Factorization Algebras and Local-to-Global Observables
Factorization algebras combine observables in disjoint regions and recover larger regions by descent. This chapter explains that local-to-global structure, its quantization, and the additional conditions needed for comparison with algebraic QFT.
Enter this chapter
Section titled “Enter this chapter”Start with disjoint structure maps, then Weiss descent. Ordinary sheaf gluing is a useful analogy but uses a different cover condition. Helpful background. Presheaves, sheaves, cosheaves, and Čech descent supplies the ordinary local-to-global language. Derived, higher, and factorization frameworks supplies homotopy colimits and higher coherence. From the local OPE to conformal data gives a physical comparison point without equating an OPE expansion with Weiss descent.
Topics
Section titled “Topics”- Prefactorization and Factorization Algebras — Defines disjoint-region products and their coherence.
- Weiss Descent and Local-to-Global Observables — Uses covers that contain every finite configuration in some member.
- Elliptic Complexes and Factorization Observables — Builds observable complexes from elliptic field data.
- Classical Observables and Poisson Factorization — Adds the classical Poisson structure to local observables.
- BV Quantization and Obstruction–Deformation Complexes — Treats quantization as an obstruction problem.
- Quantum Observables, Renormalization, and Factorization — Constructs renormalized quantum structure maps.
- Locally Constant Factorization Algebras and Eₙ Algebras — Identifies the extra local constancy behind Eₙ structures.
- Factorization Homology and Manifold Invariants — Integrates local algebraic data over manifolds.
- Holomorphic, Topological, and Mixed Factorization Theories — Distinguishes topological and holomorphic directions of dependence.
- Factorization Comparison Theorems and Their Limits — States comparison results with their exact analytic and categorical scope.
- AQFT to Prefactorization on Time-Orderable Covers — Constructs time-ordered prefactorization data from suitable Lorentzian nets.
- Prefactorization to AQFT: The Infinity-Categorical Converse Gap — Explains why a higher-categorical converse needs additional proof.
How the ideas fit together
Section titled “How the ideas fit together”Disjoint multiplication gives prefactorization; descent is a separate condition Costello and Gwilliam 2017, Chapters 2–3. Local constancy then licenses the Eₙ comparison Lurie 2017, Theorem 5.4.5.9 (PDF). In Lorentzian geometry, the AQFT comparison instead uses additivity, Cauchy constancy, and time-orderability Benini, Perin, and Schenkel 2020, Theorems 3.11, 4.7, and 5.1 (PDF). A cochain-level equivalence does not automatically add positive states or an operator-algebra completion.
Hypotheses and licensed conclusions
Section titled “Hypotheses and licensed conclusions”| Object and domain | Required hypotheses | Licensed result | Excluded converse or upgrade | Adversarial check |
|---|---|---|---|---|
| Assignment on opens | Symmetric monoidal target; coherent maps for finite disjoint families; unit and equivariance | Prefactorization algebra | Disjoint multiplication alone does not give local-to-global reconstruction | Add a class visible only on one large open and missed by every cover member |
| Prefactorization algebra on a manifold | Declared Weiss or factorizing covers; homotopically correct Čech object; suitable completion | Factorization algebra with derived local-to-global descent | Ordinary sheaf descent or underived colimits need not recover multilocal observables | Use a cover in which separated insertion points never occur together |
| Classical field complex | Elliptic Euclidean complex or Green-hyperbolic Lorentzian operator; support conditions; equation-of-motion quotient; wavefront domain where needed | Classical observable complex with the appropriate shifted BV or Peierls bracket | Ellipticity does not imply Lorentzian causality, and local functionals alone are not generally bracket-closed | Expose a zero mode, noncompact-support class, or forbidden wavefront product |
| Perturbative quantum observables | Gauge-fixed BV resolution; local renormalization; effective quantum master equation; vanishing or cancelled obstruction class | Quantum factorization algebra as a formal, scale-compatible deformation | No nonperturbative convergence, positive state, or regulator-independent completion follows | Compute a nonzero local anomaly class or introduce a nonlocal counterterm |
| Locally constant factorization algebra | Disk inclusions are weak equivalences; specified framing, orientation, or other tangential structure; presentable monoidal target | $E_n$ algebra and factorization homology by disk extension and excision | A generic metric-dependent QFT is not locally constant; an abstract $E_n$ algebra is not automatically a relativistic theory | Vary a mass-dependent correlator with disk size or transport framed data around an unlicensed rotation |
| Additive Cauchy-constant AQFT | Globally hyperbolic Lorentzian regions; Einstein causality; time-slice; time-orderable tuples; compatible monoidal target | Associated additive Cauchy-constant time-orderable prefactorization algebra | No Euclidean continuation, Weiss descent, positivity transfer, or BV model is supplied for free | Choose a causally cyclic tuple with no linear time order |
| Time-orderable prefactorization algebra | Additivity and Cauchy constancy in the proved strict setting; coherent multiplication reconstructed from Cauchy morphisms | Strict AQFT comparison and inverse functors in the stated one-category | The strict theorem does not establish the general infinity-categorical converse | Retain descent but remove time-slice or required higher coherence and test associativity |
Review the chapter
Section titled “Review the chapter”Can an ordinary open cover fail to be a Weiss cover?
Solution
Yes. Two disjoint nonempty components cover their union, but a finite subset containing one point in each component lies in neither member. Weiss descent tests finite configurations jointly, so ordinary pointwise coverage is insufficient.
Where to go next
Section titled “Where to go next”Continue to derived and deformation methods for the complexes and obstruction classes underlying perturbative quantization.
References
Section titled “References”- Benini, Marco, Marco Perin, and Alexander Schenkel. “Model-Independent Comparison between Factorization Algebras and Algebraic Quantum Field Theory on Lorentzian Manifolds.” Communications in Mathematical Physics 377 (2020): 971–997. DOI; Open PDF.
- Costello, Kevin, and Owen Gwilliam. Factorization Algebras in Quantum Field Theory, Volume 1. Cambridge: Cambridge University Press, 2017. DOI.
- Lurie, Jacob. Higher Algebra. September 18, 2017. Author PDF.