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Continuous Hilbert factorization of the spectral form

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QAlgorithms.Papers.Independent.Intakethird100.P38.hilbert_space_factorization

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.

Suppose σ∈C\sigma\in\mathcal Cσ∈C and the complex Hilbert space L2(σ)L^2(\sigma)L2(σ) is infinite dimensional. There exists a continuous complex-linear map Q:S→L2(Rn,dx)Q:\mathcal S\to L^2(\mathbb R^n,dx)Q:S→L2(Rn,dx) such that

⟨Qψ,Qφ⟩source=∫ψ^(u)φ^(u)‾ dσ(u),∥Qψ∥22=∫∣ψ^∣2 dσ.\langle Q\psi,Q\varphi\rangle_{\mathrm{source}}=\int\widehat\psi(u)\overline{\widehat\varphi(u)}\,d\sigma(u),\qquad\|Q\psi\|_2^2=\int|\widehat\psi|^2\,d\sigma.⟨Qψ,Qφ⟩source​=∫ψ​(u)φ​(u)​dσ(u),∥Qψ∥22​=∫∣ψ​∣2dσ.

This realizes the spectral form in Lebesgue L2L^2L2. The codomain follows the construction and proof, correcting the printed L2(σ)L^2(\sigma)L2(σ). Mathlib's conjugate-linear-first inner product reverses the displayed slots.

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

/-- Theorem 3.4, PDF pp.9--10. SOURCE CORRECTION: the theorem and (3.6) print
L2(σ); (3.7), §1(b), and every norm in the proof use L2(dx), used here.
The explicit infinite-dimensional assumption is retained. -/
theorem hilbert_space_factorization (n : ℕ) (hn : 0 < n)
    (σ : Measure (SpectralDomain n)) (hσ : InC σ) (hinfinite : ¬ FiniteDimensional ℂ (L2 σ)) :
    ∃ Q : ComplexTest n →L[ℂ] L2 (volume : Measure (SpectralDomain n)),
      HilbertFactor σ Q ∧ ∀ ψ : ComplexTest n,
        fourierEnergy σ ψ = ENNReal.ofReal (‖Q ψ‖ ^ 2) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P38

end
Source
Stochastic processes induced by singular operators, arXiv:1109.5273v1, PDF p. 9, Theorem 3.4: Hilbert-space factorization
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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 regular measure σ\sigmaσ on Rn\mathbb R^nRn satisfying ∫(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, assume additionally that the complex Hilbert space L2(σ;C)L^2(\sigma;\mathbb C)L2(σ;C) is not finite-dimensional. Then there exists a continuous complex-linear map QQQ from the complex-valued Schwartz functions on Rn\mathbb R^nRn to L2(dx;C)L^2(dx;\mathbb C)L2(dx;C) such that, for every pair ψ,ϕ\psi,\phiψ,ϕ of such functions,

⟨Qϕ,Qψ⟩C=∫Rnψ^(u) ϕ^(u)‾ dσ(u),\langle Q\phi,Q\psi\rangle_{\mathbb C} =\int_{\mathbb R^n}\widehat\psi(u)\, \overline{\widehat\phi(u)}\,d\sigma(u),⟨Qϕ,Qψ⟩C​=∫Rn​ψ​(u)ϕ​(u)​dσ(u),

and, for every such ψ\psiψ,

∫Rn∣ψ^(u)∣2 dσ(u)=ofReal⁡ ⁣(∥Qψ∥22).\int_{\mathbb R^n}|\widehat\psi(u)|^2\,d\sigma(u) =\operatorname{ofReal}\!\left(\|Q\psi\|_2^2\right).∫Rn​∣ψ​(u)∣2dσ(u)=ofReal(∥Qψ∥22​).

Here dxdxdx is Euclidean volume measure, 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⁡\operatorname{ofReal}ofReal embeds the nonnegative real squared norm into the extended nonnegative reals. The complex pairing integral uses the total Bochner integral, which is 000 when its integrand is not integrable.

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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