MATHLIBANNEX / PROJECT LFH

Trace extensions and faithful representations on a separable space

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Scope

The CAR trace extends uniquely to a state on the same shell-generated target, and that extension is tracial. Pointed transport supplies faithful representations on separable trace spaces; representation faithfulness is distinct from faithfulness of a vector state.

9 direct Cards + 30 reused prerequisites = 39 unique Cards. This count is a selected Card closure, not a source-declaration count.

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Cards in this route

Read this route with prerequisites

Reference index: direct Cards and reused prerequisites

Direct references: 51 — Extending the CAR trace to the fixed shell target · 59 — Pointed unitary transport between trace-cyclic target representations · 55 — The GNS representation of the target trace extension · 52 — Uniqueness among all state extensions of the CAR trace · 53 — The unique trace extension is tracial on the whole target · 56 — Faithfulness of the target-state GNS representation · 57 — The target represented on the CAR trace GNS space · 54 — The fixed shell target has a unique tracial state · 58 — Faithfulness of the representation on the CAR trace Hilbert space

Reused prerequisites: 38 — The atomic common range is one embedded GNS line · 43 — The ambient inclusion of the fixed shell-family target · 3 — The product-vector state on the completed CAR algebra · 10 — Root compression becomes scalar in norm · 27 — The selected GNS representation of a pure-state class · 36 — The matching GNS fiber retains exactly its cyclic line · 28 — Distinct GNS classes have no unitary intertwiner · 29 — The atomic direct sum of the selected CAR representations · 46 — Every irreducible representation is unitarily equivalent to the inclusion · 33 — Realizing a shell family by a faithful irreducible operator algebra · 42 — The CAR source map into the fixed shell-family target · 34 — Shell matching fixes the trace of transported flags · 1 — The normalized trace on a finite CAR stage · 35 — Transported flags vanish on vectors generated by a trace vector · 9 — The decreasing root projections in the CAR completion · 48 — Closed-ideal simplicity of the shell-generated algebra · 4 — Purity of the completed root state · 30 — An irreducible operator algebra constructed from projection shells · 7 — Constructing the normalized trace on the completed CAR algebra · 2 — The CAR algebra as a completion of finite matrix stages · 37 — An inequivalent GNS fiber has no residual common range · 8 — Normalization and the trace identity determine the CAR trace · 40 — An irreducible target representation has a surviving fixed space · 39 — Reconstructing a represented unitary from its shells and residual corner · 25 — A fixed representative family of CAR shell data · 31 — The atomic-shell construction on selected pure-GNS fibers · 32 — The closed operator algebra generated by a representation and extra operators · 45 — The cyclic sum fills every irreducible target representation · 41 — A common root vector realizes every selected state through the generators · 44 — Assembling selected GNS cyclic subspaces into an isometric source representation

Detailed route conditions

Fix the same and , and first extend the CAR trace to a state on . Existence precedes uniqueness and traciality. In each trace-realizing cyclic representation, the estimates for and kill the residual projections on the source-cyclic subspace. Target cyclicity then proves source cyclicity. The fixed-left-hand-side limit calculation is retained with its full dependence in the pointed-transport Card.

Pointed transport proves uniqueness among all state extensions. Uniqueness gives invariance under source unitaries; their span and the actual represented shell limits put all generators in the closed centralizer. This proves traciality. A different restriction argument then proves uniqueness among all tracial states.

The CAR trace space and the extension-state space are different: the selected unitary points as , and . This is not the capture map . Faithfulness of a representation is distinct from faithfulness of its vector state. The Hilbert spaces are separable here; norm separability of is not assumed.

Reference index: exact Card references

Exact Card references

Dependency-first reading route

Read selected Card prerequisites before their uses. Levels are recomputed from the selected reachability-preserving projection; omitted source helpers remain traceable in the source exploration.

39 Cards

Level 0 (5 Cards)

Level 0

The selected GNS representation of a pure-state class

A choice of representative pure states, fixed literally at a root, gives one concrete GNS representation per equivalence class.

MathlibAnnex.CStarAlgebra.PureState.selectedRepresentation

Level 0

The CAR algebra as a completion of finite matrix stages

Names the completed CAR algebra in which finite matrix calculations can be extended by norm approximation.

MathlibAnnex.CStarAlgebra.CAR.Limit

Level 0

A fixed representative family of CAR shell data

One family records a transporting automorphism and exact shell links for each selected pure-state class, with an explicitly fixed root component.

MathlibAnnex.CStarAlgebra.CAR.RepresentativeShellFamily

Level 0

The closed operator algebra generated by a representation and extra operators

Places a represented algebra and a chosen family of bounded operators in one concrete closed algebra.

MathlibAnnex.CStarAlgebra.AtomicConstruction.concreteTarget

Level 1 (5 Cards)

Level 1

Constructing the normalized trace on the completed CAR algebra

Carries compatible bounded matrix traces through the algebraic limit, normed union and completion.

MathlibAnnex.CStarAlgebra.CAR.trace

Level 1

An irreducible operator algebra constructed from projection shells

Shell partial isometries with rank-one limiting defects can be completed to unitary links that join inequivalent irreducible fibers.

MathlibAnnex.CStarAlgebra.AtomicConstruction.exists_irreducible_atomicShellModel

Level 1

Distinct GNS classes have no unitary intertwiner

The class index makes the selected pure-GNS family pairwise unitarily inequivalent.

MathlibAnnex.CStarAlgebra.PureState.no_unitaryIntertwiner_selectedRepresentation

Level 1

The decreasing root projections in the CAR completion

The distinguished stage corners give a nested sequence of projections supporting the root state.

MathlibAnnex.CStarAlgebra.CAR.rootFlag

Level 2 (5 Cards)

Level 2

Root compression becomes scalar in norm

Extends an exact rank-one compression identity on finite stages to a pointwise norm limit on the completed algebra.

MathlibAnnex.CStarAlgebra.CAR.tendsto_norm_compressionError

Level 2

Purity of the completed root state

Passes extremality of the root vector states from every finite matrix stage to the completed CAR algebra.

MathlibAnnex.CStarAlgebra.CAR.isPureState_rootState

Level 2

The atomic-shell construction on selected pure-GNS fibers

Pure-state GNS data supplies the irreducible and inequivalent fibers required by the generic shell construction.

MathlibAnnex.CStarAlgebra.AtomicConstruction.exists_irreducible_pureAtomicShellModel

Level 2

Shell matching fixes the trace of transported flags

Recovers exact trace values from the initial and final supports of shell links.

MathlibAnnex.CStarAlgebra.CAR.trace_transportedFlag

Level 3 (4 Cards)

Level 3

The atomic direct sum of the selected CAR representations

All selected pure-GNS fibers of the completed CAR algebra act together on one Hilbert direct sum.

MathlibAnnex.CStarAlgebra.CAR.selectedAtomicRepresentation

Level 3

The matching GNS fiber retains exactly its cyclic line

Identifies the residual projection of a transported CAR flag in its matching pure-state representation.

MathlibAnnex.CStarAlgebra.CAR.selected_commonFixedProjection_eq_rankOne

Level 3

Transported flags vanish on vectors generated by a trace vector

Turns decay of projection traces into norm convergence on each source-orbit vector.

MathlibAnnex.CStarAlgebra.CAR.tendsto_transportedFlag_orbit_zero

Level 3

An inequivalent GNS fiber has no residual common range

Uses compression and cyclic transport to exclude fixed vectors in every other chosen pure-state class.

MathlibAnnex.CStarAlgebra.CAR.selected_commonFixedProjection_eq_zero

Level 4 (3 Cards)

Level 4

The atomic common range is one embedded GNS line

Assembles the matching and inequivalent fiber calculations in an arbitrary Hilbert direct sum.

MathlibAnnex.CStarAlgebra.CAR.iInf_range_atomic_transportedFlag_eq_span

Level 4

Assembling selected GNS cyclic subspaces into an isometric source representation

Joins mutually orthogonal pure-state cyclic copies and controls the limiting flag projections on their sum.

MathlibAnnex.CStarAlgebra.CAR.exists_selectedAtomicCyclicIsometry

Level 4

Reconstructing a represented unitary from its shells and residual corner

Separates a represented generator into a strong shell sum and the exact operator between its limiting fixed spaces.

MathlibAnnex.CStarAlgebra.CAR.exists_targetShellReconstruction

Level 5 (2 Cards)

Level 5

Realizing a shell family by a faithful irreducible operator algebra

Constructs unitary links between pure-state summands and an irreducible algebra containing a faithful copy of CAR.

MathlibAnnex.CStarAlgebra.CAR.exists_completedAtomicShellModel

Level 5

An irreducible target representation has a surviving fixed space

Rules out simultaneous disappearance of all limiting CAR flags by passing reduction through the reconstructed generators.

MathlibAnnex.CStarAlgebra.CAR.exists_nonzero_targetFixedSpace

Level 6 (3 Cards)

Level 6

A common root vector realizes every selected state through the generators

Builds a compatible family of unit vectors from a surviving residual space and identifies their CAR vector states.

MathlibAnnex.CStarAlgebra.CAR.exists_targetDefectVectorFamily

Level 6

The CAR source map into the fixed shell-family target

Restricting the codomain of the selected atomic representation gives the source map into one fixed generated target.

MathlibAnnex.CStarAlgebra.CAR.shellFamilySourceHom

Level 7 (3 Cards)

Level 7

Pointed unitary transport between trace-cyclic target representations

Source cyclicity and strong shell sums extend the canonical CAR orbit isometry to the whole target.

MathlibAnnex.CStarAlgebra.CAR.exists_pointed_unitary_of_trace_of_cyclic

Level 7

The cyclic sum fills every irreducible target representation

Uses shell reconstruction and residual lines to turn an isometric CAR intertwiner into a unitary equivalence on the source.

MathlibAnnex.CStarAlgebra.CAR.exists_surjective_selectedAtomicCyclicIsometry

Level 8 (2 Cards)

Level 8

The GNS representation of the target trace extension

The chosen state on the existing target supplies its cyclic GNS representation.

MathlibAnnex.CStarAlgebra.CAR.tracialRepresentation

Level 8

Every irreducible representation is unitarily equivalent to the inclusion

Extends the unitary equivalence from the CAR source to all additional generators and the norm-closed target.

MathlibAnnex.CStarAlgebra.CAR.ambientInclusion_unitaryEquivalent

Level 9 (4 Cards)

Level 9

The target represented on the CAR trace GNS space

A fixed pointed unitary transports the target action onto the Hilbert space constructed from CAR alone.

MathlibAnnex.CStarAlgebra.CAR.traceModelRepresentation

Level 9

The unique trace extension is tracial on the whole target

Unitary invariance, strong shell sums, and a closed centralizer extend the trace identity beyond the source.

MathlibAnnex.CStarAlgebra.CAR.traceExtension_mul_comm

Level 9

Closed-ideal simplicity of the shell-generated algebra

Uses a faithful irreducible representation in the unique unitary-equivalence class to rule out proper nonzero closed two-sided ideals.

MathlibAnnex.CStarAlgebra.CAR.isSimpleCStarAlgebra_shellFamilyTarget

Level 10 (2 Cards)

Level 10

Faithfulness of the target-state GNS representation

The ideal dichotomy of the same target forces the constructed nonzero representation to be injective.

MathlibAnnex.CStarAlgebra.CAR.tracialRepresentation_injective

Level 11 (1 Card)

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