Nonhomogeneous quadratic duality and curvature

By L. Positselski. 2014

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A quadratic algebra is a graded algebra with generators of degree 1 and relations of degree 2. Let A be a quadratic algebra with the space of generators V and the space of relations I ⊂ V ⊗ V . The classical quadratic duality assigns the quadratic algebra A with generators from V ∗ and the relations I ⊂ V ∗ ⊗ V ∗ to the algebra A. According to the classical results of Priddy and Löfwall [1, 3], A is isomorphic to the subalgebra of Ext∗A(k, k) generated by Ext 1 A(k, k). Priddy called an algebra A a Koszul algebra if this subalgebra coincides with the whole of Ext∗A(k, k). Koszul algebras constitute a wonderful class of quadratic algebras, which is closed under a large set of operations, contains the main examples, and perhaps admits a finite classification. In this paper, we propose an extension of the quadratic duality to the nonhomogeneous case. Roughly speaking, a nonhomogeneous quadratic algebra (or a quadratic-linear-scalar algebra, a QLS-algebra) is an algebra defined by (generators and) nonhomogeneous relations of degree 2. A quadratic-linear algebra (QL-algebra) is an algebra defined by nonhomogeneous quadratic relations without the scalar parts; in other words, it is an augmented QLS-algebra. The precise definition takes into account the fact that a collection of nonhomogeneous relations does not necessarily “make sense” (its coefficients must satisfy some equations; the Jacobi identity is a classical example). The dual object for a QL-algebra is [6] a quadratic DG-algebra [7]. The dual object for a QLS-algebra is a set of data which we call a quadratic CDG-algebra (“curved”), defined up to an equivalence. The classical Poincaré–Birkhoff–Witt theorem on the universal enveloping algebra structure [9] finds its natural place in this context as a particular case of the fact that every Koszul CDG-algebra corresponds to a QLS-algebra. Remarkable examples of nonhomogeneous quadratic duality are provided by Differential Geometry. The algebra of differential operators on a manifold may be considered as a QL-algebra defined by the commutation relations for the vector fields. The dual object for this algebra is the de Rham complex; the corresponding equivalence of the categories of modules is constructed in [4]. The algebra of differential operators in a vector bundle is a QLS-algebra. The dual object is the algebra of differential forms with coefficients in linear operators in this bundle and with the exterior differential defined by means of a connection. Its square is not zero—it is equal to the commutator with the curvature; the equivalence relation mentioned in the previous paragraph corresponds to changing the connection. Thus, the curvature corresponds to the scalar part of the relations. A question arises about the obstructions to existence of a QL-algebra structure (i.e., of “a flat connection”) on a given QLS-algebra. In the present paper we construct obstructions of this kind generalizing the Chern classes of vector bundles [8] and (which is less evident) the Chern–Weil classes of principal G-bundles. Our analogues of the secondary characteristic classes [5] form the Chern–Simons functor on the category of CDG-algebras.

Subfields: Algebra and Number Theory, Mathematical Physics

View Paper: https://www.semanticscholar.org/paper/e81ee996d4e0ac2ceee5dd412149c3154c114713

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In Algebra and Number Theory

  1. Alexander Polishchuk
  2. Joan Millès
  3. Joseph Hirsh
  4. L. Positselski
  5. Michel van den Bergh
  6. I. Burban
  7. Alexander I. Efimov
  8. D. Pomerleano

In Mathematical Physics

  1. Alexander Polishchuk
  2. L. Positselski
  3. Joan Millès
  4. Joseph Hirsh
  5. D. Pomerleano
  6. Kevin Lin
  7. Alexander I. Efimov
  8. Yuri I. Manin

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