Whole-cycle quantum time reversal
OpenQAlgorithms.Papers.Independent.Intakethird100.P15.wholeCycle_timeReversalLet be a nonzero complex Hilbert space with a nonempty finite or countable complete orthonormal basis real in a fixed conjugation. The self-adjoint Hamiltonian is real in that conjugation, periodic with period , and satisfies . Start at this symmetry origin and observe an integer number of full cycles. Let be the well-defined unitary strong limit of the chronological infinitesimal slice products, with each slice equal to and .
For every finite slicing at the symmetry origin, and for its unitary strong limit, the adjoint equals entrywise conjugation in the fixed real basis:
Explicitly, for all basis labels ; equivalently . The same coefficient identity holds for each finite chronological slice product.
This is the reversal identity underlying the fluctuation relations, derived from the real Hamiltonians and palindromic slicing.
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P15
namespace QAlgorithms.Papers.Independent.Intakethird100.P15
open MeasureTheory Filter
open QAlgorithms.Papers.Independent.Information100.P37 (transition)
open QAlgorithms.Papers.Independent.Support21.P03 (reflectedLaw)
open QAlgorithms.Papers.Independent.Next46.P01 (extendedExpectation)
open scoped ENNReal Topology
universe u v w
variable {E : Type u} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
variable {ι : Type v} {Ω : Type w} [MeasurableSpace Ω]
/-- Kurchan, PDF p.2, (3). Finite slice products and their well-defined unitary
strong limit have adjoint equal to entrywise conjugation in the fixed real basis.
The inverse of a unitary is its adjoint; scalar `star` is complex conjugation.
This derives reversal rather than including reversal in `CyclicDrive`. -/
theorem wholeCycle_timeReversal [Countable ι] [Nonempty ι]
(b : HilbertBasis ι ℂ E) (d : CyclicDrive (Ω := Ω) b) :
(∀ n i j,
inner ℂ (b i) ((chronologicalEvolution (List.ofFn (d.slices n))).symm (b j)) =
star (inner ℂ (b i) (chronologicalEvolution (List.ofFn (d.slices n)) (b j)))) ∧
(∀ i j, inner ℂ (b i) (d.evolution.symm (b j)) =
star (inner ℂ (b i) (d.evolution (b j)))) := by sorry
end QAlgorithms.Papers.Independent.Intakethird100.P15
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What the Lean code literally says, in plain math · gpt-6.1-sol
Let be a complex Hilbert space, a measurable space, and a Hilbert basis with countable and nonempty. The given cyclic drive consists of a period , a number , a cycle count , and, for every real , spectral data , where is a measure on , is measurable, and is a complex linear isometric bijection such that each is real almost everywhere. These entire spectral data satisfy and . For every there are surjective complex linear isometries , ; writing and , they satisfy, for all ,
The drive also supplies a surjective complex linear isometry such that for every , where . The theorem asserts
The cycle count is included.
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.