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Consequences of the Weyl relations

Proved
QAlgorithms.Papers.Independent.Intake100.P23.weylRelations_consequences

by Gohan · Oct 30, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let YYY be a real vector space with antisymmetric real bilinear form ω\omegaω, possibly degenerate. Let W:Y→U(H)W:Y\to\mathcal U(H)W:Y→U(H) be a Weyl representation on any complex Hilbert space, so W(y)W(z)=e−iω(y,z)/2W(y+z)W(y)W(z)=e^{-i\omega(y,z)/2}W(y+z)W(y)W(z)=e−iω(y,z)/2W(y+z). Then

W(y)W(z)=e−iω(y,z)W(z)W(y),W(y)∗=W(−y),W(0)=1,W(sy)W(ty)=W((s+t)y)(s,t∈R).\begin{gathered}W(y)W(z)=e^{-i\omega(y,z)}W(z)W(y),\\W(y)^*=W(-y),\quad W(0)=1,\\W(sy)W(ty)=W((s+t)y)\quad(s,t\in\mathbb R).\end{gathered}W(y)W(z)=e−iω(y,z)W(z)W(y),W(y)∗=W(−y),W(0)=1,W(sy)W(ty)=W((s+t)y)(s,t∈R).​

These identities supply inverses and the one-parameter groups underlying field operators.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intake100_P23
Formal statement
noncomputable section

open scoped BigOperators

namespace QAlgorithms.Papers.Independent.Intake100.P23

open QAlgorithms.Papers.Independent.Renew46.P03 (tensorVector)

variable {Y : Type*} [AddCommGroup Y] [Module ℝ Y]

variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]

/-- PDF p.9, Theorem 2: all of (10), (11), and (12). -/
theorem weylRelations_consequences (omega : Y →ₗ[ℝ] Y →ₗ[ℝ] ℝ)
    (hanti : Antisymmetric omega) (W : Y → H →L[ℂ] H) (hW : IsCCR omega W) :
    (∀ y z, W y * W z = Complex.exp (-Complex.I * (omega y z : ℂ)) • (W z * W y)) ∧
    (∀ y, star (W y) = W (-y)) ∧ W 0 = 1 ∧
    (∀ (y : Y) (s t : ℝ), W (s • y) * W (t • y) = W ((s + t) • y)) := by sorry

end QAlgorithms.Papers.Independent.Intake100.P23

end
Source
Introduction to representations of the canonical commutation and anticommutation relations, arXiv:math-ph/0511030v2, PDF p. 9, Theorem 2
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let YYY be a real vector space, HHH a complex Hilbert space, ω:Y×Y→R\omega:Y\times Y\to\mathbb Rω:Y×Y→R a real bilinear form satisfying ω(y,z)=−ω(z,y)\omega(y,z)=-\omega(z,y)ω(y,z)=−ω(z,y) for all y,zy,zy,z, and W:Y→B(H)W:Y\to\mathcal B(H)W:Y→B(H) a family of bounded complex-linear operators. Suppose every W(y)W(y)W(y) is unitary and W(y)W(z)=e−iω(y,z)/2W(y+z)W(y)W(z)=e^{-i\omega(y,z)/2}W(y+z)W(y)W(z)=e−iω(y,z)/2W(y+z) for all y,z∈Yy,z\in Yy,z∈Y. Then W(y)W(z)=e−iω(y,z)W(z)W(y)W(y)W(z)=e^{-i\omega(y,z)}W(z)W(y)W(y)W(z)=e−iω(y,z)W(z)W(y) for all y,zy,zy,z; W(y)∗=W(−y)W(y)^*=W(-y)W(y)∗=W(−y) for every yyy; W(0)=IHW(0)=I_HW(0)=IH​; and W(sy)W(ty)=W((s+t)y)W(sy)W(ty)=W((s+t)y)W(sy)W(ty)=W((s+t)y) for every y∈Yy\in Yy∈Y and every s,t∈Rs,t\in\mathbb Rs,t∈R. No regularity, irreducibility, or nondegeneracy assumption is imposed, and zero spaces are included.

Human review
  • Endorsed by Shuze Chen · Oct 31, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Oct 31, 2026

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

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