Chiral algebra

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In mathematics, a chiral algebra is an algebraic structure introduced by Beilinson and Drinfeld (2004)[1] as a rigorous version of the rather vague concept of a chiral algebra in physics. In Chiral Algebras, Beilinson and Drinfeld introduced the notion of chiral algebra, which based on the pseudo-tensor category of D-modules. They give a 'coordinate independent' notion of vertex algebras, which are based on formal power series. Chiral algebras on curves are essentially conformal vertex algebras.

Definition

A chiral algebra[2] on a smooth algebraic curve X is a right D-module 𝒜, equipped with a D-module homomorphism μ:𝒜⊠𝒜(∞Δ)→Δ!𝒜 on X2 and with an embedding Ω↪𝒜, satisfying the following conditions

  • μ=−σ12∘μ∘σ12 (Skew-symmetry)
  • μ1{23}=μ{12}3+μ2{13} (Jacobi identity)
  • The unit map is compatible with the homomorphism μΩ:Ω⊠Ω(∞Δ)→Δ!Ω; that is, the following diagram commutes

Ω⊠𝒜(∞Δ)→𝒜⊠𝒜(∞Δ)↓↓Δ!𝒜→Δ!𝒜 Where, for sheaves ℳ,𝒩 on X, the sheaf ℳ⊠𝒩(∞Δ) is the sheaf on X2 whose sections are sections of the external tensor product ℳ⊠𝒩 with arbitrary poles on the diagonal: ℳ⊠𝒩(∞Δ)=lim→ℳ⊠𝒩(nΔ), Ω is the canonical bundle, and the 'diagonal extension by delta-functions' Δ! is Δ!ℳ=Ω⊠ℳ(∞Δ)Ω⊠ℳ.

Relation to other algebras

Vertex algebra

The category of vertex algebras as defined by Borcherds or Kac is equivalent to the category of chiral algebras on X=𝔸1 equivariant with respect to the group T of translations.

Factorization algebra

Chiral algebras can also be reformulated as factorization algebras.

See also

References

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Further reading


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