MathlibAnnex.CStarAlgebra.PureState.selectedRepresentation
def
A choice of representative pure states, fixed literally at a root, gives one concrete GNS representation per equivalence class.
Statement
Let be a unital complex C*-algebra, with the positive order used for its states, and fix a pure state . A pure state is an extreme point of the normalized positive continuous linear functionals. Let be the set of pure-state GNS representations modulo unitary equivalence. For each , choose a pure state in that class, retaining literally at . Write for its GNS space, representation and canonical cyclic vector. The selected representation is the GNS action associated to this particular . The choice concerns the representative state; the construction then uses its actual GNS Hilbert space and action.
Definition
Take the chosen state , regard it as a positive linear functional, and form its GNS completion . Left multiplication induces the bounded action on that completion. The selected vector is the GNS cyclic vector. Its orbit is dense. The vector-functional identity and purity of , together with this cyclicity and normalization, supply the separate irreducibility theorem.
Assumptions
The class and the root pure state are given. GNS representations here are unital complex-linear star homomorphisms on complete complex Hilbert spaces. No separability or faithfulness of is assumed.
Conclusion
The definition specifies on . The separate selected-vector and pure-GNS results give , , and irreducibility of . These properties explain why this selected family supplies the summands of the direct-sum representation.
The inner product is conjugate linear in its first argument. Irreducibility means that the only closed reducing subspaces are and ; this Hilbert space is nonzero because it contains the unit vector . The definition does not itself prove those properties, and it does not claim that different pure states always have inequivalent GNS representations.
Main citations
- Definition
and its exact construction —
MathlibAnnex.CStarAlgebra.PureState.selectedRepresentation - Root-preserving
choice of a pure state in each GNS class —
MathlibAnnex.CStarAlgebra.PureState.representative - The
selected GNS Hilbert space —
MathlibAnnex.CStarAlgebra.PureState.SelectedGNS - The
selected cyclic vector —
MathlibAnnex.CStarAlgebra.PureState.selectedVector - Normalization
of the selected cyclic vector —
MathlibAnnex.CStarAlgebra.PureState.norm_selectedVector - The
selected state as a vector functional —
MathlibAnnex.CStarAlgebra.PureState.selected_vectorFunctional - Density
of the selected GNS orbit —
MathlibAnnex.CStarAlgebra.PureState.denseRange_representative_gns_orbit - Irreducibility
supplied by purity and cyclicity —
MathlibAnnex.CStarAlgebra.PureState.isIrreducible_selectedRepresentation
Lean source signature (exact)
noncomputable def selectedRepresentation (root : PureState A) (j : GNSClass A) :
MathlibAnnex.Analysis.CStarAlgebra.Representation A (SelectedGNS root j) :=
(representative root j).positiveFunctional.gnsStarAlgHom
| In the source | Mathematical meaning |
|---|---|
A; root : PureState A |
The given unital complex C*-algebra with its state order, and a fixed pure state . A pure state is a positive normalized continuous complex-linear functional extreme in the real convex state space. |
j : GNSClass A |
A class of pure-state GNS representations modulo unitary equivalence; this class is not itself a state functional. |
representative root j |
The selected pure state belonging to class , chosen with at . |
SelectedGNS root j |
The actual complete GNS Hilbert space of that selected state . |
Representation A (SelectedGNS root j) |
The output is a unital complex-linear star homomorphism . |
(representative root j).positiveFunctional.gnsStarAlgHom |
The full RHS takes the positive functional of and its GNS left-multiplication action on . The vector and the cyclicity, normalization and irreducibility properties have their separate cited definitions and theorems. |
Further source notes: The vector
is named | |
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