nLab string topology

Context

Topology

topology (point-set topology, point-free topology)

see also differential topology, algebraic topology, functional analysis and topological homotopy theory

Introduction

Basic concepts

Universal constructions

Extra stuff, structure, properties

Examples

Basic statements

Theorems

Analysis Theorems

topological homotopy theory

Higher algebra

Contents

Idea

In string topology one studies the BV-algebra-structure on the ordinary homology of the free loop space X S 1X^{S^1} of an oriented manifold XX, or more generally the framed little 2-disk algebra-structure on the singular chain complex. This is a special case of the general algebraic structure on higher order Hochschild cohomology, as discussed there.

The study of string topology was initated by Moira Chas and Dennis Sullivan.

The string operations

Let XX be a smooth manifold, write LXL X for its free loop space (for XX regarded as a topological space) and H (LX)H_\bullet(L X) for the ordinary homology of this space (with coefficients in the integers \mathbb{Z}).

The string product

Definition

The string product is a morphism of abelian groups

()():H (LX)H (LX)H dimX(LX) (-)\cdot(-) \;\colon\; H_\bullet(L X) \otimes H_\bullet(L X) \longrightarrow H_{\bullet - dim X}(L X)

(where dimXdim X is the dimension of XX), defined as follows:

Write ev *:LXXev_* \colon L X \to X for the evaluation map at the basepoint of the loops.

For [α]H i(LX)[\alpha] \in H_i(L X) and [β]H j(LX)[\beta] \in H_j(L X) we can find representatives α\alpha and β\beta such that ev(α)ev(\alpha) and ev(β)ev(\beta) intersect transversally. There is then an ((i+j)dimX)\big((i+j)-dim X\big)-chain αβ\alpha \cdot \beta such that ev(αβ)ev(\alpha \cdot \beta) is the chain given by that intersection: above xev(αβ)x \in ev(\alpha \cdot \beta) this is the loop obtained by concatenating α x\alpha_x and β x\beta_x at their common basepoint. The string product is then defined using such representatives by

[α][β][αβ]. [\alpha] \cdot [\beta] \coloneqq [\alpha \cdot \beta] \,.
Theorem

The string product is associative and graded-commutative.

This is due to Chas & Sullivan. There is is a more elegant way to capture this, due to Cohen & Jones:

Let

S 1S 18S 1 S^1 \coprod S^1 \to 8 \leftarrow S^1

be the cospan that exhibts the inner and the outer circle of the figure “8” topological space. By forming hom spaces this induces the span

X 8 in out LX×LX LX. \array{ && X^8 \\ & {}^{\mathllap{in}}\swarrow && \searrow^{\mathrlap{out}} \\ L X \times L X &&&& L X } \,.

Write in !in^! for the “pullback” in ordinary homology along inin (the dual fiber integration) and out *out_* for the ordinary pushforward.

Theorem

The string product is the pull-push operation

out *in !:H (LX×LX)H (LX)H (LX)H dimX(LX). out_* \circ in^! : H_\bullet(L X \times L X) \simeq H_\bullet(L X) \otimes H_\bullet(L X) \to H_{\bullet - dim X}(L X) \,.

This is due to Cohen & Jones.

The BV-operator

Definition

Define a morphism of abelian groups

Δ:H (LX)H +1(LX) \Delta : H_\bullet(L X) \to H_{\bullet + 1}(L X)

as follows. Consider first the rotation map

ρ:S 1×LXLX \rho : S^1 \times L X \to L X

that sends (θ,γ)(tγ(θ+t))(\theta, \gamma) \mapsto (t \mapsto \gamma(\theta + t)). Then take

Δ:aρ *([S 1]×a), \Delta \colon a \mapsto \rho_* \big([S^1] \times a\big) \,,

where [S 1]H 1(S 1)[S^1] \in H_1(S^1) is the fundamental class of the circle.

This is called the BV-operator for string topology.

Proposition

The Goldman bracket on H 0(LX)H_0(L X) is equivalent to the string product applied to the image of the BV-operator

{[γ 1],[γ 2]}=Δ[Γ 1]Δ[Γ 2]. \{[\gamma_1], [\gamma_2]\} = \Delta[\Gamma_1] \cdot \Delta[\Gamma_2] \,.

This is due to Chas & Sullivan.

Properties

As a TQFT

The structures studied in the string topology of a smooth manifold XX may be understood as being essentially the data of a 2-dimensional topological field theory sigma model with target space XX, or rather its linearization to an HQFT (with due care on some technical subtleties).

The idea is that the configuration space of a closed or open string-sigma-model propagating on XX is the loop space or path space of XX, respectively. The space of states of the string is some space of sections over this configuration space, to which the (co)homology H (LX)H_\bullet(L X) is an approximation. The string topology operations are then the cobordism-representation with coefficients in the category of chain complexes

H (Bord 2)Ch H_\bullet(Bord_2) \to Ch_\bullet

given by the FQFT corresponding to the σ\sigma-modelon these state spaces, acting on these state spaces.

,\,,

Let XX be an oriented compact manifold of dimension dd.

For ={A,B,}\mathcal{B} = \{A, B , \cdots\} a collection of oriented compact submanifolds write P X(A,B)P_X(A,B) for the path space of paths in XX that start in AXA \subset X and end in BXB \subset X.

Theorem

The tuple (H (LM,),{H (P X(A,B),)} A,B)(H_\bullet(L M, \mathbb{Q}), \{H_\bullet(P_X(A,B), \mathbb{Q})\}_{A,B \in \mathcal{B}}) carries the structure of a dd-dimensional HCFT with positive boundary and set of branes \mathcal{B}, such that the correlators in the closed sector are the standard string topology operation.

For closed strings this is discussed by Cohen & Godin 2003, Tamanoi 2007. For open strings on a single space-filling brane, ={X}\mathcal{B} = \{ X \} this was shown by Godin 2007, where the general statement for arbitrary branes is conjectured. A detailed proof of this general statement is given by Kupers 2011.

Remark

These constructions work by regarding the mapping spaces from 2-dimensional cobordisms with maps to the base space as correspondences and then applying pull-push (pullback followed by push-forward in cohomology/Umkehr maps) to these. Hence these quantum field theory realizations of string topology may be thought of as arising from a quantization process of the form path integral as a pull-push transform/motivic quantization.

Example

(open string product on 0-brane is Pontrjagin product)
For the case of a single brane being a 0-brane, hence a point {x}X\{x\} \hookrightarrow X, then:

  1. the open string configuration spaces is the based loop space P(x,x)=Ω xXP(x,x) = \Omega_x X,

  2. whence the homology is the homology of loop spaces H (Ω xX)H_\bullet(\Omega_x X), and

  3. the open string product coincides with the Pontrjagin product,

    (1)(conc x) *:H (ΩX)H (ΩX)H (ΩX), (conc_x)_\ast \colon H_\bullet(\Omega X) \otimes H_\bullet(\Omega X) \longrightarrow H_\bullet(\Omega X) \mathrlap{\,,}

    given simply by pushforward in homology along the loop concatenation map

    (2)conc x:Ω xX×Ω xXlongrightarrpwΩ xX. conc_x \colon \Omega_x X \times \Omega_x X \longrightarrpw \Omega_x X \mathrlap{\,.}

(Sullivan 2005 SFT, Ex. 3)
Proof

The first two statements are immediate from the definitions. The third statement is a special case of the explicit formula for the open string product μ a,b,c\mu_{a,b,c} (here: μ x,x,x\mu_{x,x,x}) given in Kupers 2011 p. 137:

In our case of a 0-brane, the map denoted “M iM^i” there (on the previous p. 136), is an isomorphism, and the map “M jM^j” there (beware the typo in the orientation of the arrow) becomes the loop concatenation operation conc xconc_x (2), whence the formula for the string product reduces to the Pontrjagin product (1):

μ x,x,x (M j) *(M i) ! (conc x) *(id) ! (conc x) *. \begin{aligned} \mu_{x,x,x} & \coloneqq (M^j)_\ast \circ (M^i)^! \\ & \equiv (conc_x)_\ast \circ (id)^! \\ & \simeq (conc_x)_\ast \mathrlap{\,.} \end{aligned}

References

General

Original references:

Exposition:

  • Ralph Cohen: Homotopy and geometric perspectives on string topology (2005) [pdf, pdf]

Realizing the string product as a pull-push (in terms of dual fiber integration via Thom isomorphism):

More on relation to homology of the based loop space and its Pontrjagin product:

On string topology operations in the generality of (the homology of loop spaces of) Poincaré duality spaces:

Refinements of string topology from homology groups to the full ordinary homology-spectra:

Further generalization to target spaces that need not be compact and moreover may be differentiable stacks/Lie groupoids:

On therelation between string topology and Hochschild cohomology:

Specifically on string topology of n-spheres (in particular on the ordinary homology of free loop spaces of n-spheres):

As a TQFT

The interpretation of closed string topology as an HQFT:

The open-closed HQFT in the presence of a single space-filling brane:

The generalization to multiple branes:

Exposition of the perspective of regarding string topology-operations as the TQFT of a topological string sigma model:

For target space the classifying space BGB G of a compact Lie group GG (such as a finite group):

Arguments that this string-topology HQFT should refine to a chain-level theory – a TCFT:

For the string product and the BV-operator this extension has been known early on, it yields a homotopy BV algebra considered in

  • Scott Wilson, around page 101 of: On the Algebra and Geometry of a Manifold’s Chains and Cochains (2005) (pdf)

Evidence for the existence of the TCFT version by exhibiting a dg-category that looks like it ought to be the dg-category of string-topology branes (hence ought to correspond to the TCFT under the suitable version of the TCFT-version of the cobordism hypothesis) is discussed in

Last revised on November 14, 2025 at 17:19:43. See the history of this page for a list of all contributions to it.