MathlibAnnex.Analysis.CStarAlgebra.NonUnitalCStarRepresentation.exists_preimage_rankOne_of_singleton
theorem
Turns one represented rank-one projection into every rank-one operator using dense orbits and a closed range.
Statement
Let be a nonzero complex -algebra, with no unit assumed, let be a separable complex Hilbert space, and let represent the unique unitary-equivalence class of nonzero irreducible -representations. For every there is such that
Assumptions
The vectors are arbitrary, including zero. They need not be unit vectors. The separability assumption concerns . No unit is required in .
Conclusion
Each rank-one operator belongs to the image of the original algebra, not merely to the image of its unitization.
Proof route
Find one rank-one projection in the range. Use irreducibility to obtain a dense original-algebra orbit, multiply around the projection, and pass to limits in both vectors.
Proof steps
Apply A rank-one projection in a singleton model to the nonzero ordered , separable , and singleton . It supplies and a unit vector with . In particular . The theorem Faithfulness of a non-unital singleton model also gives injectivity of .
The dense-orbit step in One rank-one projection generates all rank-one operators in the range uses irreducibility of the unitized representation. Its orbit of is dense; every unitization element has the form and acts by
Thus already is dense in . This calculation is why the preimages below stay in .
For and , multiplicativity and adjoints give
Hence .
Because is injective, it is isometric and has norm-closed range. Approximate arbitrary by vectors in the dense orbit. The estimates and
show convergence of the corresponding rank-one operators. Closedness then puts in , which is the asserted existence of .
Main citations
Lean source signature (exact)
theorem exists_preimage_rankOne_of_singleton [Nontrivial A]
[PartialOrder A] [StarOrderedRing A]
[TopologicalSpace.SeparableSpace H]
(pi : NonUnitalCStarRepresentation A H)
(hsingle : IsSingletonIrreducibleModel.{u, v, u} pi) :
∀ x y : H, ∃ a : A, pi a = InnerProductSpace.rankOne ℂ x y
| In the source | Mathematical meaning |
|---|---|
[Nontrivial A] |
The algebra is nonzero: . This condition does not say whether a unit is assumed; that information comes from the surrounding -algebra structure. |
[PartialOrder A] [StarOrderedRing A] |
These typeclasses provide the usual order on a -algebra, equivalently when is positive. They are used by the state and positivity arguments. |
[TopologicalSpace.SeparableSpace H] |
is a separable complex Hilbert space. |
pi : NonUnitalCStarRepresentation A H |
The specified -representation ; its interface does not require a unit equation. |
hsingle : IsSingletonIrreducibleModel.{u, v, u} pi |
The specified representation is nonzero irreducible, and every nonzero irreducible -representation of the same algebra is unitarily equivalent to it. |
∀ x y : H, ∃ a : A |
After any two vectors are chosen, an element may be chosen depending on both. |
InnerProductSpace.rankOne ℂ x y |
The entire operator , with this order of . |
pi a = InnerProductSpace.rankOne ℂ x y |
The chosen represents that operator on every vector . |
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