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Bounded perturbations of the Heisenberg commutation relation via dilation theory

Malte Gerhold, Orr Shalit

TL;DR

The paper extends dilation distance to $d$-tuples of strongly continuous one-parameter unitary groups and proves that finite distance $d_{ m D}(u,v)$ yields equivalent representations on a common space with generators sharing domain and differing by a bounded perturbation. It establishes explicit norm bounds for the proximity of unitary-group realizations and their generators, linking dilation proximity to bounded perturbations of the associated self-adjoint generators. Applying this framework to Weyl canonical commutation relations, the authors recover Haagerup–Rordam's bounded-perturbation result and Gao's higher-dimensional generalization, with dimension-free constants. Using Weyl operators on symmetric Fock space, they derive a bound $ orm{P_k^ fty-Q_k} le frac{5}{ sqrt{2}} orm{ heta- heta'}^{1/2}$ for $ heta$-commuting unitary groups, highlighting dilation theory as a robust route to CCR perturbations and connecting to Stone–von Neumann phenomena.

Abstract

We extend the notion of dilation distance to strongly continuous one-parameter unitary groups. If the dilation distance between two such groups is finite, then these groups can be represented on the same space in such a way that their generators have the same domain and are in fact a bounded perturbation of one another. This result extends to d-tuples of one-parameter unitary groups. We apply our results to the Weyl canonical commutation relations, and as a special case we recover the result of Haagerup and Rordam that the infinite ampliation of the canonical position and momentum operators satisfying the Heisenberg commutation relation are a bounded perturbation of a pair of strongly commuting selfadjoint operators. We also recover Gao's higher-dimensional generalization of Haagerup and Rordam's result, and in typical cases we significantly improve control of the bound when the dimension grows.

Bounded perturbations of the Heisenberg commutation relation via dilation theory

TL;DR

The paper extends dilation distance to -tuples of strongly continuous one-parameter unitary groups and proves that finite distance yields equivalent representations on a common space with generators sharing domain and differing by a bounded perturbation. It establishes explicit norm bounds for the proximity of unitary-group realizations and their generators, linking dilation proximity to bounded perturbations of the associated self-adjoint generators. Applying this framework to Weyl canonical commutation relations, the authors recover Haagerup–Rordam's bounded-perturbation result and Gao's higher-dimensional generalization, with dimension-free constants. Using Weyl operators on symmetric Fock space, they derive a bound for -commuting unitary groups, highlighting dilation theory as a robust route to CCR perturbations and connecting to Stone–von Neumann phenomena.

Abstract

We extend the notion of dilation distance to strongly continuous one-parameter unitary groups. If the dilation distance between two such groups is finite, then these groups can be represented on the same space in such a way that their generators have the same domain and are in fact a bounded perturbation of one another. This result extends to d-tuples of one-parameter unitary groups. We apply our results to the Weyl canonical commutation relations, and as a special case we recover the result of Haagerup and Rordam that the infinite ampliation of the canonical position and momentum operators satisfying the Heisenberg commutation relation are a bounded perturbation of a pair of strongly commuting selfadjoint operators. We also recover Gao's higher-dimensional generalization of Haagerup and Rordam's result, and in typical cases we significantly improve control of the bound when the dimension grows.
Paper Structure (2 sections, 8 theorems, 39 equations)

This paper contains 2 sections, 8 theorems, 39 equations.

Key Result

Lemma 1.3

Let $U$ and $V$ be one-parameter unitary groups on the same Hilbert space $\mathcal{L}$, and let $C,D\in \mathbb R_+$. Then the following are equivalent.

Theorems & Definitions (20)

  • Definition 1.1
  • Definition 1.2
  • Lemma 1.3
  • proof
  • Theorem 1.4
  • proof
  • Lemma 1.5
  • proof
  • Lemma 1.6
  • proof
  • ...and 10 more