OAI/Analysis/KadisonSimilarity/FreeProduct/CommonFieldCompression.lean
4 declarations, 0 contain sorry, 0 declared as axioms
Compressing an actual measurable field in the common spectral model returns an operator in the original abelian commutant.
- def
OAI.KadisonSimilarity.commonFieldCompressionline 22Source documentation
The original operator obtained by compressing the reconstructed field.
def commonFieldCompression (R : WeakDual.characterSpace ℂ A → ScalarHilbertCoordinates D.generators →L[ℂ] ScalarHilbertCoordinates D.generators) (hmeas : ∀ v, AEStronglyMeasurable (fun x => R x v) (cyclicCommonBaseMeasure π D)) (C : ℝ) (hbound : ∀ᵐ x ∂cyclicCommonBaseMeasure π D, ‖R x‖ ≤ C) : H →L[ℂ] H := …Mentions: OAI.KadisonSimilarity.ScalarHilbertCoordinates, OAI.KadisonSimilarity.cyclicCommonBaseMeasure
- theorem
OAI.KadisonSimilarity.commonFieldCompression_eqline 32Source documentation
Expose the compression formula without unfolding its field operator.
theorem commonFieldCompression_eq (R : WeakDual.characterSpace ℂ A → ScalarHilbertCoordinates D.generators →L[ℂ] ScalarHilbertCoordinates D.generators) (hmeas : ∀ v, AEStronglyMeasurable (fun x => R x v) (cyclicCommonBaseMeasure π D)) (C : ℝ) (hbound : ∀ᵐ x ∂cyclicCommonBaseMeasure π D, ‖R x‖ ≤ C) : commonFieldCompression π D R hmeas C hbound = ((cyclicCommonEmbedding π D).toContinuousLinearMap.adjoint.comp (boundedFieldOperator (cyclicCommonBaseMeasure π D) R hmeas C hbound)).comp (cyclicCommonEmbedding π D).toContinuousLinearMap := rflMentions: OAI.KadisonSimilarity.ScalarHilbertCoordinates, OAI.KadisonSimilarity.cyclicCommonBaseMeasure, OAI.KadisonSimilarity.commonFieldCompression, OAI.KadisonSimilarity.cyclicCommonEmbedding, OAI.KadisonSimilarity.boundedFieldOperator
- theorem
OAI.KadisonSimilarity.commonFieldCompression_memline 42 - theorem
OAI.KadisonSimilarity.commonFieldCompression_mem_of_range_eqline 59Source documentation
The same compression belongs to any representation generating this commutant.
theorem commonFieldCompression_mem_of_range_eq {B : Type*} [CStarAlgebra B] (σ : B →⋆ₐ[ℂ] (H →L[ℂ] H)) (hgen : representationVonNeumannAlgebra σ = starSubalgebraCommutant π.range) (R : WeakDual.characterSpace ℂ A → ScalarHilbertCoordinates D.generators →L[ℂ] ScalarHilbertCoordinates D.generators) (hmeas : ∀ v, AEStronglyMeasurable (fun x => R x v) (cyclicCommonBaseMeasure π D)) (C : ℝ) (hbound : ∀ᵐ x ∂cyclicCommonBaseMeasure π D, ‖R x‖ ≤ C) : ((cyclicCommonEmbedding π D).toContinuousLinearMap.adjoint.comp (boundedFieldOperator (cyclicCommonBaseMeasure π D) R hmeas C hbound)).comp (cyclicCommonEmbedding π D).toContinuousLinearMap ∈ representationVonNeumannAlgebra σ := by …Mentions: OAI.KadisonSimilarity.representationVonNeumannAlgebra, OAI.KadisonSimilarity.starSubalgebraCommutant, OAI.KadisonSimilarity.ScalarHilbertCoordinates, OAI.KadisonSimilarity.cyclicCommonBaseMeasure, OAI.KadisonSimilarity.cyclicCommonEmbedding, OAI.KadisonSimilarity.boundedFieldOperator