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Configuration Spaces in Algebraic Topology: Lecture 1 CONFIGURATION SPACES IN ALGEBRAIC TOPOLOGY: LECTURE 1 BEN KNUDSEN This course is concerned with the study of the following spaces. Definition (Configuration spaces). The configuration space of k ordered points in the topological space X is k Confk(X) := f(x1; : : : ; xk) 2 X : xi 6= xj if i 6= jg; endowed with the subspace topology. The unordered configuration space is the quotient Bk(X) := Confk(X)=Σk: Remark. We warn the reader that, in the literature on configuration spaces, there are almost as many traditions of notation as there are references. Our goal is to attempt to understand the topology of these spaces, in the case that X is a manifold or nearly so, through the lens of homotopy groups and (co)homology. Before beginning our study in earnest, we first mention a few reasons that configuration spaces are particularly interesting objects of study. Perspective (Invariants). The homotopy type of a fixed configuration space is a homeomor- phism invariant of the background space, and, in the case of a manifold, it turns out that these invariants remember a rather large amount of information. A simple-minded example is pro- vided by Euclidean spaces of different dimension; indeed, as we will see, there is a homotopy m n equivalence B2(R ) ' B2(R ) if and only if m = n. In other words, configuration spaces are sensitive to the dimension of a manifold. 2 2 0 A somewhat more sophisticated example is provided by the fact that B2(T npt) 6' B2(R nS ), which can be shown by a homology calculation. Note that T 2 n pt and R2 n S0 have the same dimension and homotopy type, having S1 _ S1 as a common deformation retract. On the other hand, (T 2 n pt)+ =∼ T 2 6' S1 _ S1 _ S2 ' (R2 n S0)+, so we might conclude from this example that configuration spaces are sensitive to the proper homotopy type of a manifold. In order to discuss the most striking illustration of the sensitivity of configuration spaces, we recall that the Lens spaces are a family of compact 3-manifolds given by 3 L(p; q) := S =Cp; 3 2 2πi=p 2πiq=p where the cyclic group Cp acts on S ⊆ C by multiplication by (e ; e ). It is a classical theorem of Reidemeister that 2 L(p; q1) ' L(p; q2) () q1q2 ≡ ±n mod p ∼ ±1 L(p; q1) = L(p; q2) () q1 ≡ ±q2 mod p: In particular, L(7; 1) and L(7; 2) are homotopy equivalent but not homeomorphic, and, according to a theorem of Longoni-Salvatore [LS05], their configuration spaces distinguish them. Thus, configuration spaces are sensitive at least to the simple homotopy type of a manifold. Date: 30 August 2017. 1 2 BEN KNUDSEN 2 Perspective (Braids). A point moving in Bk(R ) traces out k different paths that weave among one another but can never overlap. For this reason, we think of the fundamental group 2 π1(Bk(R )) as the group of geometric braids on k strands, with composition given by concate- nation of braids. As we shall see, this braid group admits the remarkably simple presentation 2 ∼ π1(Bk(R )) = hσ1; : : : ; σk−1 j σiσi+1σi = σi+1σiσi+1; σiσj = σjσi if ji − jj > 1i; due originally to Artin [Art47]. The combinatorial, algebraic, and geometric properties of these and related braid groups are of fundamental importance to a vast swath of mathematics that encompasses knot theory, mapping class groups [Bir75], quantum groups [Kas95], category theory [JS86], and motion planning [Far17]. Perspective (Embeddings). In the company of manifolds with trivialized tangent bundles, it is possible to speak of a framed embedding, which is to say an embedding respecting the fixed trivialization, possibly up to a homotopy through bundle maps. The tangent bundle of any Euclidean space is canonically trivialized, and evaluation at the origin determines a homotopy equivalence fr n n ∼ n Emb (qkR ; R ) −! Confk(R ): As a consequence of this observation and the fact that framed embeddings compose, we see that n the collection fConfk(R )gk≥0 of homotopy types is equipped with hidden algebraic structure. This algebraic structure is that of an operad, which goes by the name of En. This perspective has many important consequences, three of which we name. (1) Iterated loop spaces. For any X, there is a collection of maps fr n n n k n Emb (qkR ; R ) × (Ω X) ! Ω X; which arise from a particularly simple variant of the Pontrjagin-Thom collapse construc- tion. The compatibilities among these maps are summarized by saying that ΩnX is an n En-algebra; in particular, the homology groups of the configuration spaces of R encode n algebraic operations on H∗(Ω X). Remarkably, there is also a partial converse, often called May's recognition principle [May72], which amounts to an algebraic classification of n-fold loop spaces. (2) Factorization homology. The operad En is defined in terms of embeddings among disjoint unions of Euclidean spaces, and so, after choosing a coordinate chart, we think of the structure of an En-algebra A as being “defined locally" on a manifold M. Patching this local structure together across the elements of an atlas produces a manifold invariant, R called the factorization homology of M with coefficients in A and denoted M A, which can be thought of as a kind of space of configurations in M labeled by elements of the algebra [AF15]. In the example of an n-fold loop space discussed above, the non-Abelian Poincar´e duality of Salvatore [Sal01] and Lurie [Lur03] supplies the identification Z n ∼ Ω X −! Mapc(M; X); M as long as X is (n − 1)-connected. Later in the course, we will encounter a precursor to this result in the configuration space models for mapping spaces introduced by McDuff [McD75, B¨od87]. In a sense, factorization homology is a method for using configuration spaces to probe manifolds, but it can also be used to study the configuration spaces themselves, reversing this flow of information [Knu17]. In particular, a theorem of Ayala-Francis shows that CONFIGURATION SPACES IN ALGEBRAIC TOPOLOGY: LECTURE 1 3 configuration spaces enjoy a kind of Mayer-Vietoris property in the existence of a quasi- isomorphism OL C∗(B(M)) ' C∗(B(M1)) C∗(B(M2)); C∗(B(N×R)) ` where B(X) := k≥0 Bk(X). The fundamental fact underlying this quasi-isomorphism is the contractibility of the unordered configuration spaces of R (see below). (3) Embedding calculus. The embedding calculus of Goodwillie and Weiss [Wei99, GW99] produces a tower of approximations . > . T Emb(M; N) 2 6 Emb(M; N) / T1Emb(M; N); which can be thought of as algebraic approximations, where algebra is construed in the operadic sense. Often these approximations become arbitrarily good|in particular, ac- cording to a theorem of Goodwillie-Klein [GK15], this occurs in codimension at least 3|so that one obtains a cofiltration of the space of embeddings. The layers of this cofil- tration are described as spaces of sections of certain bundles over configuration spaces, so hard questions about embeddings may be translated, at least in principle, into softer questions about the ordinary topology of configuration spaces. In order to develop a feel for how configuration spaces behave, we close with a few examples. Example (?, R0). It is usually best to begin with the trivial cases. In the case of the empty manifold, we have ( pt k = 0 Confk(?) = ? else, while ( 0 pt k = 0; 1 Confk(R ) = ? else. Notice that Conf0(X) is a singleton for any space X. ∼ 2 Example (R = (0; 1)). From the definition Conf2((0; 1)) = (0; 1) n f(x; y): x = yg, it is clear that the ordered configuration space two points in (0; 1) is a disjoint union of two open 2-simplices, ∼ 2 and that Σ2 acts by permuting these components. In particular, B2((0; 1)) = ∆˚ ' pt. This description generalizes readily to higher k. Note that the natural orientation of (0; 1) induces a second ordering on the coordinates of any configuration, which is to say a permutation of f1; : : : ; kg, that any such permutation is possible, and that the assignment of configuration to permutation is locally constant by the intermediate value theorem. Thus, we have a Σk- ∼ equivariant bijection π0(Confk((0; 1))) = Σk, and the unordered configuration space is naturally 4 BEN KNUDSEN identified with the path component of the identity permutation. For this space, we define a map ( k ) ˚k k+1 X Bk((0; 1)) ! ∆ := (t0; : : : ; tk) 2 R : ti > 0; ti = 1 i=0 fx1; : : : ; xkg 7! (x1; x2 − x1;:::; 1 − xk); where the set fx1; : : : ; xkg is ordered so that x1 < ··· < xk. This map is a homeomorphism; in particular, the unordered configuration spaces of R are all contractible. Example (Rn). In the configuration space of two points in Rn, there are exactly three pieces of data|the direction, the center of mass, and the distance|and only one of these is not a contractible choice. Precisely, the map n n−1 n Conf2(R ) ! S × R>0 × R x2 − x1 x1 + x2 (x1; x2) 7! ; kx2 − x1k; kx2 − x1k 2 is a homeomorphism, and, in particular, the Gauss map n n−1 Conf2(R ) ! S given by the first coordinate of this homeomorphism is a homotopy equivalence. Since this n map is also Σ2-equivariant for the antipodal action on the target, we conclude that B2(R ) ' n−1 RP . The Gauss map will play a fundamental role in our later study; in particular, by pulling back a standard volume form, this map furnishes us with our first example of a nonzero higher dimensional class in the cohomology of configuration spaces.
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