The core component of the Connes rigidity formalization.
Countable discrete group carrier. Paper: §7.
- Carrier : Type u
The
Carriercomponent ofCountableDiscreteGroup.
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Coercion from the group wrapper to its carrier. Paper: §7.
ICC predicate boundary. Paper: §5.
Equations
- Connes.IsICC G = (Infinite G.Carrier ∧ ∀ (g : G.Carrier), g ≠ 1 → (conjugatesOf g).Infinite)
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Unitary-representation carrier. Paper: §4.
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Invariant-vector predicate. Paper: §4.
Equations
- π.IsInvariant ξ = ∀ (g : G), ↑(π g) ξ = ξ
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Almost-invariant-vector predicate. Paper: §4.
Equations
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Property-(T), universe-polymorphic in the representation carrier so concrete
Type 0 groups are not restricted to Type 0 Hilbert spaces. Paper: §4.
Equations
- One or more equations did not get rendered due to their size.
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Relative property-(T), universe-polymorphic in the representation carrier so
concrete Type 0 groups are not restricted to Type 0 Hilbert spaces. Paper: §4.
Equations
- One or more equations did not get rendered due to their size.
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Group-indexed Hilbert carrier. Paper: §3.
Equations
- Connes.GroupL2 G = lp (fun (x : G) => ℂ) 2
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Left-regular unitary boundary. Paper: §3.
Equations
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Left-regular representation boundary. Paper: §3.
Equations
- Connes.leftRegularRepresentation G = { toFun := Connes.leftRegularUnitary, map_one' := ⋯, map_mul' := ⋯ }
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Bicommutant presentation of the von Neumann closure boundary. Paper: §3.
Equations
- Connes.vonNeumannClosure S = (let __StarSubalgebra := StarSubalgebra.centralizer ℂ S; { toStarSubalgebra := __StarSubalgebra, centralizer_centralizer' := ⋯ }).commutant
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The von Neumann closure has the expected bicommutant carrier.
Membership in the von Neumann closure is membership in the star-algebraic bicommutant of the generating set.
Group von Neumann algebra boundary. Paper: §3.
Equations
- Connes.groupVonNeumannAlgebra G = Connes.vonNeumannClosure (Set.range fun (g : G.Carrier) => ↑((Connes.leftRegularRepresentation G.Carrier) g))
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Group von Neumann algebra carrier. Paper: §3.
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Point-mass basis vector boundary. Paper: §3.
Equations
- Connes.delta G g = lp.single 2 g 1
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Canonical trace boundary. Paper: §3.
Equations
- Connes.canonicalTrace G x = inner ℂ (Connes.delta G 1) (↑x (Connes.delta G 1))
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Projection-supremum predicate boundary. Leastness is among projection upper bounds,
not all ambient upper bounds as in IsLUB. Paper: §3.
Equations
- Connes.IsProjectionSupremum S p = (IsStarProjection p ∧ (∀ q ∈ S, IsStarProjection q ∧ q ≤ p) ∧ ∀ (r : A), IsStarProjection r → (∀ q ∈ S, q ≤ r) → p ≤ r)
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Construct a projection supremum from its projection, upper-bound, and leastness clauses.
The supremum candidate is a projection.
Every member is a projection below the supremum candidate.
The supremum candidate lies below every projection upper bound.
Projection suprema are unique.
Preservation of projection suprema by a star-algebra equivalence and its inverse, relative to the supplied order relations. Paper: §3.
Equations
- One or more equations did not get rendered due to their size.
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Construct normality from projection-supremum transport in both directions.
A normal star-algebra equivalence preserves projection suprema.
The inverse of a normal star-algebra equivalence preserves projection suprema.
A composite of normal star-algebra equivalences is normal.
Trace-preserving factor-equivalence witness. Paper: §3.
The
toStarAlgEquivcomponent ofTracialGroupFactorEquiv.- normal : IsNormalStarAlgEquiv self.toStarAlgEquiv
- trace_preserving (x : ↥(GroupVonNeumannAlgebra G)) : canonicalTrace H (self.toStarAlgEquiv x) = canonicalTrace G x
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Trace-preserving factor-isomorphism predicate. Paper: §3.