factorization algebra


Higher algebra

Quantum field theory



A factorization algebra is an algebra over an operad where the operad in question is like the little disk operad, but with each disk embedded into a given manifold XX.

This way a factorization algebra is an assignment of a chain complex V DV_D to each ball DXD \subset X embedded in XX, and for each collection of non-intersecting embedded balls D 1,,D nDXD_1 , \cdots, D_n \subset D \subset X sitting inside a bigger embedded ball DD in XX a morphism

V D 1V D 2V D nV D V_{D_1} \otimes V_{D_2} \otimes \cdots \otimes V_{D_n} \to V_{D}

such that composition of such operations is suitably respected.


Prefactorization algebra


For XX a topological space write Fact XFact_X be the colored operad in Set whose

  • objects are the connected open subsets of XX;

  • the hom-set Fact X({U i} i,V)Fact_X(\{U_i\}_i, V) is the singleton precisely if the U iU_i are all in VV and are pairwise disjoint and is the empty set otherwise.

This specifies composition uniquely.


For (C,)(C, \otimes) a symmetric monoidal abelian category let End(C)End(C) be its endomorphism operad. A prefactorization algebra on XX with values in CC is an algebra over an operad over Fact XFact_X in CC, hence a morphism of operads

:Fact XEnd(C). \mathcal{F} : Fact_X \to End(C) \,.

These definitions appear (here).

Factorization algebras


For XX a topological space and UXU \subset X an open subset, a open cover {U iU} iI\{U_i \hookrightarrow U\}_{i \in I} is called a factorizing cover if for every finite set of points {x 1,,x k}U\{x_1, \cdots, x_k\} \subset U there is a finite subset {U i j} jJI\{U_{i_j}\}_{j \in J \subset I} of pairwise disjoint open subsets such that each point is contained in their union.


Every Hausdorff space admits a factorizing cover.


For a factorizing cover {U iU} iI\{U_i \to U\}_{i \in I} write PIP I for the set of finite subsets αI\alpha \subset I such that for j,jαj,j' \in \alpha we have U jU j=U_j \cap U_{j'} = \emptyset.

Given a prefactorization algebra \mathcal{F} and αPI\alpha \in P I write

(α):= jαF(U j) \mathcal{F}(\alpha) := \otimes_{j \in \alpha} F(U_j)

and for α 1,,α kPI\alpha_1, \cdots, \alpha_k \in P I write

(α 1,,α k)= (j 1,,j k)α 1××α k(U j 1U j k). \mathcal{F}(\alpha_1, \cdots, \alpha_k) = \bigotimes_{(j_1, \cdots, j_k) \in \alpha_1 \times \cdots \times \alpha_k} \mathcal{F}(U_{j_1} \cap \cdots \cap U_{j_k}) \,.

For each 1ik1 \leq i \leq k there is a canonical morphism

p i:(α 1,,α k)(α 1,,α i1,α i+1,,α k). p_i : \mathcal{F}(\alpha_1,\cdots, \alpha_k) \to \mathcal{F}(\alpha_1, \cdots, \alpha_{i-1}, \alpha_{i+1}, \cdots, \alpha_k) \,.

A prefactorization algebra :Fact XEnd(C)\mathcal{F} : Fact_X \to End(C) is called a factorization algebra if for every open subset UXU \subset X and every factorizing cover {U iU} iI\{U_i \to U\}_{i \in I} the sequence

α 1,α 2PI(α 1,α 2)p 1p 2 βPI(β)(U)0 \bigoplus_{\alpha_1, \alpha_2 \in P I} \mathcal{F}(\alpha_1, \alpha_2) \stackrel{p_1 - p_2}{\to} \bigoplus_{\beta \in P I} \mathcal{F}(\beta) \to \mathcal{F}(U) \to 0

is an exact sequence.

These definitions appear here.

See also at cosheaf.

Homotopy factorization algebras

Let now (C,)(C,\otimes) specifically be a category of chain complexes.


A [prefactorization algebra] :Fact XEnd(X)\mathcal{F} : Fact_X \to End(X) is a homotopy factorization algebra if for all factorizing covers {U iUX} iI\{U_i \to U \subset X\}_{i \in I} the canonical morpshim

k0 α 1,,α kPI(α 1,,α k)[k1](U) \bigoplus_{k \geq 0} \bigoplus_{\alpha_1, \cdots, \alpha_k \in P I} \mathcal{F}(\alpha_1, \cdots, \alpha_k)[k-1] \to \mathcal{F}(U)

is a quasi-isomorphism, where the differential on the left is defined by (…).


This is the analogue of a descent condition for simplicial presheaves.

These definitions appear here.


Factorization algebras have some similarity with

duality between algebra and geometry in physics:

Poisson algebraPoisson manifold
deformation quantizationgeometric quantization
algebra of observablesspace of states
Heisenberg pictureSchrödinger picture
higher algebrahigher geometry
Poisson n-algebran-plectic manifold
En-algebrashigher symplectic geometry
BD-BV quantizationhigher geometric quantization
factorization algebra of observablesextended quantum field theory
factorization homologycobordism representation


The notion of factorization algebra may be regarded as a slight variation on the concept chiral algebra originally introduced in

A definition formulated genuinely in Higher Algebra appears in section 4.1 Topological Chiral Homology of

This discusses how locally constant factorization algebras obtained from En-algebras induce extended FQFTs.

A fairly comprehensive account of factorization algebras as a formalization of perturbative quantum field theory (see at factorization algebra of observables) is in

and the beginning of

Lecture notes include

There seems to be a close relation between the description of quantum field theory by factorization algebras and the proposal presented in

The relation of locally constant factorization algebras to higher order Hochschild homology is in

  • Gregory Ginot, Thomas Tradler, Mahmoud Zeinalian, Derived higher Hochschild homology, topological chiral homology and factorization algebras, arxiv/1011.6483

An (infinity,1)-category theoretic treatment of higher factorization algebras is in

A higher-dimensional generalization of vertex algebras is suggested in the framework of factorization algebras in

We introduce categories of weak factorization algebras and factorization spaces, and prove that they are equivalent to the categories of ordinary factorization algebras and spaces, respectively. This allows us to define the pullback of a factorization algebra or space by an 'etale morphism of schemes, and hence to define the notion of a universal factorization space or algebra. This provides a generalization to higher dimensions and to non-linear settings of the notion of a vertex algebra.

Revised on August 30, 2016 10:20:21 by Zoran Škoda (