nLab derived loop space

Redirected from "derived loop spaces".
Contents

Context

Higher geometry

Mapping space

Contents

Idea

A derived loop space is a free loop space object in derived geometry.

Definition

Let TT be an (∞,1)-algebraic theory and CTAlg opC \subset T Alg_\infty^{op} an (∞,1)-site of formal duals of \infty-algebras over TT. Then the (∞,1)-topos H=(,1)Sh(C)\mathbf{H} = (\infty,1) Sh(C) encodes derived geometry modeled on TT.

A derived loop space is a free loop space object in such H\mathbf{H}.

More specifically, if TT is an ordinary Lawvere theory, regarded as a 1-truncated (,1)(\infty,1)-theory, then TAlg T Alg_{\infty} are its simplicial algebras. There is a canonical embedding TAlg opTAlg opT Alg^{op} \hookrightarrow T Alg_\infty^{op} of the ordinary algebras into the \infty-algebras, so that we may regard XTAlg opX \in T Alg^{op} as an object of H\mathbf{H}. Then the derived loop space of XX is its free loop space object computed in H\mathbf{H}.

The point is that the derived loop space of an ordinary XTAlg opX \in T Alg^{op} in general is a significantly richer object than the free loop space object of XX as computed just in the underived (,1)(\infty,1)-topos (,1)Sh(TAlg op)(\infty,1)Sh(T Alg^{op}). In fact, since XX is 0-truncated in (,1)Sh(TAlg op)(\infty,1)Sh(T Alg^{op}), it coincides with its free loop space object there, but the derived loop space does not.

Function complexes on derived loop spaces: Hochschild homology

The function complex on the derived loop space X\mathcal{L}X is the Hochschild homology complex of C(X)C(X). See there for further details. In particular see the section Hochschild cohomology – As function algebra on the derived loop space.

Also see free loop space object for more information.

References

Using Toën’s theory of function algebras on ∞-stacks for showing that the function complex on a derived loop space X\mathcal{L}X is, under mild conditions, the Hochschild homology complex of XX hence by Hochschild-Kostant-Rosenberg theorem the collection of Kähler differential forms on XX, and that the functions on X\mathcal{L}X that are invariant under the canonical S 1S^1-action on X\mathcal{L}X are the closed forms (this also gives a geometric interpretation of the old observation by Maxim Kontsevich and others, that the differential and grading on the de Rham complex may be understood as induced from automorphisms of the odd line):

Last revised on May 12, 2026 at 12:49:32. See the history of this page for a list of all contributions to it.