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Bochner variation of constants for real evolution

Statement

Let S(t,r) be the evolution of Global real evolution, cocycle and inverse and use the Bochner integration conventions of Continuous free convolution on a finite time interval. For every strongly measurable f with ∫0T∥f(s)∥ ds<∞, the oriented integral Frf(t)=∫rtS(t,s)f(s) ds exists in the real Banach space E, belongs to C([0,T];E), and has norm at most C0∥f∥1. The unique forced solution is u(t)=S(t,r)x+Frf(t), and it satisfies u(t)=W(t−r)x+∫rtW(t−s)(P(s)u(s)+f(s)) ds. The integral is the Bochner integral of Bochner-integrable function. The exchange of triangular time integrals follows from scalar Fubini's theorem for L¹ functions on a sigma-finite product and Bochner simple approximation as proved below. In particular a physical forcing −if contributes ∫rtS(t,s)(−if(s)) ds; real linearity alone does not identify this with −iFrf(t).

Facts & Assumptions

Given: The bounded jointly strongly continuous real evolution, the finite time interval, and L1(E) forcing.

Goal: Prove the forced formula, including integrability and the interchange used to verify its Volterra identity.

[F1]

Global real evolution, cocycle and inverse gives joint strong continuity, the Volterra equation, global uniqueness and ∥S(t,s)∥≤C0.

[F2]

Continuous free convolution on a finite time interval fixes the real Banach space, complete finite Lebesgue time measure, Countable Choice hypothesis, oriented indicator ar,t and free integral Dr, and supplies its grid-simple approximation construction. Bochner integrability means simple L1 approximation as in Bochner-integrable function; strongly measurable functions with integrable norm are Bochner integrable by Bochner integrability criterion. Under the inherited Countable Choice, Bochner dominated convergence theorem applies to norm-dominated, almost-everywhere convergent sequences. The general integral norm bound is Bochner integral norm inequality. Bounded real-linear maps commute with general Bochner integrals by Bounded linear maps commute with Bochner integration, applied to real Banach spaces.

[F3]

Scalar Fubini for L1 functions on the product of the two finite Lebesgue intervals is Fubini's theorem for L¹ functions on a sigma-finite product.

[F4]

Linearity of the Bochner integral supplies additivity, subtraction and real homogeneity for general Bochner integrals. Tonelli's theorem for nonnegative measurable functions on a sigma-finite product applies to nonnegative measurable norm errors on the finite time square, and to their sums using counting measure on N. The finite time measures are sigma-finite by [F2], as is counting measure.

Proof

Given: The bounded jointly strongly continuous real evolution, the finite time interval, and L1(E) forcing.

Goal: Prove the forced formula, including integrability and the interchange used to verify its Volterra identity.

1.1F1F2given

For each fixed vector z, (t,s)↦S(t,s)z is continuous on the compact square and thus admits uniformly convergent grid-simple approximations, just as in [F2]. Composing with a pointwise simple approximation to f(s) proves joint strong measurability of S(t,s)f(s). The bound C0∥f(s)∥ proves integrability on each time section. With the oriented indicator ar,t(s) from [F2], the integrands converge almost everywhere as tn→t by [F1] and are dominated by that bound. Bochner dominated convergence in [F2] proves continuity; its norm inequality gives the uniform C0∥f∥1 estimate.

1.2F2F3F4given

Here is the needed vector version of [F3]. For a strongly measurable kernel H on the square with integrable norm, [F2] and the Bochner definition give integrable finite-valued simple functions Hn with ∫∥Hn−H∥≤2−n. Each Hn has the form ∑jzj1Aj, so [F3] on each scalar indicator and real linearity in [F4] give equality of its two iterated vector integrals and its product integral. Its section-integral functions are strongly measurable, since they are finite sums of fixed vectors times measurable scalar section measures, each of which admits scalar simple approximations. By Tonelli in [F4], the sum of the norm errors has finite product integral; for almost every outer variable the corresponding inner L1 errors are summable, and the simple sections converge pointwise to H off an inner null set. Thus those sections of H are strongly measurable and have integrable norm, and [F2] makes their Bochner integrals exist. The norm inequality in [F2] shows convergence of the section integrals. Their norms are bounded by the integrable outer function ∫∥H∥+∑n∫∥Hn−H∥, where these integrals are over the inner variable; its integrability follows from [F3] and [F4]. Bochner dominated convergence in [F2] therefore passes the outer vector integrals to the limit. The product vector integrals also converge by the norm inequality and real linearity. Repeat with the variables reversed to obtain both orders; assigning zero on the exceptional outer sets does not change the integrals.

2.1F1F2F4step 1.1step 1.2

For r≤t, insert S(t,s)=W(t−s)+∫stW(t−ρ)P(ρ)S(ρ,s) dρ into Frf(t). The kernel on r≤s≤ρ≤t is strongly measurable by the same grid-simple argument and norm-continuity of P, with bound MKC0∥f(s)∥. Its product norm integral is at most MKC0T∥f∥1, so step 1.2 applies. Commuting the bounded real-linear map W(t−ρ)P(ρ) with the inner integral by [F2], and using real linearity in [F4], gives Frf(t)=Drf(t)+∫rtW(t−ρ)P(ρ)Frf(ρ) dρ. For t<r, write both oriented integrals with minus signs: the double integral has two minus signs and region t≤ρ≤s≤r. Reversing that region gives exactly the same displayed oriented identity; its absolute majorant is unchanged.

3.1F1F2F4step 1.1step 2.1∎

By real linearity in [F4], add the unforced Volterra equation for S(t,r)x to the identity in step 2.1. The sum satisfies the forced Volterra equation and the correct value x at r. Global uniqueness from [F1] identifies it with the solution there. The norm estimate follows from step 1.1 and the homogeneous bound in [F1]. Since all bounded maps were used as real-linear maps, none of the integral identities permits moving a complex scalar through S. This proves the final forcing assertion and completes the proof.

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