MATHLIBANNEX / CANONICAL DECLARATION CARD

The selected GNS representation of a pure-state class

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

Supporting route explanation

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 selectedVector root j in its separate cited definition; the normalization, vector-functional identity and irreducibility are separate cited theorems, not extra fields of this definition.

Earlier published Card and PDF

Exact content identity

Declaration: MathlibAnnex.CStarAlgebra.PureState.selectedRepresentation

Accepted content SHA-256: 03a298e788ee0db85d5beb7267b35048408970cdbf4e2bccc8c0f5163ee51b84

Accepted source guide SHA-256: ce6f62005374b949f2186d0a6ac7e0ed796f2b9cbdb22c8fc03e4289ac0bdef7

Source commit: 437e6e46228bbb8e91211ebded349d7a30020e73

Back to top ↑