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Stationary-state covariance identity for time-integrated observables

Statement

Let A be a unital complex C∗-algebra, and let (αt)t∈R be a group of ∗-automorphisms of A, so α0=id⁡A and αs+t=αs∘αt. Assume point-norm continuity: for each X∈A, the orbit map t↦αt(X) is norm-continuous. Let ϕ:A→C be a bounded linear functional with ϕ(I)=1, ϕ(X∗X)≥0 for every X∈A, and ϕ∘αt=ϕ for every t. For m≥1, take self-adjoint V1,…,Vm∈A with ϕ(Va)=0. For T>0, regard A as its underlying real Banach space with the same norm for these time integrals, and define the norm-Riemann integrals Xa,T=∫0Tαt(Va) dt, and for s≥0 define Gab(s)=12(Re⁡ϕ(Vaαs(Vb))+Re⁡ϕ(Vbαs(Va))). Then each Xa,T is self-adjoint and 12TRe⁡ϕ(Xa,TXb,T)=∫0T(1−sT)Gab(s) ds. The real symmetric matrix with entries on the left is positive semidefinite.

Facts & Assumptions

Given: The unital C∗-algebra, strongly continuous automorphism group, invariant state, self-adjoint centered observables, and T>0 in the Statement.

[F1]

C star algebra: A is complete, multiplication is bounded, and the involution is continuous.

[F2]

Riemann integration of continuous curves in a complete normed space, with the fundamental theorem of calculus and coefficient functionals: continuous curves in a complete normed real vector space have norm-Riemann integrals, with linearity, additive subdivision, bounded-functional interchange, and the norm estimate from Riemann sums; for these integrals, the complex algebra A is viewed as its underlying real Banach space.

Proof

technique · direct double integration over the time square, followed by stationarity and positivity

Given: [F1]–[F2], the bounded normalized positive functional, and the invariant group in the Statement.

1.1givenF1F2algebra

The functional is Hermitian: if H=H∗ then ϕ((I+rH)∗(I+rH))=1+2rϕ(H)+r2ϕ(H2) is real for every real r, so ϕ(H)∈R; decomposing X=(X+X∗)/2+i(X−X∗)/(2i) gives ϕ(X∗)=ϕ(X)‾. For each a, t↦αt(Va) is norm-continuous, so [F2] defines Xa,T. Riemann sums of self-adjoint elements are self-adjoint, and continuity of the involution in [F1] passes this property to the limit. The product map (s,t)↦αs(Va)αt(Vb) is norm-continuous on [0,T]2 by continuity of multiplication; approximating each integral by Riemann sums and multiplying the sums shows Xa,TXb,T equals the iterated integral of this product.

2.1givenF1F2step 1.1algebra

Invariance of ϕ and the group law give ϕ(αs(Va)αt(Vb))=ϕ(Vaαt−s(Vb)) for every s,t∈[0,T]. The scalar integrand is continuous; splitting the square into the triangles t≥s and s≥t, and integrating the slices with fixed u=∣t−s∣, whose lengths are T−u, yields ϕ(Xa,TXb,T)=∫0T(T−u)ϕ(Vaαu(Vb)) du+∫0T(T−u)ϕ(Vaα−u(Vb)) du. The diagonal has zero area and does not affect the Riemann integral. The slice formula follows from the one-variable substitution u=t−s on each triangle and the additivity of the Riemann integral.

3.1step 1.1step 2.1algebra

For u≥0, invariance gives ϕ(Vaα−u(Vb))=ϕ(αu(Va)Vb)=ϕ(Vbαu(Va))‾, where the last equality uses self-adjointness and step 1.1. Taking real parts in step 2.1 therefore gives the stated identity after dividing by 2T.

4.1givenstep 1.1algebra∎

For any real vector c=(c1,…,cm), Xc,T=∑acaXa,T is self-adjoint and ∑a,bcacbRe⁡ϕ(Xa,TXb,T)=ϕ(Xc,T2)=ϕ(Xc,T∗Xc,T)≥0 by positivity. Hermiticity from step 1.1 gives symmetry of the real matrix, so it is positive semidefinite.

Depends on

Dependency tree · 2 levels

Sources