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Translation invariance characterizes spectral quadratic forms

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QAlgorithms.Papers.Independent.Intakethird100.P38.translation_invariant_quadratic_iff

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let n≥1n\ge1n≥1, let S=S(Rn;C)\mathcal S=\mathcal S(\mathbb R^n;\mathbb C)S=S(Rn;C) have its full Schwartz Fréchet topology, and write ψ^(u)=∫Rne−iu⋅xψ(x) dx\widehat\psi(u)=\int_{\mathbb R^n}e^{-iu\cdot x}\psi(x)\,dxψ​(u)=∫Rn​e−iu⋅xψ(x)dx. Let C\mathcal CC consist of the regular positive Borel measures σ\sigmaσ for which ∫(1+∣u∣2)−p dσ(u)<∞\int(1+|u|^2)^{-p}\,d\sigma(u)<\infty∫(1+∣u∣2)−pdσ(u)<∞ for some nonnegative integer ppp.

Let q:S→Rq:\mathcal S\to\mathbb Rq:S→R be continuous, nonnegative, satisfy q(cψ)=∣c∣2q(ψ)q(c\psi)=|c|^2q(\psi)q(cψ)=∣c∣2q(ψ), and satisfy the parallelogram identity. Then

[∃σ∈C  ∀ψ∈S,q(ψ)=∫∣ψ^∣2 dσ]⟺[∀t∈Rn  ∀ψ∈S,q(ψ(⋅−t))=q(ψ)].\left[\exists\sigma\in\mathcal C\;\forall\psi\in\mathcal S,\quad q(\psi)=\int|\widehat\psi|^2\,d\sigma\right]\quad\Longleftrightarrow\quad\left[\forall t\in\mathbb R^n\;\forall\psi\in\mathcal S,\quad q(\psi(\cdot-t))=q(\psi)\right].[∃σ∈C∀ψ∈S,q(ψ)=∫∣ψ​∣2dσ]⟺[∀t∈Rn∀ψ∈S,q(ψ(⋅−t))=q(ψ)].

This characterizes precisely the continuous positive quadratic forms represented by spectral measures.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P38
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P38

open MeasureTheory Filter

open scoped Topology ComplexConjugate ENNReal

/-- Lemma 3.2, PDF pp.7--8: all translations t are universally quantified.
The complex quadratic axioms are those explicitly given on p.6. -/
theorem translation_invariant_quadratic_iff (n : ℕ) (hn : 0 < n)
    (q : ComplexTest n → ℝ) (hq : PositiveQuadratic q) (hc : Continuous q) :
    (∃ σ : Measure (SpectralDomain n), InC σ ∧
      ∀ ψ : ComplexTest n, fourierEnergy σ ψ = ENNReal.ofReal (q ψ)) ↔
    (∀ (t : SpectralDomain n) (ψ : ComplexTest n), q (testTranslation t ψ) = q ψ) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P38

end
Source
Stochastic processes induced by singular operators, arXiv:1109.5273v1, PDF p. 7, Lemma 3.2: translation-invariant continuous quadratic forms
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every natural number n>0n>0n>0 and every continuous function qqq from the complex-valued Schwartz functions on Rn\mathbb R^nRn to R\mathbb RR, assume that q(ψ)≥0q(\psi)\ge0q(ψ)≥0 for every ψ\psiψ, that q(cψ)=∣c∣2q(ψ)q(c\psi)=|c|^2q(\psi)q(cψ)=∣c∣2q(ψ) for every complex number ccc and every ψ\psiψ, and that

q(ψ+ϕ)+q(ψ−ϕ)=2(q(ψ)+q(ϕ))q(\psi+\phi)+q(\psi-\phi)=2\bigl(q(\psi)+q(\phi)\bigr)q(ψ+ϕ)+q(ψ−ϕ)=2(q(ψ)+q(ϕ))

for every ψ,ϕ\psi,\phiψ,ϕ. Then the following are equivalent: there exists a regular measure σ\sigmaσ on Rn\mathbb R^nRn with ∫(1+∥u∥2)−p dσ(u)<∞\int(1+\|u\|^2)^{-p}\,d\sigma(u)<\infty∫(1+∥u∥2)−pdσ(u)<∞ for some natural number ppp, possibly 000, such that, for every complex-valued Schwartz function ψ\psiψ,

∫Rn∣ψ^(u)∣2 dσ(u)=ofReal⁡(q(ψ));\int_{\mathbb R^n}\left|\widehat\psi(u)\right|^2\,d\sigma(u) =\operatorname{ofReal}(q(\psi));∫Rn​​ψ​(u)​2dσ(u)=ofReal(q(ψ));

and q(x↦ψ(x−t))=q(ψ)q(x\mapsto\psi(x-t))=q(\psi)q(x↦ψ(x−t))=q(ψ) for every t∈Rnt\in\mathbb R^nt∈Rn and every such ψ\psiψ. Here ψ^(u)=∫Rne−i⟨u,x⟩ψ(x) dx\widehat\psi(u)=\int_{\mathbb R^n}e^{-i\langle u,x\rangle}\psi(x)\,dxψ​(u)=∫Rn​e−i⟨u,x⟩ψ(x)dx, the energy integral is extended nonnegative, and ofReal⁡(r)\operatorname{ofReal}(r)ofReal(r) is the extended nonnegative value of max⁡(r,0)\max(r,0)max(r,0), which here equals q(ψ)q(\psi)q(ψ) because of the assumed nonnegativity.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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