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Variation of constants for a finite-matrix action defect

Statement

Let n≥1, A∈Mn(C), T>0, v∈Cn, and u:[−T,T]→Cn be continuously differentiable, with one-sided derivatives at the endpoints. Define the continuous defect r(s):=Au(s)−u′(s). Then, for every t∈[−T,T],

etAv−u(t)=etA(v−u(0))+∫0te(t−s)Ar(s) ds.

The vector integral is the oriented componentwise Riemann integral after identifying Cn with R2n. In particular, if u(0)=v, the initial term vanishes.

Facts & Assumptions

Given: n≥1, a complex square matrix A, T>0, a vector v, and a continuously differentiable curve u:[−T,T]→Cn with defect r(s)=Au(s)−u′(s).

[F1]

The exponential series of a bounded operator: for a bounded operator A, E(t):=etA is differentiable, E′(t)=AE(t)=E(t)A, and E(t)E(s)=E(t+s).

[F2]

The derivative and the Riemann integral of a vector-valued function: an intrinsic derivative and a componentwise integral: derivatives and integrals of finite-dimensional real vector-valued curves are taken componentwise.

[F3]

If f:[a,b]→Rm is differentiable with integrable f′ then ∫abf′=f(b)−f(a); and a bounded derivative makes f Lipschitz: if a real vector-valued curve is differentiable on a compact interval and its derivative is integrable, the integral of the derivative equals the endpoint difference.

[F4]

C is the real coordinate plane, with coordinate arithmetic and The standard formulas ⟨x,y⟩=∑k<nxkyk on Rn and ∑k<nxkyk‾ on Cn are inner products: real and imaginary coordinates identify Cn with a finite-dimensional real vector space, and the standard inner product is given coordinatewise.

[F5]

Every finite-dimensional normed space is Banach: the finite-dimensional complex-inner-product space Cn is complete.

[F6]

The operator norm is zero on the zero domain and otherwise is max_{||v||=1} ||Tv||: for a linear map between finite-dimensional inner-product spaces, its operator norm is the maximum of ∥Ax∥2 over unit vectors.

[F7]

A continuous function on [a,b] is Riemann integrable, by Heine-Cantor and Riemann's criterion: every continuous real-valued function on a nondegenerate closed bounded interval is Riemann integrable.

Proof

technique · direct
1.1givenF1F5F6algebra

Set x(t):=etAv−u(t). If y≠0, rescaling y/∥y∥2 in [F6] gives ∥Ay∥2≤∥A∥2∥y∥2, while the same inequality is immediate for y=0; thus A is bounded. By [F1] and [F5], the exponential series applies on the complete space Cn. It gives x′(t)=AetAv−u′(t)=A(x(t)+u(t))−u′(t)=Ax(t)+r(t), and x(0)=v−u(0).

2.1step 1.1F1algebra

Define g(t):=e−tAx(t). Differentiating the product and using that A commutes with every power in its exponential series gives g′(t)=−Ae−tAx(t)+e−tA(Ax(t)+r(t))=e−tAr(t).

3.1step 2.1F2F3F4F7

By [F2] and [F4], g is a real finite-dimensional vector-valued curve with continuous derivative. Each coordinate of g′ is continuous and therefore Riemann integrable on every nondegenerate closed subinterval by [F7]. If t=0, then g(t)=g(0) and the oriented integral is zero. If t>0, [F3] on [0,t] gives g(t)=g(0)+∫0te−sAr(s) ds. If t<0, [F3] on [t,0] gives g(0)−g(t)=∫t0e−sAr(s) ds, which is the same oriented identity after reversing the bounds.

4.1step 3.1F1F2algebra∎

Multiply this equality by etA. Matrix multiplication is a fixed finite-dimensional linear map and therefore commutes with the componentwise integral; [F1] gives etAg(t)=x(t), etAg(0)=etA(v−u(0)), and etAe−sA=e(t−s)A. Substitution yields the stated identity.

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