Interior spatial analyticity of classical solutions #
The proof of thm:analytic:interior. On nested regions of depth τ ∈ (0, 1] inside a
compactly contained cylinder, the weighted derivatives (τ d)^k |∂^α g| of the velocity
components and the pressure are bounded by the majorant b_k ≤ M K^k k!, by induction on k:
the one-step estimate on a backward window one geometric step deeper, the absorption of the
provisional top-order bound, and the majorant arithmetic. At depth 1 this is the bound
AnalyticBoundOn u R' [s₁, s₂] M (d / K).
Compactness gives a finite bound at each fixed derivative order.
A finite bound at each fixed order for the velocity components and the pressure on the closed outer region.
The weighted bound at order k + 1 from the weighted bounds at orders ≤ k, by absorbing
the provisional bound (the compactness bound halves at each iteration).
The weighted bounds (τ d)^k |∂^α g| ≤ b_k at every depth τ and every order k, by
strong induction on the order.
The analyticity bound of thm:analytic:interior on one compactly contained cylinder.
thm:analytic:interior: a classical solution of eq:nse:forced on B(R) × (t₁, t₂) with
a locally uniformly spatially analytic force is locally uniformly spatially analytic.