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String topology, a branch of
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, is the study of algebraic structures on the homology of free loop spaces. The field was started by .


Motivation

While the
singular cohomology In mathematics, specifically in homology theory and algebraic topology, cohomology is a general term for a sequence of abelian groups, usually one associated with a topological space, often defined from a cochain complex. Cohomology can be viewed ...
of a space has always a product structure, this is not true for the
singular homology In algebraic topology, singular homology refers to the study of a certain set of algebraic invariants of a topological space X, the so-called homology groups H_n(X). Intuitively, singular homology counts, for each dimension n, the n-dimensional ...
of a space. Nevertheless, it is possible to construct such a structure for an oriented
manifold In mathematics, a manifold is a topological space that locally resembles Euclidean space near each point. More precisely, an n-dimensional manifold, or ''n-manifold'' for short, is a topological space with the property that each point has a N ...
M of dimension d. This is the so-called
intersection product In mathematics, the intersection of two or more objects is another object consisting of everything that is contained in all of the objects simultaneously. For example, in Euclidean geometry, when two Line (geometry), lines in a Plane (geometr ...
. Intuitively, one can describe it as follows: given classes x\in H_p(M) and y\in H_q(M), take their product x\times y \in H_(M\times M) and make it transversal to the diagonal M\hookrightarrow M\times M. The intersection is then a class in H_(M), the intersection product of x and y. One way to make this construction rigorous is to use stratifolds. Another case, where the homology of a space has a product, is the (based)
loop space In topology, a branch of mathematics, the loop space Ω''X'' of a pointed topological space ''X'' is the space of (based) loops in ''X'', i.e. continuous pointed maps from the pointed circle ''S''1 to ''X'', equipped with the compact-open topolog ...
\Omega X of a space X. Here the space itself has a product :m\colon \Omega X\times \Omega X \to \Omega X by going first through the first loop and then through the second one. There is no analogous product structure for the free loop space LX of all maps from S^1 to X since the two loops need not have a common point. A substitute for the map m is the map :\gamma\colon (S^1 \lor S^1, M)\to LM where (S^1 \lor S^1, M) is the subspace of LM\times LM, where the value of the two loops coincides at 0 and \gamma is defined again by composing the loops.


The Chas–Sullivan product

The idea of the Chas–Sullivan product is to now combine the product structures above. Consider two classes x\in H_p(LM) and y\in H_q(LM). Their product x\times y lies in H_(LM\times LM). We need a map :i^!\colon H_(LM\times LM)\to H_((S^1 \lor S^1,M)). One way to construct this is to use stratifolds (or another geometric definition of homology) to do transversal intersection (after interpreting (S^1 \lor S^1, M) \subset LM\times LM as an inclusion of Hilbert manifolds). Another approach starts with the collapse map from LM\times LM to the
Thom space In mathematics, the Thom space, Thom complex, or Pontryagin–Thom construction (named after René Thom and Lev Pontryagin) of algebraic topology and differential topology is a topological space associated to a vector bundle, over any paracompact s ...
of the normal bundle of (S^1 \lor S^1, M). Composing the induced map in homology with the
Thom isomorphism In mathematics, the Thom space, Thom complex, or Pontryagin–Thom construction (named after René Thom and Lev Pontryagin) of algebraic topology and differential topology is a topological space associated to a vector bundle, over any paracompact sp ...
, we get the map we want. Now we can compose i^! with the induced map of \gamma to get a class in H_(LM), the Chas–Sullivan product of x and y (see e.g. ).


Remarks

*As in the case of the intersection product, there are different sign conventions concerning the Chas–Sullivan product. In some convention, it is graded commutative, in some it is not. *The same construction works if we replace H by another multiplicative
homology theory In mathematics, the term homology, originally introduced in algebraic topology, has three primary, closely-related usages. The most direct usage of the term is to take the ''homology of a chain complex'', resulting in a sequence of abelian grou ...
h if M is oriented with respect to h. *Furthermore, we can replace LM by L^n M = (S^n, M). By an easy variation of the above construction, we get that \mathcalh_*((N,M)) is a module over \mathcalh_*L^n M if N is a manifold of dimensions n. *The
Serre spectral sequence In mathematics, the Serre spectral sequence (sometimes Leray–Serre spectral sequence to acknowledge earlier work of Jean Leray in the Leray spectral sequence) is an important tool in algebraic topology. It expresses, in the language of homologica ...
is compatible with the above algebraic structures for both the
fiber bundle In mathematics, and particularly topology, a fiber bundle ( ''Commonwealth English'': fibre bundle) is a space that is a product space, but may have a different topological structure. Specifically, the similarity between a space E and a pr ...
\colon LM\to M with fiber \Omega M and the fiber bundle LE\to LB for a fiber bundle E\to B, which is important for computations (see and ).


The Batalin–Vilkovisky structure

There is an action S^1\times LM \to LM by rotation, which induces a map :H_*(S^1)\otimes H_*(LM) \to H_*(LM). Plugging in the fundamental class ^1in H_1(S^1), gives an operator :\Delta\colon H_*(LM)\to H_(LM) of degree 1. One can show that this operator interacts nicely with the Chas–Sullivan product in the sense that they form together the structure of a Batalin–Vilkovisky algebra on \mathcalH_*(LM). This operator tends to be difficult to compute in general. The defining identities of a Batalin-Vilkovisky algebra were checked in the original paper "by pictures." A less direct, but arguably more conceptual way to do that could be by using an action of a cactus operad on the free loop space LM. The cactus operad is weakly equivalent to the framed little disks operad and its action on a topological space implies a Batalin-Vilkovisky structure on homology.


Field theories

There are several attempts to construct (topological) field theories via string topology. The basic idea is to fix an oriented manifold M and associate to every surface with p incoming and q outgoing boundary components (with n\geq 1) an operation :H_*(LM)^ \to H_*(LM)^ which fulfills the usual axioms for a topological field theory. The Chas–Sullivan product is associated to the pair of pants. It can be shown that these operations are 0 if the genus of the surface is greater than 0 ().


References


Sources

* * * * * {{Cite journal, first=Hirotaka, last=Tamanoi, title=Loop coproducts in string topology and triviality of higher genus TQFT operations, journal=
Journal of Pure and Applied Algebra The ''Journal of Pure and Applied Algebra'' is a monthly peer-reviewed scientific journal covering that part of algebra likely to be of general mathematical interest: algebraic results with immediate applications, and the development of algebraic t ...
, volume= 214, issue=5, pages=605–615, year=2010, mr=2577666 , doi=10.1016/j.jpaa.2009.07.011, arxiv=0706.1276, s2cid=2147096 Geometric topology Algebraic topology String theory