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Scalar Banach-function retarded estimates by Fatou approximation

Statement

Assume Countable Choice. Fix 0<T<∞. All scalar functions and vector spaces below are over C. Let (X,μ) be sigma-finite, choose An↑X of finite measure, and suppose the Hilbert space H is continuously and injectively realized as scalar classes in Lloc,A1(X): for each n its restriction Jn:H→L1(An) is bounded, the restrictions agree, and together they separate points of H. Let W be a strongly continuous unitary group on H.

Let Y be a Banach space of measurable scalar classes with these explicit properties: its norm is a lattice norm, meaning that ∣u∣≤∣v∣ almost everywhere and v∈Y imply u∈Y and ∥u∥Y≤∥v∥Y; for every n, ∫An∣y∣≤bn∥y∥Y; if yj→y almost everywhere, then ∥y∥Y≤lim inf⁡j∥yj∥Y, with norm infinity outside Y; for every jointly measurable scalar G(z,x), with time or time-pair parameter z, the extended norm z↦∥G(z,⋅)∥Y is measurable; and for jointly measurable scalar K(r,x) with ∫∥K(r,⋅)∥Y dr<∞, the spatial integral triangle property ∥∫K(r,⋅) dr∥Y≤∫∥K(r,⋅)∥Y dr holds. These are local-integrability, lattice, sequential Fatou, section-measurability and integral-triangle hypotheses; they do not assert Bochner measurability into Y. Local integrability and scalar Tonelli ensure that the scalar integral in this property actually exists almost everywhere.

Here scalar La spaces, including L1(An) and scalar time Lp, consist of almost-everywhere equivalence classes of measurable complex functions; for 1≤a<∞ their norm is (∫∣u∣a)1/a. The notation Lloc,A1(X) means measurable scalar classes whose restrictions belong to L1(An) for every n. In the forcing space L1(0,T;H), a representative is a strongly measurable function f:(0,T)→H, meaning a norm almost-everywhere limit of measurable H-valued simple functions, with ∫0T∥f(r)∥H dr<∞. Two such representatives define the same forcing class exactly when they agree in H for almost every r; its norm is ∥[f]∥Lt1H=∫0T∥f(r)∥H dr. Bochner integrability has its norm-limit-of-integrable-simple-functions meaning. The Bochner integrability criterion therefore supplies integrable simple approximants converging in this forcing norm. The norm and integral do not depend on the representative: the norm functions agree almost everywhere, and the Bochner norm inequality makes the integral of an almost-everywhere-zero difference zero.

For a jointly measurable scalar representative u(t,x), the scalar mixed norm is ∥u∥LtpY=(∫0T∥u(t,⋅)∥Yp dt)1/p, allowing the value infinity before membership is established; scalar representatives are identified almost everywhere on (0,T)×X. The notation CtH means C([0,T];H) with norm sup⁡0≤t≤T∥u(t)∥H.

Suppose 1≤p<∞ and the actual scalar orbits satisfy ∥W(⋅)h∥LtpY≤CT∥h∥H on (0,T), with the scalar mixed-norm convention. Then for every f∈L1(0,T;H) the continuous H-valued Bochner solution Df(t)=∫0tW(t−r)f(r) dr has a jointly measurable scalar representative and ∥Df∥CtH+∥Df∥LtpY≤(1+CT)∥f∥Lt1H.

Facts & Assumptions

[F1]

Unitarity and strong continuity have the meaning of Strongly continuous one-parameter unitary group. Bochner existence, simple L1 approximation, the norm bound and bounded-map interchange are Bochner integrability criterion, Bochner integral norm inequality and Bounded linear maps commute with Bochner integration.

[F3]

Scalar Fatou is Fatou's lemma. We use the sequential Fatou and local-integrability axioms of Y as actual hypotheses, and The Axiom of Countable Choice (AC_ω) for countable approximation choices.

[F4]

The Hilbert and Banach structures use Hilbert space and Banach space, over the common complex scalar field specified in the Statement. Scalar spaces use the almost-everywhere quotient convention of The space Lᵖ(μ) as the quotient by null functions.

[F5]

Strong measurability and Bochner integrability are Strongly measurable Banach-valued function and Bochner-integrable function. The forcing quotient and norm are defined inline in the Statement. By Bochner integrability criterion, every forcing representative is Bochner integrable and has integrable simple approximants converging in that norm; Bochner integral norm inequality makes its integral invariant under changes on time-null sets.

Proof

Given: The scalar local realizations of H, the declared Banach-function-space axioms, the homogeneous mixed estimate and L1(H) forcing. A mixed norm here is the scalar Lp norm of the section norms.

Goal: Identify the scalar limit with the continuous H solution and prove its mixed estimate without a nonseparable Bochner integration claim.

1.1F1F2F3F4F5given

By the forcing convention and [F5], choose a strongly measurable representative of f, with integrable norm and integrable simple approximants. All integrals below are independent of this choice by [F5]. The function W(−r)f(r) is strongly measurable by pointwise simple approximation of f and continuous orbit approximation for each of its finitely many values. It has integrable norm ∥f(r)∥H. Thus G(t)=∫0tW(−r)f(r) dr is continuous, since increments have norm bounded by the integral of ∥f∥H over the increment interval. The function Df(t)=W(t)G(t) is continuous and has CtH norm at most ∥f∥1. A continuous H path has a jointly measurable scalar representative: approximate it uniformly in H by finite interval-step paths, restrict using each bounded Jn, and pass to a common almost-everywhere limit on the countable product exhaustion. To justify that last passage choose errors summable in the uniform H norm; their product L1 errors on each An are summable, so Tonelli gives almost-everywhere convergence there. The limits agree on overlaps and represent the path in local L1 for almost every time. This construction also supplies measurable orbit representatives with Borel time parameter, allowing the shifts t−r.

1.2F1F2given

For a simple forcing f(r)=∑j=1N1Ej(r)hj, use those representatives to form the measurable kernel K(r,t,x)=10<r<t<TW(t−r)f(r)(x). On each finite spatial piece, its absolute triple integral is finite: ∥JnW(t−r)hj∥L1(An)≤∥Jn∥∥hj∥H by unitarity. Scalar Fubini and bounded-map interchange show that ∫0tK(r,t,x) dr is the local scalar representative of the H integral for almost every (t,x). The Y integral-triangle property and then time Minkowski give ∥Df∥LtpY≤∫0T∥1t>rW(t−r)f(r)∥LtpY dr≤CT∥f∥Lt1H. The last inequality is the original homogeneous bound restricted after the translation τ=t−r to (0,T−r); the section norms and all scalar integrals here are measurable by the stated axioms and [F2].

2.1F1F2F3F5step 1.1step 1.2

Using [F5] and Countable Choice, choose integrable simple fj→f with ∥fj−f∥L1(H)≤2−j. Step 1.1 gives uniform H convergence Dfj→Df, hence product L1((0,T)×An) convergence with summable errors for every n. Use the measurable representative of Df constructed there; Tonelli applied to the error series shows Dfj(t,x)→Df(t,x) outside a single product-null set in the countable exhaustion. Fubini then gives spatial almost-everywhere convergence for almost every t. The sequential Fatou hypothesis yields ∥Df(t)∥Y≤lim inf⁡j∥Dfj(t)∥Y, and scalar Fatou applied to the pth powers proves ∥Df∥LtpY≤lim inf⁡j∥Dfj∥LtpY≤CT∥f∥1.

3.1F1F2F3step 1.1step 2.1∎

For completeness, the assumed spatial integral property has a well-defined left side: local-integrability bounds give ∫∫An∣K(r,x)∣ dμ dr≤bn∫∥K(r,⋅)∥Y dr<∞, so Tonelli implies absolute scalar integrability for almost every x on every An. The mixed-norm limit has already been identified with the actual H solution in step 2.1, rather than postulated. Combining that estimate with step 1.1 proves the asserted sum estimate.

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