How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
CAR over a Hilbert Space Has the Universal Inductive-Limit Norm
Statement
Assume Countable Choice (The Axiom of Countable Choice ()). Let be a complex Hilbert space, and let be the completion of its directed union of finite-dimensional CAR algebras from CAR C*-Algebra over a Complex Hilbert Space. Let be a complex Hilbert space, and let be a complex-linear family of bounded operators satisfying
There is a unique unital isometric -homomorphism with . For each in the algebraic union, its inductive-limit norm equals the supremum of over all such families on nonzero Hilbert spaces. This family is nonempty: the fermionic Fock representation of Fock Creation and Annihilation Operators Satisfy the CAR attains the norm on every finite stage.
Facts & Assumptions
Given: A complex Hilbert space , a nonzero complex Hilbert space , and a complex-linear CAR family .
is the completion of the directed union of its finite-dimensional CAR C*-algebras, with generator-preserving isometric inclusions (CAR C*-Algebra over a Complex Hilbert Space, Finite-Subspace CAR Inclusions Are Isometric).
Every finite-dimensional CAR C*-algebra is a full matrix algebra, and every unital -representation on a nonzero Hilbert space is isometric (Finite-Dimensional CAR over an Inner-Product Space Is a Matrix Algebra).
Fermionic Fock space has a nonzero vacuum vector (Fermionic Fock Space over a Complex Hilbert Space).
Fock creation operators and their adjoints satisfy the stated CAR relations (Fock Creation and Annihilation Operators Satisfy the CAR).
If is Banach, then is Banach for the operator norm (If (Y) is Banach then (\mathcal B(X,Y)) is Banach).
denotes bounded linear operators with operator norm (The spaces (\mathcal B(X,Y)) and (\mathcal B(X)) of bounded linear operators, The operator norm as the least bound and as the unit-sphere or unit-ball supremum).
Countable Choice is retained for the Hilbert tensor/Fock construction and Hilbert-space adjoints in the Fock representation (The Axiom of Countable Choice (), The Hilbert-space adjoint of a bounded operator, Hilbert-adjoint identities).
Under Countable Choice, bounded Hilbert-space adjoints satisfy and (Hilbert-adjoint identities).
Operator norms satisfy (Composition satisfies |ST|\le|S|,|T|).
A C*-norm is submultiplicative and its involution is isometric (C star algebra).
Proof
For each finite-dimensional , the restriction satisfies the defining relations of . Its universal property gives a unital -homomorphism from that algebra to . These homomorphisms agree on inclusions because each sends every to . By [F2], every is isometric since . They therefore define an isometric -homomorphism on the algebraic union.
Since is Hilbert, it is Banach; applying [F5] with shows is complete for its operator norm [F6]. The isometry sends Cauchy sequences to Cauchy sequences, so for choose a local sequence and define . Isometry makes this limit independent of the chosen sequence and proves that is a linear isometry extending .
Let and choose local sequences and . Since is bounded, [F9] gives ; [F8] gives the same estimate for . Because , limits prove multiplicativity. Also [F9] gives , while [F7] and give . Since , taking limits proves . The common unit is preserved on the dense union. Any other continuous extension agrees there and hence equals .
By [F3] the Fock space is nonzero, and under [A1] the creation and adjoint operators in [F4] give one of the stated CAR families. Applying the extension construction of steps 1.1, 2.1 and 3.1 to this family gives its representation of . Every such representation restricts on a finite stage to a unital representation of that matrix algebra, so [F2] makes its norm on each local element equal the stage norm. Thus the global family is nonempty and the supremum of represented norms equals the inductive-limit norm for every local element.
Remarks
The directed finite-dimensional CAR system and its finite-stage norms use finite-dimensional subspaces and finite orthonormal bases. The theorem retains Countable Choice for its completion and Hilbert/Fock construction context, including the bounded Hilbert adjoints in the Fock representation that witnesses nonemptiness of the global representation family. This is an abstract CAR C*-algebra statement and supplies no QFT locality or spin-statistics theorem.
Depends on
- CAR C*-Algebra over a Complex Hilbert Space
- Finite-Dimensional CAR Algebra over an Inner-Product Space
- Finite-Dimensional CAR over an Inner-Product Space Is a Matrix Algebra
- Finite-Subspace CAR Inclusions Are Isometric
- Fock Creation and Annihilation Operators Satisfy the CAR
- Fermionic Fock Space over a Complex Hilbert Space
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
- The Hilbert-space adjoint of a bounded operator
- Hilbert-adjoint identities
- If \(Y\) is Banach then \(\mathcal B(X,Y)\) is Banach
- The spaces \(\mathcal B(X,Y)\) and \(\mathcal B(X)\) of bounded linear operators
- The operator norm as the least bound and as the unit-sphere or unit-ball supremum
- Composition satisfies \|ST\|\le\|S\|\,\|T\|
- C star algebra
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
43 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Günther Hörmann, C*-Algebras with Aspects of Quantum Physics, Chapter 6, §§6.4 and 6.7 (standard reference, not scraped)
- Jan Dereziński, Introduction to Representations of the Canonical Commutation and Anticommutation Relations, §§4.1, 4.2 and 5.7 (standard reference, not scraped)