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MIPRE.Background.Repetition.CommutingRepetition.VN.JointModulus

Eₓ ∈ R(M)′ commutes with J E_y J.

The joint spectral measure of (Eₓ, J E_y J) at the trace vector.

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    theorem CommutingRepetition.GraphMod.νxy_prod (M : StdTracialAlgebra) (x y : M.H) {K K' : Set } (hK : MeasurableSet K) (hK' : MeasurableSet K') :
    ((νxy M x y) (K ×ˢ K')).toReal = inner M.traceVector ((BorelCalc.P (Eop M x) K) ((BorelCalc.P (Eop M y) K') M.traceVector))

    Rectangle masses: ν_{x,y}(K × K') = ⟪Ω, 1_K(Eₓ) 1_{K'}(E_y) Ω⟫.

    theorem CommutingRepetition.GraphMod.integral_νxy_mul (M : StdTracialAlgebra) (x y : M.H) {g h : } (hg : BorelCalc.Bdd g) (hh : BorelCalc.Bdd h) :
    (p : × ), g p.1 * h p.2 νxy M x y = (inner ((BorelCalc.bfc (Eop M x) g) M.traceVector) ((BorelCalc.bfc (Eop M y) h) M.traceVector)).re

    The product formula at the trace vector, for bounded Borel g, h: ∫ g(s) h(t) dν_{x,y} = re ⟪g(Eₓ) Ω, h(E_y) Ω⟫.

    The coupling of the modulus distributions #

    The joint coupling ν_{x,y} = (ψ × ψ)_* ν_{Eₓ, JE_yJ; Ω} of μₓ and μ_y.

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      theorem CommutingRepetition.GraphMod.cross (M : StdTracialAlgebra) (x y : M.H) {I J : Set } (hI : MeasurableSet I) (hJ : MeasurableSet J) :
      M.vnModel.τ (projx M x I * projx M y J) = ((νψ M x y) (I ×ˢ J)).toReal

      The rectangle identity in the form consumed by JointSpectralData.cross.

      The cross moment #

      theorem CommutingRepetition.GraphMod.integral_ψ_mul (M : StdTracialAlgebra) (x y : M.H) :
      (p : × ), ψ p.1 * ψ p.2 νxy M x y = (inner (hvec M x) (hvec M y)).re

      The cross term: ∫ ψ(s) ψ(t) dν_{x,y} = re ⟪hvec x, hvec y⟫.

      theorem CommutingRepetition.GraphMod.crossMoment (M : StdTracialAlgebra) (x y : M.H) :
      (p : × ), (p.1 - p.2) ^ 2 νψ M x y = hvec M x - hvec M y ^ 2

      The cross moment: ∫ (s − t)² dν_{x,y}(s, t) = ‖hvec x − hvec y‖².