PhysLean Documentation

PhysLean.SpaceAndTime.Space.Distributions.ConstantTime

Distributions which are constant in time #

i. Overview #

in this module given a distribution on Space d, we define the associated distribution on Time × Space d which is constant in time.

This is defined by integrating Schwartz Maps on Time × Space d over the time coordinate, to get a Schwartz Map on Space d.

ii. Key results #

iii. Table of contents #

iv. References #

A. Properties of time integrals of Schwartz maps #

A.1. Continuity as a function of space #

theorem Space.continuous_time_integral {d : } (η : SchwartzMap (Time × Space d) ) :
Continuous fun (x : Space d) => (t : Time), η (t, x)

A.2. Derivative a function of space #

theorem Space.time_integral_hasFDerivAt {d : } (η : SchwartzMap (Time × Space d.succ) ) (x₀ : Space d.succ) :
HasFDerivAt (fun (x : Space d.succ) => (t : Time), η (t, x)) ( (t : Time), fderiv (fun (x : Space d.succ) => η (t, x)) x₀) x₀

A.3. Differentiability as a function of space #

A.4. Integrability of the derivative as a function of space #

A.5. Smoothness as a function of space #

theorem Space.time_integral_contDiff {d : } (n : ) (η : SchwartzMap (Time × Space d.succ) ) :
ContDiff n fun (x : Space d.succ) => (t : Time), η (t, x)

B. Properties of schwartz maps at a constant space point #

B.1. Integrability #

B.2. Integrability of powers times norm of iterated derivatives #

B.2.1. Bounds on powers times norm of iterated derivatives #

theorem Space.pow_mul_iteratedFDeriv_norm_le {n m d : } :
∃ (rt : ), ∀ (η : SchwartzMap (Time × Space d.succ) ) (x : Space d.succ), MeasureTheory.Integrable (fun (x : Time) => ((1 + x) ^ rt)⁻¹) MeasureTheory.volume ∀ (t : Time), (t, x) ^ m * iteratedFDeriv n η (t, x) 2 ^ (rt + m, n).1 * ((Finset.Iic (rt + m, n)).sup fun (m : × ) => SchwartzMap.seminorm m.1 m.2) η * (1 + t) ^ rt⁻¹

B.2.2. Integrability of powers times norm of iterated derivatives #

B.3. Integrability of iterated derivatives #

C. Decay results for derivatives of the time integral #

C.1. Moving the iterated derivative inside the time integral #

theorem Space.time_integral_iteratedFDeriv_apply {d : } (n : ) (η : SchwartzMap (Time × Space d.succ) ) (x : Space d.succ) (y : Fin nSpace d.succ) :
(iteratedFDeriv n (fun (x : Space d.succ) => (t : Time), η (t, x)) x) y = (t : Time), (iteratedFDeriv n η (t, x)) fun (i : Fin n) => (0, y i)

C.2. Bound on the norm of iterated derivative #

C.3. Bound on the norm of iterated derivative mul a power #

D. The time integral as a schwartz map #

The continuous linear map taking Schwartz maps on Time × Space d to space d by integrating over time.

Equations
Instances For

    E. Constant time distributions #

    Distributions on Time × Space d from distributions on Space d. These distributions are constant in time.

    Equations
    Instances For

      E.1. Space derivatives of constant time distributions #

      E.2. Space gradient of constant time distributions #

      E.3. Space divergence of constant time distributions #

      E.4. Space curl of constant time distributions #

      E.5. Time derivative of constant time distributions #