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LeanPool.AnomalousDiffusion.AVenhance.Infra.Section4.Amnr.CurveLocalImplicit

Smooth parameter dependence from the actual local Volterra equation.

The substitution derivative is the actual pointwise primitive state Jacobian operator, with no global derivative bound premise.

The actual residual is smooth on trajectories from local field smoothness.

The actual residual derivative follows from the local substitution rule.

theorem AVenhance.Infra.Section4.amnrCurveResidual_solution_contDiffAt_local {K E P : Type} [TopologicalSpace K] [CompactSpace K] [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [CompleteSpace E] [NormedAddCommGroup P] [NormedSpace ℝ P] {f : ℝ × E → E} (hf : ContDiff ℝ (↑⊤) f) (η : C(K, ℝ)) (V : C(K, E) →L[ℝ] C(K, E)) {Q R : P → C(K, E)} {x : P} (hQ : ContinuousAt Q x) (hR : ContDiffAt ℝ (↑⊤) R x) (heq : ∀ (y : P), amnrCurveResidual f ⋯ η V (Q y) = R y) (hsmall : ‖amnrCurveJacobianCoefficient f hf η V (Q x)‖ < 1) :
ContDiffAt ℝ (↑⊤) Q x

A continuous family solving the actual integral equation is smooth whenever the actual linearized Volterra operator is small at the reference curve. This is a local calculus criterion, not a flow regularity assumption.

theorem AVenhance.Infra.Section4.amnrCurveJacobianCoefficient_norm_le_along {K E : Type} [TopologicalSpace K] [CompactSpace K] [NormedAddCommGroup E] [NormedSpace ℝ E] {f : ℝ × E → E} (hf : ContDiff ℝ (↑⊤) f) (η : C(K, ℝ)) (V : C(K, E) →L[ℝ] C(K, E)) (u : C(K, E)) {M : ℝ} (hM : 0 ≤ M) (hstate : ∀ (t : K), ‖amnrStateDerivative f (η t, u t)‖ ≤ M) :

Primitive Jacobian bounds along a single actual reference trajectory control the local linearized Volterra operator.