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Derivations on Operator Algebras

The infinitesimal generator of a continuous observable-algebra evolution is generally a closed, densely defined *-derivation. The continuity here is norm continuity of the orbit of each algebra element. We will prove density and closedness and identify the generator’s domain. Dynamics as Automorphisms explains the algebraic formulation, the corresponding state evolution, and the connection to equilibrium.

Helpful background. Operator Algebra Minimum introduces C*-algebras and their norm. Heisenberg Dynamics explains why conjugation by an unbounded Hamiltonian need not satisfy the point-norm condition on all of B(H)\mathcal B(\mathcal H).

The generator is an operator on the observable algebra

Section titled “The generator is an operator on the observable algebra”

Let A\mathcal A be a C*-algebra and α:R→Aut⁡(A)\alpha:\mathbb R\to\operatorname{Aut}(\mathcal A) a group satisfying

∥αt(A)−A∥⟶0(t→0),A∈A.\|\alpha_t(A)-A\|\longrightarrow0 \quad(t\to0),\qquad A\in\mathcal A.

Each automorphism is an isometry. Regard α\alpha as a strongly continuous group on the Banach space A\mathcal A and define

D(δ)={A∈A:lim⁡t→0αt(A)−At exists in norm},δ(A)=lim⁡t→0αt(A)−At.\begin{aligned} D(\delta)&=\left\{A\in\mathcal A: \lim_{t\to0}\frac{\alpha_t(A)-A}{t} \text{ exists in norm}\right\},\\ \delta(A)&=\lim_{t\to0}\frac{\alpha_t(A)-A}{t}. \end{aligned}

The generator domain is a *-subalgebra and

δ(AB)=δ(A)B+Aδ(B),δ(A∗)=δ(A)∗.\delta(AB)=\delta(A)B+A\delta(B),\qquad \delta(A^*)=\delta(A)^*.

These product and adjoint identities follow from the norm product rule, whose calculation is given in Dynamics as Automorphisms. They are the algebraic derivation property. The analytic assertions that D(δ)D(\delta) is dense and δ\delta is closed require additional arguments.

The group preserves the generator domain and satisfies

δ(αt(A))=αt(δ(A)),A∈D(δ),\delta(\alpha_t(A))=\alpha_t(\delta(A)), \qquad A\in D(\delta),

by applying the bounded map αt\alpha_t to the defining difference quotient.

Time averaging creates dense smooth elements

Section titled “Time averaging creates dense smooth elements”

For f∈Cc∞(R)f\in C_c^\infty(\mathbb R) and A∈AA\in\mathcal A, define the norm-convergent Bochner integral

Af=∫Rf(t)αt(A) dt.A_f=\int_{\mathbb R}f(t)\alpha_t(A)\,dt.

Changing variables gives

αs(Af)=∫Rf(t−s)αt(A) dt.\alpha_s(A_f)=\int_{\mathbb R}f(t-s)\alpha_t(A)\,dt.

Difference quotients of f(t−s)f(t-s) converge in L1L^1, so the norm derivative may be passed under the integral. Consequently

δ(Af)=−∫f′(t)αt(A) dt.\delta(A_f)=-\int f'(t)\alpha_t(A)\,dt.

Repeated differentiation shows Af∈D(δn)A_f\in D(\delta^n) for every nn, with

δn(Af)=(−1)n∫f(n)(t)αt(A) dt,∥δn(Af)∥≤∥f(n)∥1∥A∥.\delta^n(A_f)=(-1)^n\int f^{(n)}(t)\alpha_t(A)\,dt, \qquad \|\delta^n(A_f)\|\leq\|f^{(n)}\|_1\|A\|.

Now take a nonnegative smooth approximate identity fεf_\varepsilon with integral one and support shrinking to zero. Then

∥Afε−A∥≤∫fε(t)∥αt(A)−A∥ dt⟶0.\|A_{f_\varepsilon}-A\| \leq\int f_\varepsilon(t)\|\alpha_t(A)-A\|\,dt \longrightarrow0.

Thus infinitely differentiable elements are dense, and in particular D(δ)D(\delta) is dense. Smoothness should not be confused with analyticity: these estimates do not automatically make the formal series ∑tnδn(A)/n!\sum t^n\delta^n(A)/n! converge.

For A∈D(δ)A\in D(\delta), integration of the norm derivative yields

αt(A)−A=∫0tαs(δ(A)) ds.\alpha_t(A)-A=\int_0^t\alpha_s(\delta(A))\,ds.

Suppose An∈D(δ)A_n\in D(\delta), An→AA_n\to A, and δ(An)→B\delta(A_n)\to B in norm. Isometry of the group permits passage to the limit on both sides:

αt(A)−A=∫0tαs(B) ds.\alpha_t(A)-A=\int_0^t\alpha_s(B)\,ds.

Dividing by tt and taking t→0t\to0 gives BB, by point-norm continuity of the orbit of BB. Therefore A∈D(δ)A\in D(\delta) and δ(A)=B\delta(A)=B. This is precisely closedness of the graph.

The proof also shows why topology is part of the theorem. Replacing norm convergence by strong operator convergence without changing the domain and conclusion would be a different assertion.

If A\mathcal A is unital and K=K∗∈AK=K^*\in\mathcal A, then

αt(A)=eitK/ℏAe−itK/ℏ\alpha_t(A)=e^{itK/\hbar}Ae^{-itK/\hbar}

has the everywhere-defined bounded generator δ(A)=(i/ℏ)[K,A]\delta(A)=(i/\hbar)[K,A], with norm at most 2∥K∥/ℏ2\|K\|/\hbar. The derivation is inner because its implementing element belongs to the algebra.

An instructive contrasting example is rotation of continuous functions on the circle:

A=C(T),(αtf)(θ)=f(θ+t).\mathcal A=C(\mathbb T),\qquad (\alpha_t f)(\theta)=f(\theta+t).

Compactness of the circle makes each continuous function uniformly continuous, so this is point-norm continuous. Its generator has domain C1(T)C^1(\mathbb T) and is δf=f′\delta f=f'. The functions fn(θ)=einθf_n(\theta)=e^{in\theta} have norm one and derivative norm ∣n∣|n|, proving unboundedness.

This derivation cannot be an internal commutator: the algebra is commutative, so every such commutator vanishes. It can nevertheless be implemented in a Hilbert-space representation by a unitary translation group with an unbounded generator. Innerness in a chosen algebra and unitary implementability in a representation are distinct questions.

Conversely, writing a formal Leibniz rule does not prove that a proposed derivation generates an automorphism group. A generation theorem requires analytic hypotheses, including the appropriate domain and resolvent control. The present argument begins with an existing group and identifies its generator.

  1. Prove that the generator domain for rotations of C(T)C(\mathbb T) is exactly C1(T)C^1(\mathbb T).
Solution

For a continuously differentiable periodic function, uniform continuity of its derivative gives uniform convergence of translation difference quotients to f′f'. Conversely, if the quotients converge uniformly to gg, then gg is continuous and the integrated group identity gives f(θ+t)−f(θ)=∫0tg(θ+s) dsf(\theta+t)-f(\theta)=\int_0^t g(\theta+s)\,ds. Hence ff is continuously differentiable with derivative gg.

  1. For λ>0\lambda>0, show that the operator RλA=∫0∞e−λtαt(A) dtR_\lambda A=\int_0^\infty e^{-\lambda t}\alpha_t(A)\,dt has norm at most 1/λ1/\lambda and solves (λ−δ)RλA=A(\lambda-\delta)R_\lambda A=A.
Solution

Isometry gives the norm bound by integrating e−λte^{-\lambda t}. Changing variables in αh(RλA)\alpha_h(R_\lambda A) and taking the norm difference quotient gives δRλA=λRλA−A\delta R_\lambda A=\lambda R_\lambda A-A. Thus the integral takes values in D(δ)D(\delta) and is the resolvent of the Banach-space generator. Integration by parts gives the reverse inverse identity on D(δ)D(\delta).

  • O. Bratteli and D. W. Robinson, Operator Algebras and Quantum Statistical Mechanics 1, 2nd ed., Springer, 1987, Chapter 3, publisher edition — automorphism groups, smooth elements, and derivations.
  • A. Pazy, Semigroups of Linear Operators and Applications to Partial Differential Equations, Applied Mathematical Sciences 44, Springer, 1983, Chapter 1, publisher edition — closed densely defined generators and Laplace resolvents.