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In this chapter, we will discuss the (infinite-dimensional) geometric framework for rough paths and their signature. Rough path theory originated in the 1990s with the work of T. Lyons. It seeks to establish a theory of integrals and differential equations driven by rough signals. For example, one is interested in controlled ordinary differential equations driven by a rough signal. Here, a rough signal is a Hölder continuous path of potentially low Hölder regularity. Numerical methods for equations with more regularity suggest that iterated integrals of the rough signal against itself are needed to construct solutions. However due to Youngs theorem, these iterated integrals do not exist. To compensate this problem, the notion of a rough path was developed. After a qucik introduction to the theory of rough paths, we shall see that rough paths of various flavours can be understood as certain continuous paths taking values in infinite-dimensional Lie groups. The main focus of the chapter is to present an introduction to this geometric side of the theory.
In this paper we extend the computation of the the typical curves of algebraic K-theory done by Lars Hesselholt and Ib Madsen to general tensor algebras. The models used allow us to determine the stages of the Taylor tower of algebraic K-theory as a functor of augmented algebras, as defined by Tom Goodwillie, when evaluated on derived tensor algebras.
For R a discrete ring, and M a simplicial R-bimodule, we let R(M) denote the (derived) tensor algebra of M over R, and πR denote the ring of formal (derived) power series in M over R. We define a natural transformation of functors of simplicial R-bimodules Φ: which is closely related to Waldhausen's equivalence We show that Φ induces an equivalence on any finite stage of Goodwillie's Taylor towers of the functors at any simplicial bimodule. This is used to show that there is an equivalence of functors , and for connected bimodules, also an equivalence
We prove that two quiver operator algebras can be isometrically isomorphic only if the quivers (=directed graphs) are isomorphic. We also show how the graph can be recovered from certain representations of the algebra.
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