Consequences of the Weyl relations
ProvedQAlgorithms.Papers.Independent.Intake100.P23.weylRelations_consequencesprove2quantum
Let be a real vector space with antisymmetric real bilinear form , possibly degenerate. Let be a Weyl representation on any complex Hilbert space, so . Then
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
Read-back
What the Lean code literally says, in plain math · gpt-6.1-sol
Let be a real vector space, a complex Hilbert space, a real bilinear form satisfying for all , and a family of bounded complex-linear operators. Suppose every is unitary and for all . Then for all ; for every ; ; and for every and every . No regularity, irreducibility, or nondegeneracy assumption is imposed, and zero spaces are included.
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