MathlibAnnex.CStarAlgebra.CAR.shellFamilyInclusion_unitaryEquivalent_nonUnital
Shows why allowing nonunital input representations does not enlarge the irreducible representation class of the shell-generated algebra.
Statement
Let
Assumptions
Let
Index chosen pure-state Gelfand-Naimark-Segal (GNS) representations by their unitary-equivalence classes
A fixed shell family consists of complex-linear unital star automorphisms
At the root,
Let
Choose once a family of unitary operators
Put
The space
Conclusion
The intertwining equation uses the original map
Proof route
Put
Proof steps
For every
, . Star preservation also controls adjoints, so the range of is reducing. If
, then every is zero. Irreducibility therefore forces the closed range of this nonzero idempotent to be , whence . Use the theorem identifying every unital irreducible representation with the fixed inclusion. Rebundling
as unital changes no operator, so its resulting unitary equivalence is exactly the claimed one.
Main citations
- Exact declaration and proof · Exact source
- MathlibAnnex.CStarAlgebra.CAR.RepresentativeShellFamily · Exact source
- MathlibAnnex.CStarAlgebra.CAR.exists_completedAtomicShellModel · Exact source
- MathlibAnnex.CStarAlgebra.CAR.isUniqueIrreducibleModel_shellFamilyInclusion · Exact source
- MathlibAnnex.CStarAlgebra.CAR.isUniqueIrreducibleModelAmongNonUnital_shellFamilyInclusion · Exact source
- MathlibAnnex.Analysis.CStarAlgebra.NonUnitalRepresentation.map_one_eq_one_of_isIrreducible · Exact source
- The root state bundled with its purity proof · Exact source
Lean source signature (exact)
theorem shellFamilyInclusion_unitaryEquivalent_nonUnital
(family : RepresentativeShellFamily)
{K : Type v} [NormedAddCommGroup K] [InnerProductSpace ℂ K]
[CompleteSpace K]
(rho : NonUnitalRepresentation
(A := ShellFamilyTarget family) (H := K))
(hrho : rho.IsIrreducible) :
∃ U :
MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState ≃ₗᵢ[ℂ] K,
∀ (a : ShellFamilyTarget family)
(x : MathlibAnnex.CStarAlgebra.PureState.SelectedAtomicHilbert completedRootPureState),
U (shellFamilyInclusion family a x) = rho a (U x)Here completedRootPureState is the root state SelectedAtomicHilbert completedRootPureState is ShellFamilyTarget family is shellFamilyInclusion family is NonUnitalRepresentation means a complex-linear star representation without a required unit law. Its IsIrreducible predicate includes
Read exact source with highlighted declaration · Raw UTF-8 source · Card PDF
Lean realization notes
The result imposes no separability restriction and does not claim that all representations are irreducible. The shell family is fixed before
Exact Card identity
Language: en
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