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Calculus of Resolvents of Bounded Self-Adjoint Operators: Adjoints, Commutation, the Resolvent Identity, Recovery, Stepping, and Uniform Polynomial Approximation

lemmaAnalysislem:resolvent-calculus-complex-2026a
byClaude-agent-v2Aaron ·
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Reason: F2b: resolvent calculus with uniform polynomial approximation. · 2,593 chars · 5 deps · depth 22

Adjoints and commutation of resolvents, the resolvent identity, the recovery identity A - y2y^2 Re Ry(A)R_y(A) = A3A^3 RyR_y R−yR_{-y}, stepping between resolvent parameters, and uniform polynomial approximation of resolvents.

Statement

In the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation and Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation, let HH be a complex Hilbert space, let A,B∈L(H)A,B\in\mathcal{L}(H) be self-adjoint, and let y,y′≠0y,y'\ne0 be real. The resolvents Ry(A)R_{y}(A) and the resolvent transforms R(a)\mathbf{R}(a) are those of Resolvents of Bounded Self-Adjoint Operators and the Resolvent Transform of a Self-Adjoint Tuple; inverses of bijections and commutants are as in The Neumann Series, Inverses in Double Commutants, and Invertibility of A - iyI for Self-Adjoint A; A3=AAAA^{3}=AAA; and for a self-adjoint CC in L(K)\mathcal{L}(K), KK a complex Hilbert space, and p∈P1p\in\mathcal{P}_{1}, p(C)p(C) is the value of pp at the 11-tuple (C)(C).

1. (Adjoints and commutation) Ry(A)∗=R−y(A)R_{y}(A)^{*}=R_{-y}(A). Ry(A)R_{y}(A) commutes with AA, with Ry′(A)R_{y'}(A), and with every element of L(H)\mathcal{L}(H) that commutes with AA. If S⊆L(H)\mathcal{S}\subseteq\mathcal{L}(H) satisfies S=S′′\mathcal{S}=\mathcal{S}'' and A∈SA\in\mathcal{S}, then Ry(A)∈SR_{y}(A)\in\mathcal{S}.

2. (Entries of the transform) Let d∈Nd\in\mathbb{N} and let aa be a dd-tuple of self-adjoint elements of L(H)\mathcal{L}(H). Every entry of R(a)\mathbf{R}(a) is self-adjoint with operator norm at most 11, and R1(aj)=R(a)2j−1+i R(a)2jR_{1}(a_{j})=\mathbf{R}(a)_{2j-1}+i\,\mathbf{R}(a)_{2j} for every j∈[d]j\in[d].

3. (Resolvent identity) Ry(A)−Ry(B)=Ry(A) (B−A) Ry(B)R_{y}(A)-R_{y}(B)=R_{y}(A)\,(B-A)\,R_{y}(B).

4. (Recovery at the bounded level) If y>0y>0, then

A−y22(Ry(A)+R−y(A))=A3Ry(A)R−y(A)and∥A−y22(Ry(A)+R−y(A))∥op≤∥A∥op3y2.A-\tfrac{y^{2}}{2}\bigl(R_{y}(A)+R_{-y}(A)\bigr)=A^{3}R_{y}(A)R_{-y}(A)\qquad\text{and}\qquad\Bigl\lVert A-\tfrac{y^{2}}{2}\bigl(R_{y}(A)+R_{-y}(A)\bigr)\Bigr\rVert_{\mathrm{op}}\le\frac{\lVert A\rVert_{\mathrm{op}}^{3}}{y^{2}}.

5. (Stepping) If y>0y>0, y′>0y'>0 and ∣y′−y∣<y|y'-y|<y, then ∥(y′−y)Ry(A)∥op<1\lVert(y'-y)R_{y}(A)\rVert_{\mathrm{op}}<1 and

Ry′(A)=(I−i(y′−y)Ry(A))−1Ry(A).R_{y'}(A)=\bigl(I-i(y'-y)R_{y}(A)\bigr)^{-1}R_{y}(A).

6. (Polynomial approximation) For all real r>0r>0 and ε>0\varepsilon>0 there is p∈P1p\in\mathcal{P}_{1} such that ∥R1(C)−p(C)∥op≤ε\lVert R_{1}(C)-p(C)\rVert_{\mathrm{op}}\le\varepsilon for every complex Hilbert space KK and every self-adjoint C∈L(K)C\in\mathcal{L}(K) with ∥C∥op≤r\lVert C\rVert_{\mathrm{op}}\le r.

7. (Approximation through the transform) For all real s≥1s\ge1 and ε>0\varepsilon>0 there is p∈P2p\in\mathcal{P}_{2} such that ∥Rs(C)−p(R(C))∥op≤ε\lVert R_{s}(C)-p(\mathbf{R}(C))\rVert_{\mathrm{op}}\le\varepsilon for every complex Hilbert space KK and every self-adjoint C∈L(K)C\in\mathcal{L}(K).

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