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Associative rings and algebras Definition

Koszul duality

Builds on FieldTensor algebraDual spaceKoszul algebra

Definition

Let kk be a field and let VV be a finite-dimensional vector space over kk, with dual space V∗V^*. Let R⊆V⊗VR \subseteq V \otimes V be a subspace. Let A=T(V)/(R)A = T(V)/(R) be the quotient of the tensor algebra by the two-sided ideal generated by RR; such an AA is a quadratic algebra. Identify V∗⊗V∗V^* \otimes V^* with (V⊗V)∗(V \otimes V)^*, and let R⊥⊆V∗⊗V∗R^\perp \subseteq V^* \otimes V^* be the set of forms that vanish on RR. The quadratic dual of AA is A!=T(V∗)/(R⊥)A^! = T(V^*)/(R^\perp). Koszul duality is the correspondence A↔A!A \leftrightarrow A^! between Koszul algebras, together with the induced relations between their module categories.

Remarks

The construction is an involution: (A!)!≅A(A^!)^! \cong A, because (R⊥)⊥=R(R^\perp)^\perp = R in finite dimension. If AA is Koszul, then A!A^! is Koszul, and the algebra Ext⁡A∙(k,k)\operatorname{Ext}^\bullet_A(k, k) is isomorphic to A!A^! (some conventions give the opposite algebra). For Koszul AA the Hilbert series satisfy hA(t) hA!(−t)=1h_A(t) \, h_{A^!}(-t) = 1. Example: let A=S(V)A = S(V) be the symmetric algebra, so RR is spanned by the tensors x⊗y−y⊗xx \otimes y - y \otimes x. A form on V⊗VV \otimes V vanishes on RR exactly when it is symmetric, so R⊥R^\perp is the space of symmetric tensors, spanned by the tensors ξ⊗ξ\xi \otimes \xi and ξ⊗η+η⊗ξ\xi \otimes \eta + \eta \otimes \xi. Hence A!=Λ(V∗)A^! = \Lambda(V^*) is the exterior algebra, and hA(t)=(1−t)−nh_A(t) = (1 - t)^{-n}, hA!(−t)=(1−t)nh_{A^!}(-t) = (1 - t)^n for n=dim⁡Vn = \dim V.

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  1. Dual space concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Koszul_duality
About this page
TagYX0J6TVGZ8
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Kinddefinition
WritingW0 stub
MSC16S37
DefinesKoszul duality
UsesField, Tensor algebra, Dual space, Koszul algebra
Changed2 November 2026

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