MathlibAnnex.CStarAlgebra.CAR.exists_surjective_selectedAtomicCyclicIsometry
Uses shell reconstruction and residual lines to turn an isometric CAR intertwiner into a unitary equivalence on the source.
Statement
Under the shell-family, generator and irreducibility assumptions below, there exist unit vectors
for every
Assumptions
Let
Choose one pure state
A supplied shell family consists of unital complex star automorphisms
Let
Conclusion
The selected cyclic pieces exhaust the target Hilbert space. The source-restriction equivalence is the direct consequence obtained by viewing the surjective isometry as a unitary. The representation being assumed irreducible is
Proof route
The common-root vector-state theorem supplies compatible unit vectors. Cyclic-sum assembly gives an isometry with closed source-reducing range
Proof steps
The common-root construction gives
and of norm one with the selected CAR vector states, , and fixedness under their respective flags. Assemble the cyclic pieces into . Its range is closed because is complete and is an isometry. The relations for and show that reduces . Let project onto the common range of and let project onto the common range of . Assembly gives . Since
, the represented root generator is . Thus the root-index member equals the common vector . Consequently and . Reconstruct with , , and . The operators and are strong limits of finite sums of and their adjoints. Closedness and source reduction make invariant under both limits. Fixedness and the vector transport give
and . For , the vector lies in , so . For the adjoint, use and to obtain . Thus reduces the residual corner and, together with the shell sum, every . The orthogonal projection onto
commutes with the represented source and every added generator. The commutation relation is stable under star-algebra operations and operator-norm limits, so reduces all of . It contains the unit vector and is therefore nonzero. Irreducibility gives , which is exactly surjectivity of . Its pointed-vector and source intertwining identities are retained.
Main citations
- Exact declaration and proof · Exact source
- MathlibAnnex.CStarAlgebra.CAR.RepresentativeShellFamily · Exact source
- MathlibAnnex.CStarAlgebra.CAR.selectedAtomicRepresentation · Exact source
- MathlibAnnex.CStarAlgebra.CAR.exists_targetDefectVectorFamily · Exact source
- MathlibAnnex.CStarAlgebra.CAR.exists_selectedAtomicCyclicIsometry · Exact source
- MathlibAnnex.CStarAlgebra.CAR.exists_targetShellReconstruction · Exact source
- MathlibAnnex.CStarAlgebra.AtomicConstruction.reduces_concreteTarget_of_generators · Exact source
- MathlibAnnex.CStarAlgebra.CAR.selectedAtomicRepresentation_unitaryEquivalent_restricted · Exact source
- MathlibAnnex.CStarAlgebra.CAR.ambientInclusion_unitaryEquivalent · Exact source
- MathlibAnnex.CStarAlgebra.CAR.completedRootPureState · Exact source
Lean source signature (exact)
theorem exists_surjective_selectedAtomicCyclicIsometry
(family : RepresentativeShellFamily)
(L : MathlibAnnex.CStarAlgebra.PureState.GNSClass Limit →
MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState →L[ℂ]
MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState)
(hLunit : ∀ i, L i ∈ unitary
(MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState →L[ℂ]
MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState))
(hLsource : ∀ i n, (L i).comp (selectedAtomicRepresentation
(transportedFlag family i n - transportedFlag family i (n + 1))) =
representedShellLink family i n)
(hLroot : L completedRootPureState.classOf = 1)
{K : Type v} [NormedAddCommGroup K] [InnerProductSpace ℂ K]
[CompleteSpace K] (rho : Representation (AtomicTarget L) K)
(hrho : rho.IsIrreducible) :
∃ (eta_o : K) (eta : MathlibAnnex.CStarAlgebra.PureState.GNSClass Limit → K)
(W : MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState →ₗᵢ[ℂ] K),
Function.Surjective W ∧
‖eta_o‖ = 1 ∧
(∀ i, ‖eta i‖ = 1) ∧
(∀ i, W (MathlibAnnex.CStarAlgebra.PureState.selectedEmbedding completedRootPureState i
(MathlibAnnex.CStarAlgebra.PureState.selectedVector completedRootPureState i)) = eta i) ∧
(∀ i, (Unitary.linearIsometryEquiv
(representedGeneratorUnitary L hLunit rho i) : K ≃ₗᵢ[ℂ] K)
(eta i) = eta_o) ∧
∀ a,
W.toContinuousLinearMap.comp (selectedAtomicRepresentation a) =
((restrictedRepresentation L rho) a).comp
W.toContinuousLinearMapHere Limit is completedRootPureState is the root state SelectedAtomicHilbert ... is AtomicTarget L is restrictedRepresentation L rho is eta_o denotes the common vector eta i denotes i. The equality of eta at the root index with eta_o follows from hLroot, rather than from their names. Function.Surjective W supplies the extra property that the isometry fills hLsource records the shell action; no hypothesis named hLmap occurs in this declaration.
Read exact source with highlighted declaration · Raw UTF-8 source · Card PDF
Lean realization notes
The conclusion displayed here intertwines the CAR source. To obtain intertwining for every element of
Exact Card identity
Language: en
CARD_CONTENT_COMPLETE
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