Factorization algebra

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Short description: Algebraic structure in mathematical physics

In mathematics and mathematical physics, a factorization algebra is an algebraic structure first introduced by Beilinson and Drinfel'd in an algebro-geometric setting as a reformulation of chiral algebras,[1] and also studied in a more general setting by Costello to study quantum field theory.[2]

Definition

Prefactorization algebras

A factorization algebra is a prefactorization algebra satisfying some properties, similar to sheafs being a presheaf with extra conditions.

If M is a topological space, a prefactorization algebra of vector spaces on M is an assignment of vector spaces (U) to open sets U of M, along with the following conditions on the assignment:

  • For each inclusion UV, there's a linear map mVU:(U)(V)
  • There is a linear map mVU1,,Un:(U1)(Un)(V) for each finite collection of open sets with each UiV and the Ui pairwise disjoint.
  • The maps compose in the obvious way: for collections of opens Ui,j, Vi and an open W satisfying Ui,1Ui,niVi and V1VnW, the following diagram commutes.

ij(Ui,j)i(Vi)(W)

So resembles a precosheaf, except the vector spaces are tensored rather than (direct-)summed.

The category of vector spaces can be replaced with any symmetric monoidal category.

Factorization algebras

To define factorization algebras, it is necessary to define a Weiss cover. For U an open set, a collection of opens 𝔘={Ui|iI} is a Weiss cover of U if for any finite collection of points {x1,,xk} in U, there is an open set Ui𝔘 such that {x1,,xk}Ui.

Then a factorization algebra of vector spaces on M is a prefactorization algebra of vector spaces on M so that for every open U and every Weiss cover {Ui|iI} of U, the sequence i,j(UiUj)k(Uk)(U)0 is exact. That is, is a factorization algebra if it is a cosheaf with respect to the Weiss topology.

A factorization algebra is multiplicative if, in addition, for each pair of disjoint opens U,VM, the structure map mUVU,V:(U)(V)(UV) is an isomorphism.

Algebro-geometric formulation

While this formulation is related to the one given above, the relation is not immediate.

Let X be a smooth complex curve. A factorization algebra on X consists of

  • A quasicoherent sheaf 𝒱X,I over XI for any finite set I, with no non-zero local section supported at the union of all partial diagonals
  • Functorial isomorphisms of quasicoherent sheaves ΔJ/I*𝒱X,J𝒱X,I over XI for surjections JI.
  • (Factorization) Functorial isomorphisms of quasicoherent sheaves

jJ/I*𝒱X,JjJ/I*(iI𝒱X,p1(i)) over UJ/I.

  • (Unit) Let 𝒱=𝒱X,{1} and 𝒱2=𝒱X,{1,2}. A global section (the unit) 1𝒱(X) with the property that for every local section f𝒱(U) (UX), the section 1f of 𝒱2|U2Δ extends across the diagonal, and restricts to f𝒱𝒱2|Δ.

Example

Associative algebra

Any associative algebra A can be realized as a prefactorization algebra Af on . To each open interval (a,b), assign Af((a,b))=A. An arbitrary open is a disjoint union of countably many open intervals, U=iIi, and then set Af(U)=iA. The structure maps simply come from the multiplication map on A. Some care is needed for infinite tensor products, but for finitely many open intervals the picture is straightforward.

See also

  • Vertex algebra

References

  1. Beilinson, Alexander; Drinfeld, Vladimir (2004). Chiral algebras. Providence, R.I.: American Mathematical Society. ISBN 978-0-8218-3528-9. https://books.google.com/books?id=yHZh3p-kFqQC. Retrieved 21 February 2023. 
  2. Costello, Kevin; Gwilliam, Owen (2017). Factorization algebras in quantum field theory, Volume 1. Cambridge. ISBN 9781316678626.