MathlibAnnex.Analysis.CStarAlgebra.NonUnitalCStarRepresentation.component_matrixCoefficientKernel_eq_family
theorem
Describes each irreducible representation component by all of its nonzero vector coefficients.
Statement
Let be a complex C*-algebra, with no identity required, and let be a nonzero irreducible -representation on a complete complex Hilbert space. The inner product is conjugate-linear in its first argument. For nonzero , put
Write for the geometric structure space of . In this C*-algebra setting its points are precisely , where is extreme, for real convexity, in the closed unit ball of the Banach dual; the extreme-kernel identification guarantees this description from the original face definition. For , its closure is
Two points are linked if they are equal or their pair is not closed. Let be the equivalence class of under finite chains of linked points. Then, for every nonzero ,
Assumptions
The source uses the compatible C*-order on . Irreducibility includes nonzero action and excludes proper nonzero closed reducing subspaces. No faithfulness, finite dimension or separability is required. Under this irreducibility hypothesis, is a point of for every . The component is defined by the closure relation above, without assuming that is a topological closure.
Conclusion
Every point of the entire component, including one initially presented without reference to , is a coefficient kernel of this fixed representation. Conversely, every pair of nonzero coefficient vectors gives a point of the component. Thus the choice of the initial pair has no effect on this component. This is an equality of subsets of ; it does not identify an individual coefficient kernel with .
Main citations
- Exact whole-component theorem:
MathlibAnnex.Analysis.CStarAlgebra.NonUnitalCStarRepresentation.component_matrixCoefficientKernel_eq_family. - Component–representation correspondence: the equivalence between finite-chain components and unitary equivalence.
- The coefficient-kernel family and its same-component inclusion:
matrixCoefficientKernelFamilyandmatrixCoefficientKernelFamily_subset_component. - Ryotaro Tanaka, arXiv:2504.05551v1, Lemma 5.10. The present declaration gives the component formula for an arbitrary irreducible representation; the pure-state specialization and the intersection calculation have separate explanations.
Lean source signature (exact)
The declaration prefix below is a contiguous source excerpt, ending before its proof assignment.
theorem component_matrixCoefficientKernel_eq_family (pi : NonUnitalCStarRepresentation A H) (hpi : pi.IsIrreducible) (x y : H) (hx : x ≠ 0) (hy : y ≠ 0) : (NormedSpace.geometricStructureClosure ℂ A).component (matrixCoefficientKernel pi hpi x y hx hy) = matrixCoefficientKernelFamily pi hpiBack to the reading-guide item
| In the source | Mathematical meaning |
|---|---|
Algebra and ordervariable {A : Type u} [NonUnitalCStarAlgebra A] [Nontrivial A]
variable [PartialOrder A] [StarOrderedRing A]Fixed source | The nonzero complex C*-algebra with its compatible order; no identity is required. |
Representation spacevariable {H : Type v} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]Fixed source | The complex Hilbert space is complete. |
One irreducible representation(pi : NonUnitalCStarRepresentation A H) (hpi : pi.IsIrreducible)Fixed source | The same fixed nonzero irreducible representation supplies all coefficient kernels. It need not be faithful. |
Starting vectors(x y : H) (hx : x ≠ 0) (hy : y ≠ 0) :Fixed source | The starting pair is , without a normalization assumption. |
Component and full family(NormedSpace.geometricStructureClosure ℂ A).component
(matrixCoefficientKernel pi hpi x y hx hy) = matrixCoefficientKernelFamily pi hpi := byFixed source | The component is taken in the ambient closure , starting at . The complete equality is It concerns all points of that component, not just kernels chosen in advance. |
The coefficient-kernel familydef matrixCoefficientKernelFamily (pi : NonUnitalCStarRepresentation A H) (hpi : pi.IsIrreducible) :
Set (NormedSpace.GeometricStructureSpace ℂ A) :=
{I | ∃ (x y : H) (hx : x ≠ 0) (hy : y ≠ 0), matrixCoefficientKernel pi hpi x y hx hy = I}Fixed source | A point belongs to exactly when there are with . The vectors may depend on ; the representation is the same throughout. |
Exact surrounding source context (separate excerpts)
Exact surrounding source:
variable {A : Type u} [NonUnitalCStarAlgebra A] [Nontrivial A]
Back to the reading-guide itemExact surrounding source:
variable [PartialOrder A] [StarOrderedRing A]
Back to the reading-guide itemExact surrounding source:
variable {H : Type v} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
Back to the reading-guide itemRead exact source with highlighted declaration · Raw UTF-8 source · LFH Companion ·