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Abstract Homotopy Theory Seminar
In the topological setting, a two dimensional quantum field theory of observables is given by a disk algebra. In the case where the category of modules has sufficient duality, it defines a 3-dimensional theory of states, given by a functor out of a cobordism category.
In the conformal or algebraic setting, a theory of observables is given instead by a holomorphic or algebraic factorization algebra. An algebraic quantum field theory, described first by Beilinson-Feigin-Mazur and reinterpreted by Ben Zvi-Sakellaridis-Venkatesh, is the structure expected on the [1,2] part of a corresponding 3d theory of states. In this talk I will describe a partial construction realizing such theory.