Rescaling a short-time velocity average #
The averaging box centered at a dyadic midpoint is the affine preimage of the physical Gaussian averaging cylinder.
theorem
ESS.bu_short_average_rescaling_integral
(scale : ℝ)
(hscale : 0 < scale)
(Y : CKN.Foundation.Parabolic.Vec3)
(δ : ℝ)
(F : CKN.Foundation.Parabolic.ParabolicPoint → ℝ)
(hFm :
MeasureTheory.AEStronglyMeasurable F
(MeasureTheory.volume.restrict
(CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball (scale • Y) (scale * √(3 * δ / 2)))
(Set.Ioo (scale ^ 2 * δ / 2) (5 * scale ^ 2 * δ / 4)))))
:
∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball Y √(3 * δ / 2)) (Set.Ioo (1 / 2 + δ / 2) (1 / 2 + 5 * δ / 4)), F (buAffinePoint (-scale ^ 2 / 2) scale z) = scale⁻¹ ^ 5 * ∫ (z : CKN.Foundation.Parabolic.ParabolicPoint) in CKN.spaceTimeSet (CKN.Foundation.Parabolic.vec3Ball (scale • Y) (scale * √(3 * δ / 2)))
(Set.Ioo (scale ^ 2 * δ / 2) (5 * scale ^ 2 * δ / 4)), F z
The normalized short-time averaging integral equals the physical
integral times the inverse parabolic Jacobian (lem:bu-small-time).