OAI/Geometry/RCD/Sobolev/GradientProductAction.lean
3 declarations, 0 contain sorry, 0 declared as axioms
The gradient-product identity in terms of actual Hessian actions
This is the finite Sobolev-representative form of Gigli's formula (3.3.33). The identity itself is algebraic once the three Gram representatives exist.
- theorem
OAI.RegularPointCoordinates.localGamma_mixed_as_hessian_actionsline 21Source documentation
The two Hessian actions recover the derivative of the mixed Gram representative, including an arbitrary scalar shift.
theorem localGamma_mixed_as_hessian_actions (f a z G Fz Az : SobolevSpace μ hQ) (b : ℝ) : localGamma μ hQ (G-b • a) z =ᵐ[μ] fun x => (localHessianAction μ hQ f a z G Fz Az x-b*localGamma μ hQ a z x)+ localHessianAction μ hQ a f z G Az Fz x := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.localGamma, OAI.RegularPointCoordinates.localHessianAction
- theorem
OAI.RegularPointCoordinates.diagonal_le_of_two_actionsline 32 - theorem
OAI.RegularPointCoordinates.localGamma_shifted_mixed_boundline 48Source documentation
When the shifted mixed gradient is an admissible Hessian direction, the two action bounds give its exact factor-two gradient estimate.
theorem localGamma_shifted_mixed_bound (f a G Fz Az : SobolevSpace μ hQ) (b : ℝ) (A B : X → ℝ) (hA : ∀ᵐ x ∂μ, 0≤A x) (hB : ∀ᵐ x ∂μ, 0≤B x) (hfirst : ∀ᵐ x ∂μ, (localHessianAction μ hQ f a (G-b • a) G Fz Az x- b*localGamma μ hQ a (G-b • a) x)^2 ≤ A x*localGamma μ hQ (G-b • a) (G-b • a) x) (hsecond : ∀ᵐ x ∂μ, (localHessianAction μ hQ a f (G-b • a) G Az Fz x)^2 ≤ B x*localGamma μ hQ (G-b • a) (G-b • a) x) : ∀ᵐ x ∂μ, localGamma μ hQ (G-b • a) (G-b • a) x≤2*(A x+B x) := by …Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.localHessianAction, OAI.RegularPointCoordinates.localGamma