Documentation

LeanPool.ConnesRigidity.Foundation.OperatorAlgebra.FiniteIndex

The finite index component of the Connes rigidity formalization.

Countable discrete subgroup wrapper. Paper: §4.

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    noncomputable def Connes.OpenAIPort.FiniteIndex.correction {G : Type u} [Group G] (S : Subgroup G) (g : G) (q : G S) :
    S

    Correction element for the finite-index induced representation. Paper: §4.

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      @[simp]
      theorem Connes.OpenAIPort.FiniteIndex.correction_coe {G : Type u} [Group G] (S : Subgroup G) (g : G) (q : G S) :

      Pointwise formula for the correction element. Paper: §4.

      theorem Connes.OpenAIPort.FiniteIndex.correction_mul {G : Type u} [Group G] (S : Subgroup G) (g h : G) (q : G S) :
      correction S (g * h) q = correction S g (h q) * correction S h q

      Multiplicativity of the correction cocycle. Paper: §4.

      @[simp]
      theorem Connes.OpenAIPort.FiniteIndex.correction_one {G : Type u} [Group G] (S : Subgroup G) (q : G S) :
      correction S 1 q = 1

      Unit value of the correction cocycle. Paper: §4.

      theorem Connes.OpenAIPort.FiniteIndex.subgroup_smul_baseCoset {G : Type u} [Group G] (S : Subgroup G) (s : S) :
      s 1 = 1

      The subgroup fixes the base coset. Paper: §4.

      The chosen representative of the base coset lies in the subgroup. Paper: §4.

      @[instance_reducible]

      The finiteIndexQuotientFintype construction used in the Connes rigidity formalization.

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        @[reducible, inline]
        abbrev Connes.OpenAIPort.FiniteIndex.InducedSpace {G : Type u} [Group G] (S : Subgroup G) {H : Type v} :
        Type (max u v)

        Hilbert space induced from a finite-index subgroup. Paper: §4.

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          Linear-isometric action on the induced Hilbert space. Paper: §4.

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            @[simp]
            theorem Connes.OpenAIPort.FiniteIndex.inducedLinearIsometryEquiv_apply {G : Type u} [Group G] (S : Subgroup G) [S.FiniteIndex] {H : Type v} [NormedAddCommGroup H] [InnerProductSpace H] [CompleteSpace H] (π : UnitaryRepresentation (↥S) H) (g : G) (ξ : InducedSpace S) (q : G S) :
            ((inducedLinearIsometryEquiv S π g) ξ).ofLp q = (π (correction S g (g⁻¹ q))) (ξ.ofLp (g⁻¹ q))

            Pointwise formula for the induced linear isometry. Paper: §4.

            @[simp]
            theorem Connes.OpenAIPort.FiniteIndex.inducedUnitary_apply {G : Type u} [Group G] (S : Subgroup G) [S.FiniteIndex] {H : Type v} [NormedAddCommGroup H] [InnerProductSpace H] [CompleteSpace H] (π : UnitaryRepresentation (↥S) H) (g : G) (ξ : InducedSpace S) (q : G S) :
            ((inducedUnitary S π g) ξ).ofLp q = (π (correction S g (g⁻¹ q))) (ξ.ofLp (g⁻¹ q))

            Pointwise formula for the induced unitary. Paper: §4.

            Induced unitary representation of the ambient group. Paper: §4.

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              @[simp]
              theorem Connes.OpenAIPort.FiniteIndex.inducedRepresentation_apply {G : Type u} [Group G] (S : Subgroup G) [S.FiniteIndex] {H : Type v} [NormedAddCommGroup H] [InnerProductSpace H] [CompleteSpace H] (π : UnitaryRepresentation (↥S) H) (g : G) (ξ : InducedSpace S) (q : G S) :
              (((inducedRepresentation S π) g) ξ).ofLp q = (π (correction S g (g⁻¹ q))) (ξ.ofLp (g⁻¹ q))

              Pointwise formula for the induced representation. Paper: §4.

              Sum-of-coordinate norm bound for the induced space. Paper: §4.

              A nonzero invariant induced vector is nonzero at the base coset. Paper: §4.

              theorem Connes.OpenAIPort.FiniteIndex.correction_conjugate_at_baseCoset {G : Type u} [Group G] (S : Subgroup G) (s : S) :
              have r := Quotient.out 1, ; correction S ↑(r * s * r⁻¹) 1 = s

              Correction conjugacy at the base coset. Paper: §4.

              Invariant induced vectors restrict to invariant subgroup vectors. Paper: §4.