OAI/Analysis/KadisonKastler/MatrixOrbitSampleLaw.lean
9 declarations, 0 contain sorry, 0 declared as axioms
Finite laws of the actual matrix-orbit samples
This converts the complex four-variable matrix-average identities to real moment identities for a single product-valued sample. It supplies the diagonal and the two off-diagonal inputs to the independent-sample fourth-moment estimate.
- abbrev
OAI.KadisonKastler.MatrixOrbitIndexline 24Source documentation
The actual finite sample space for one left and one right unitary.
abbrev MatrixOrbitIndex (d : ℕ) := SignedPermutation (Fin d) × SignedPermutation (Fin d)
Mentions: OAI.KadisonKastler.SignedPermutation
- def
OAI.KadisonKastler.matrixOrbitSampleline 27Source documentation
An operator sampled from the finite two-sided matrix orbit.
def matrixOrbitSample {d : ℕ} (E : Generator.MatrixUnitSystem (Fin d) (H →L[ℂ] H)) (x : H →L[ℂ] H) (g : MatrixOrbitIndex d) : H →L[ℂ] H := …Mentions: OAI.Generator.MatrixUnitSystem, OAI.KadisonKastler.MatrixOrbitIndex
- theorem
OAI.KadisonKastler.complex_expect_eq_averageline 33 - theorem
OAI.KadisonKastler.re_averageline 38 - theorem
OAI.KadisonKastler.expect_prodline 43 - theorem
OAI.KadisonKastler.state_conjline 48Distinct definitions of this name: OAI/Analysis/KadisonKastler/MatrixGraphMomentBounds.lean:55 (different declaration text). Qualify references as OAI.KadisonKastler.state_conj@path.
- theorem
OAI.KadisonKastler.matrixOrbit_diagonal_fourthline 63Source documentation
The fourth moment of a single orbit sample is unchanged by its two unitaries, since the right unitary belongs to the state's centralizer.
theorem matrixOrbit_diagonal_fourth (M : VonNeumannAlgebra H) (Ω : H) {d : ℕ} (E : Generator.MatrixUnitSystem (Fin d) (H →L[ℂ] H)) (hEM : E.algebra ≤ M.toStarSubalgebra) (hc : ∀ a ∈ E.algebra, ∀ z ∈ M, inner ℂ Ω ((a * z) Ω) = inner ℂ Ω ((z * a) Ω)) (x : H →L[ℂ] H) (hx : x ∈ M) (g : MatrixOrbitIndex d) : realVectorState Ω ((star (matrixOrbitSample E x g) * matrixOrbitSample E x g) ^ 2) = realVectorState Ω ((star x * x) ^ 2) := by …Mentions: OAI.Generator.MatrixUnitSystem, OAI.KadisonKastler.MatrixOrbitIndex, OAI.KadisonKastler.realVectorState, OAI.KadisonKastler.matrixOrbitSample
- theorem
OAI.KadisonKastler.matrixOrbit_first_pairing_expectline 86Source documentation
The first off-diagonal moment is the actual first independent-copy matrix pairing, expressed as a real number.
theorem matrixOrbit_first_pairing_expect (M : VonNeumannAlgebra H) (Ω : H) {d : ℕ} (E : Generator.MatrixUnitSystem (Fin d) (H →L[ℂ] H)) (hEM : E.algebra ≤ M.toStarSubalgebra) (hc : ∀ a ∈ E.algebra, ∀ z ∈ M, inner ℂ Ω ((a * z) Ω) = inner ℂ Ω ((z * a) Ω)) (x : H →L[ℂ] H) (hx : x ∈ M) : (𝔼 g : MatrixOrbitIndex d, 𝔼 h : MatrixOrbitIndex d, realVectorState Ω ((star (matrixOrbitSample E x g) * matrixOrbitSample E x g) * (star (matrixOrbitSample E x h) * matrixOrbitSample E x h))) = realVectorState Ω ((star x * x) * matrixUnitAverage E (star x * x)) := by …Mentions: OAI.Generator.MatrixUnitSystem, OAI.KadisonKastler.MatrixOrbitIndex, OAI.KadisonKastler.realVectorState, OAI.KadisonKastler.matrixOrbitSample, OAI.KadisonKastler.matrixUnitAverage
- theorem
OAI.KadisonKastler.matrixOrbit_third_pairing_expectline 115Source documentation
The positive mixed pairing similarly becomes one averaged left square between
x*andx.theorem matrixOrbit_third_pairing_expect (M : VonNeumannAlgebra H) (Ω : H) {d : ℕ} (E : Generator.MatrixUnitSystem (Fin d) (H →L[ℂ] H)) (hEM : E.algebra ≤ M.toStarSubalgebra) (hc : ∀ a ∈ E.algebra, ∀ z ∈ M, inner ℂ Ω ((a * z) Ω) = inner ℂ Ω ((z * a) Ω)) (x : H →L[ℂ] H) (hx : x ∈ M) : (𝔼 g : MatrixOrbitIndex d, 𝔼 h : MatrixOrbitIndex d, realVectorState Ω ((star (matrixOrbitSample E x g) * matrixOrbitSample E x h) * (star (matrixOrbitSample E x h) * matrixOrbitSample E x g))) = realVectorState Ω (star x * matrixUnitAverage E (x * star x) * x) := by …Mentions: OAI.Generator.MatrixUnitSystem, OAI.KadisonKastler.MatrixOrbitIndex, OAI.KadisonKastler.realVectorState, OAI.KadisonKastler.matrixOrbitSample, OAI.KadisonKastler.matrixUnitAverage