Local Nets, States, and Representations
Algebraic QFT assigns observables to spacetime regions before choosing a Hilbert-space representation. This chapter follows that distinction from local nets to states, local factors, and constructive examples.
Enter this chapter
Section titled “Enter this chapter”Read nets, quasilocal algebras, and GNS representations consecutively; the later topics depend on keeping the abstract algebra and its represented closure distinct. Helpful background. Operator Algebras and Positive Functionals supplies the C*-algebra, von Neumann algebra, and state vocabulary. Von Neumann Factors and Type-III Local Algebras previews the sharp-region consequence, and Local Field Algebras, Causality, and the Time-Slice Property shows how the same structure is deployed on globally hyperbolic spacetimes.
Topics
Section titled “Topics”- Haag–Kastler Nets and Locality — Defines a net and its causal compatibility conditions.
- Quasilocal C*-Algebras and Inductive Limits — Assembles local observables through compatible C*-algebra inclusions.
- States, GNS Representations, and Folia — Constructs representations from states and identifies their normal-state families.
- Local Normality, Quasiequivalence, and Folia — Compares representations locally without assuming global unitary equivalence.
- The Reeh–Schlieder Theorem — Explains the dense vacuum orbit of a local algebra.
- Isotony, Additivity, Duality, and Primitive Causality — Separates inclusion, completeness of local generation, duality, and dynamics.
- From Pointlike Fields to Nets and Affiliated Operators — Relates unbounded fields to bounded local observable algebras.
- Factorizing S-Matrices, Wedge-Local Fields, and Borchers Constructions — Builds wedge-local models and states the extra conditions for compact localization.
- Representation Types, Factors, and Local-Algebra Structure — Identifies what factor type says about a represented local algebra.
How the ideas fit together
Section titled “How the ideas fit together”A net specifies localization; a state supplies a representation through GNS. The norm-closed quasilocal algebra and the weak closures of represented local algebras answer different questions Haag and Kastler 1964, §§ 2–3. Local quasiequivalence does not imply a global unitary identification Fewster and Rejzner 2020, §§ 2.3 and 4–6 (PDF). Likewise, wedge locality needs further estimates before it yields nontrivial double-cone observables Lechner 2008, § 3 and Theorems 5.6, 5.8; identifying the precise local factor requires further structural hypotheses Buchholz, D’Antoni, and Fredenhagen 1987, pp. 126–134.
Hypotheses and licensed conclusions
Section titled “Hypotheses and licensed conclusions”| Object and domain | Required hypotheses | Licensed conclusion | Excluded converse or upgrade | Adversarial check |
|---|---|---|---|---|
| Regional C*-algebras on a directed family of double cones | Injective coherent inclusions; spacelike commutation and covariant region maps when those properties are claimed | An isotonic local net and its representation-independent quasilocal C*-completion | The construction is not a tensor product of sharp regions, and locality does not imply duality | Assign independent factors to nested or overlapping regions and find the missing inclusion or inconsistent overlap |
| Positive normalized functional on the quasilocal algebra | C*-positivity and normalization; invariance or KMS analyticity only when separately imposed | A cyclic GNS representation, with purity equivalent to irreducibility and a representation-dependent von Neumann closure | GNS does not supply locality, positive energy, faithfulness, or a density matrix in another representation | Write an infinite-volume thermal state as a vacuum-Fock Gibbs trace and expose the non-trace-class partition function |
| Two quasifree representations restricted to bounded local algebras | Equivalent induced topologies and regional Hilbert–Schmidt covariance difference; Hadamard hypotheses in the free curved-spacetime theorem | Equality of local folia and mutual normality on every stated bounded region | Local quasiequivalence does not produce a compatible global unitary or erase infrared phase differences | Let the region exhaust infinite volume and watch the thermal covariance difference fail the global Hilbert–Schmidt test |
| Vacuum representation and a nonempty open region | Positive translation spectrum, global cyclicity, weak additivity, covariance, and locality for the separating conclusion | The vacuum is cyclic locally and separating when the causal complement has nonempty interior | Orbit density gives no uniform operator norm, energy, success probability, or signaling protocol | Drive the approximation error to zero while recording norm and energy instead of assuming they remain bounded |
| Additive free-Maxwell net on a causally completed ring-like region | Specified contractible generators, region topology, causal complement, and the vacuum representation | Einstein causality survives while a linked flux gives a strict inclusion into the dual algebra | Commutation with the complement does not prove that an operator is generated in the original region | Compute the nonzero linking pairing of electric and magnetic fluxes on disjoint thickened tori |
| Smeared unbounded fields on a common invariant core | Closability, essential self-adjointness or controlled resolvents, support covariance, and strong spacelike commutativity | Spectral unitaries generate an isotonic local von Neumann net to which the closed fields are affiliated | A vanishing form commutator or an unclosable distribution does not license local exponentials | Change the self-adjoint extension or test spectral commutation beyond the proposed core |
| Scalar factorizing amplitude and its wedge algebra in two dimensions | Unitarity, hermitian analyticity, crossing, bounded physical-strip continuation, and modular nuclearity for compact localization | ZF operators give relatively wedge-local fields and, in the proved regular class, nontrivial local intersections; further scaling and phase-space input can fix factor type | A real-axis unitary phase is not a local QFT, and type III alone is not hyperfinite type III₁ | Remove strip analyticity so the wedge contour shift fails, or remove scaling control so the Connes type is undetermined |
Review the chapter
Section titled “Review the chapter”Does Reeh–Schlieder allow a local unitary to prepare any distant state?
Solution
No. Cyclicity concerns vectors obtained using arbitrary local operators and their limits, not only unitaries. A unitary in one region commutes with observables in a spacelike-separated region and leaves their expectation values unchanged.
Where to go next
Section titled “Where to go next”Continue to modular theory, nuclearity, and split inclusions to study finer structure of these represented local algebras.
References
Section titled “References”- Buchholz, Detlev, Claudio D’Antoni, and Klaus Fredenhagen. “The Universal Structure of Local Algebras.” Communications in Mathematical Physics 111 (1987): 123–135. DOI.
- Fewster, Christopher J., and Kasia Rejzner. “Algebraic Quantum Field Theory—an Introduction.” In Progress and Visions in Quantum Theory in View of Gravity, 1–61. Cham: Birkhäuser, 2020. DOI; Open PDF.
- Haag, Rudolf, and Daniel Kastler. “An Algebraic Approach to Quantum Field Theory.” Journal of Mathematical Physics 5 (1964): 848–861. DOI.
- Lechner, Gandalf. “Construction of Quantum Field Theories with Factorizing S-Matrices.” Communications in Mathematical Physics 277 (2008): 821–860. DOI; Open PDF.