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The Commutator of a Square-Integrable Vector with a Bounded Self-Adjoint Operator: Linearity, the Norm Bound, Vacuum Vectors and Dependence on the Law Only

The commutator of a vector of the standard form with a bounded self-adjoint operator is linear in the vector and bounded by twice the operator norm, reduces to the operator commutator on vacuum vectors, and the sum of squared commutator norms of a momentum tuple with a bounded position tuple depends only on their joint law.

Statement

In the setting of Tracial W*-Probability Spaces and Square-Integrable Tuples: Standing Notation, tracial W*-probability spaces (H,M,Ω)(H,M,\Omega) and (K,N,Ψ)(K,N,\Psi) and the conjugation JJ of (H,M,Ω)(H,M,\Omega) are those of Tracial W*-Probability Spaces and Square-Integrable Tuples: Standing Notation §spaces, and self-adjoint tuples ss in MM, their vacuum tuples sΩs\Omega, L2L^{2} tuples, pairs (X,Y)(X,Y) and laws law(X,Y)\mathrm{law}(X,Y) are those of Tracial W*-Probability Spaces and Square-Integrable Tuples: Standing Notation §tuples; JNJ_{N} is the conjugation of (K,N,Ψ)(K,N,\Psi), and ∥⋅∥op\lVert\cdot\rVert_{\mathrm{op}} is the operator norm; norms of vectors are those of HH or of KK.

1. (Commutator) For a self-adjoint a∈Ma\in M and ζ∈H\zeta\in H we write

[ζ,a]=JaJζ−aζ∈H,[\zeta,a]=JaJ\zeta-a\zeta\in H,

and likewise [ζ′,b]=JNbJNζ′−bζ′∈K[\zeta',b]=J_{N}bJ_{N}\zeta'-b\zeta'\in K for a self-adjoint b∈Nb\in N and ζ′∈K\zeta'\in K.

2. (Linearity) For every self-adjoint a∈Ma\in M, all ζ,η∈H\zeta,\eta\in H and every complex cc, [ζ+cη,a]=[ζ,a]+c[η,a][\zeta+c\eta,a]=[\zeta,a]+c[\eta,a].

3. (Bound) For every self-adjoint a∈Ma\in M and every ζ∈H\zeta\in H, ∥[ζ,a]∥≤2∥a∥op∥ζ∥\lVert[\zeta,a]\rVert\le2\lVert a\rVert_{\mathrm{op}}\lVert\zeta\rVert.

4. (Vacuum vectors) For every self-adjoint a∈Ma\in M and every b∈Mb\in M, [bΩ,a]=(ba−ab)Ω[b\Omega,a]=(ba-ab)\Omega.

5. (Dependence on the law) Let d∈Nd\in\mathbb{N}, let ss be a self-adjoint dd-tuple in MM and tt a self-adjoint dd-tuple in NN, and let PP be an L2L^{2} dd-tuple of (H,M,Ω)(H,M,\Omega) and QQ an L2L^{2} dd-tuple of (K,N,Ψ)(K,N,\Psi). The vacuum tuples sΩs\Omega and tΨt\Psi are L2L^{2} dd-tuples by Standard Form of a Tracial W*-Probability Space: the Commutation Theorem, Right-Bounded Vectors, Faithfulness and Self-Adjoint Vectors §self-adjoint, so (sΩ,P)(s\Omega,P) and (tΨ,Q)(t\Psi,Q) are L2L^{2} 2d2d-tuples. Assume law(sΩ,P)=law(tΨ,Q)\mathrm{law}(s\Omega,P)=\mathrm{law}(t\Psi,Q). Then

∑j=1d∥[Pj,sj]∥2=∑j=1d∥[Qj,tj]∥2.\sum_{j=1}^{d}\lVert[P_{j},s_{j}]\rVert^{2}=\sum_{j=1}^{d}\lVert[Q_{j},t_{j}]\rVert^{2}.

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