The block Hilbert space H^κ.
Equations
- CommutingRepetition.Block.BH M κ = PiLp 2 fun (x : κ) => M.H
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Coordinate embeddings and projections #
Coordinate embedding v ↦ (0, …, v, …, 0).
Equations
- CommutingRepetition.Block.embed M κ r = ↑(PiLp.continuousLinearEquiv 2 ℂ fun (x : κ) => M.H).symm ∘SL ContinuousLinearMap.pi fun (r' : κ) => if r' = r then ContinuousLinearMap.id ℂ M.H else 0
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Coordinate projection.
Equations
- CommutingRepetition.Block.proj M κ r = PiLp.proj 2 (fun (x : κ) => M.H) r
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Entries #
The (r, r') entry of a block operator.
Equations
- CommutingRepetition.Block.entry M κ T r r' = CommutingRepetition.Block.proj M κ r ∘SL T ∘SL CommutingRepetition.Block.embed M κ r'
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The block algebra #
Block operators with all entries in the concrete von Neumann algebra.
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- One or more equations did not get rendered due to their size.
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The lift into the amplification #
The amplification dimension.
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The target algebra M_d(vnAlg M) as a standard tracial algebra.
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The index equivalence.
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The entry matrix of a block-algebra element, reindexed to Fin d.
Equations
- One or more equations did not get rendered due to their size.
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The lift blockAlg M κ →⋆ₐ[ℂ] M_d(vnAlg M).
Equations
- CommutingRepetition.Block.lift M κ = { toFun := CommutingRepetition.Block.liftFun M κ, map_one' := ⋯, map_mul' := ⋯, map_zero' := ⋯, map_add' := ⋯, commutes' := ⋯, map_star' := ⋯ }
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The amplified trace of a lifted block operator: d⁻¹ ∑ᵣ φ(entry T r r).
The corner copy of vnAlg M #
The corner copy E s T = embed s ∘ T ∘ proj s.
Equations
- CommutingRepetition.Block.E M κ s T = ⟨CommutingRepetition.Block.embed M κ s ∘SL ↑T ∘SL CommutingRepetition.Block.proj M κ s, ⋯⟩
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The corner copy as an additive monoid homomorphism.
Equations
- CommutingRepetition.Block.Eadd M κ s = { toFun := CommutingRepetition.Block.E M κ s, map_zero' := ⋯, map_add' := ⋯ }
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τ_N (lift (E s T)) = d⁻¹ φ(T).
Placement, matrix units and the block-diagonal right action #
X ↦ embed r ∘ X ∘ proj r' as a continuous linear map.
Equations
- One or more equations did not get rendered due to their size.
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The block-diagonal right action diag (R b).
Equations
- CommutingRepetition.Block.Rt M κ b = ∑ r : κ, (CommutingRepetition.Block.place M κ r r) (M.Rop b)
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Membership in the block algebra is commutation with the block-diagonal right action.