2 * s / (s - 3) / s) < ⊤) :

Both oriented cross densities have the required finite-exponent integrability and cutoff-mollification limits. The first product is the distinguished velocity against the rival's advective convection.