Topological complexity of classical configuration spaces and related objects
Daniel C. Cohen

TL;DR
This paper surveys the topological complexity of classical configuration spaces on surfaces and related spaces, highlighting recent results and connections to algebraic and geometric properties.
Contribution
It provides a comprehensive overview of the topological complexity in various configuration spaces, including orbit spaces and Eilenberg-Mac Lane spaces, linking topology with group actions.
Findings
Topological complexity varies with surface genus and configuration type.
Connections established between configuration space topology and algebraic properties of associated groups.
Survey consolidates known results and identifies open problems in the field.
Abstract
We survey results on the topological complexity of classical configuration spaces of distinct ordered points in orientable surfaces and related spaces, including certain orbit configuration spaces and Eilenberg-Mac Lane spaces associated to certain discrete groups.
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Topological complexity of classical configuration spaces and related objects
Daniel C. Cohen
Department of Mathematics, Louisiana State University, Baton Rouge, LA, USA
[email protected] www.math.lsu.edu/~cohen
Abstract.
We survey results on the topological complexity of classical configuration spaces of distinct ordered points in orientable surfaces and related spaces, including certain orbit configuration spaces and Eilenberg-Mac Lane spaces associated to certain discrete groups.
2010 Mathematics Subject Classification:
20F36, 55M30, 55R80
Partially supported by NSF 1105439
††copyright: ©2017: American Mathematical Society
Contents
1. Introduction
Investigation of the collision-free motion of distinct ordered particles in a topological space leads one to study the (classical) configuration space
[TABLE]
of distinct ordered points in , and the topological complexity of this space. For a path-connected topological space , the unit interval, and the space of all continuous paths (with the compact-open topology), the topological complexity of is the sectional category (or Schwarz genus) of the fibration , , . This homotopy invariant, introduced by Farber [16], provides a topological approach to the motion planning problem from robotics.
For any , one may more generally consider the sectional category of the fibration , where sends a path to points on the path, , where , . This is the higher topological complexity of , introduced by Rudyak [36], extending Farber’s notion above, as .
We survey results on the topological complexity of configuration spaces in the case where is an orientable surface, as well as related objects. The discussion is focused primarily on the “classical” topological complexity, , and includes remarks on the higher topological complexity in those instances where results on this invariant are known. The general principle is as follows:
The topological complexity is as large as possible, given natural constraints.
For instance, as is well known (and discussed in Section 2 below), the configuration space of distinct ordered points in the plane has the homotopy type of the product of a circle and a CW-complex of dimension . These constraints, together with the fact that , and the known bounds recorded next, yield the topological complexity of , recorded in Theorem 2.1.
If is a topological space with the homotopy type of a finite-dimensional CW-complex, let denote the homotopy dimension of . Throughout the discussion, we will make use of the following basic tools. For details and other relevant facts, see Farber’s survey [19].
[TABLE]
We call the first two of these the dimension and product inequalities, and use cohomology with -coefficients (unless stated otherwise) in the context of the third, the zero divisor cup length. We use the unreduced notions of topological complexity and higher topological complexity. For instance, is equal to the smallest integer such that there exists of cover of by open sets, on each of which the fibration admits a continuous local section. In particular, for contractible, .
2. The plane and the sphere
The topological complexity of the configuration space of ordered points in the plane was determined by Farber-Yuzvinsky.
Theorem 2.1** ([23]).**
* for .*
2.1. Arrangements, I
To discuss this result, we recall some relevant facts from the theory of complex hyperplane arrangements. Let be a complex vector space of dimension . A hyperplane in is a codimension one affine subspace . A hyperplane arrangement in is a finite collection of hyperplanes in . If we fix coordinates on , each hyperplane of may be realized as , where is a linear polynomial. The product is said to be a defining polynomial of the arrangement .
An arrangement is said to be essential if there are hyperplanes in whose intersection is a point. If the intersection of all hyperplanes in is nonempty, , we can choose coordinates so that is a linear form and for each . In this situation, is said to be central, and the defining polynomial is homogeneous. Refer to Orlik-Terao [35] as a general reference on arrangements.
A principal object of topological study of arrangements is the complement . The complement is an open, smooth manifold of real dimension , which has the homotopy type of a connected, finite CW-complex of dimension at most ( is a Stein manifold). If is essential, then the homotopy dimension of is precisely .
Example 2.2**.**
The braid arrangement in is the central arrangement consisting of the diagonal hyperplanes . Note that is not essential, as the diagonal line is contained in (the intersection of) all hyperplanes of . The complement of the braid arrangement
[TABLE]
is the configuration space of distinct ordered points in the plane , with fundamental group , the Artin pure braid group on strings.
Projecting along the diagonal line onto the subspace yields an essential arrangement in . Denoting the coordinates of by (where ), the hyperplanes of are , , and , . Letting be the complement, we have , and has the homotopy type of a CW-complex of dimension . Note that is itself a configuration space.
The diagonal action of the group on , , is free. The orbit space and map are the complex projective space and the Hopf fibration , respectively. For any nonempty central arrangement in , with complement , the restriction of the Hopf map, , is a bundle map, with fiber . If , we have and is contractible. Thus, is the restriction of a trivial bundle.
[TABLE]
Proposition 2.3**.**
Let be a nonempty central arrangement in . Then the complement of is diffeomorphic to the product space .
Remark 2.4*.*
The projective image of the complement of the central arrangement of hyperplanes in may itself be realized as the the complement of a (not necessarily central) arrangement of hyperplanes in the affine space . If the hyperplanes of are defined by linear forms , we may choose coordinates on so that , that is, . Then, , where is decone of with respect to , the arrangement in , with coordinates , defined by the linear polynomials , .
2.2. Cohomology
The cohomology of the configuration space of distinct ordered points in has been the object of a great deal of study, particularly for a manifold. See, for instance, [38] and the references therein. In the case where is a Euclidean space, the structure of the ring was determined by Arnol’d [2] (for ) and Cohen [11].
Theorem 2.5**.**
The integral cohomology ring has generators , , , of degree , and relations , , and for distinct .
The cohomology of the complement of an arbitrary complex hyperplane arrangement was determined by Brieskorn [5] (resolving positively a conjecture of Arnol’d).
Theorem 2.6**.**
Let be an arrangement in , where . Then the integral cohomology of the complement is torsion free, and is generated by the cohomology classes of the -forms .
Remark 2.7*.*
Let denote the algebra of differential forms generated by and the -forms , . Brieskorn’s theorem shows that the inclusion of in the de Rham complex of smooth forms on is a quasi-isomorphism, as induces an isomorphism . Consequently, the complement of a complex hyperplane arrangement is a (rationally) formal space.
We now discuss how the above considerations may be used to establish Theorem 2.1, determining the topological complexity of the configuration space . From Example 2.2, we have , and by Proposition 2.3, . Since has the homotopy type of a CW-complex of dimension , the product inequality yields
[TABLE]
The reverse inequality is obtained using the zero divisor cup length. Let and, abusing notation, denote the generators of (from Theorem 2.5 and the Universal Coefficient Theorem) by , .
Proposition 2.8** ([23]).**
The zero-divisors satisfy . Consequently, .
With the above considerations, this yields . Similarly, the topological complexity of the configuration space of ordered points in the punctured plane was determined by Farber-Grant-Yuzvinsky.
Theorem 2.9** ([22]).**
\operatorname{{\sf TC}}(F({\mathbb{C}}\smallsetminus\{m\ \text{points}\},n))=\begin{cases}2n,&\text{if m=1.}\\ 2n+1,&\text{if m\geq 2.}\end{cases}**
For , since , this is a restatement of Theorem 2.1. For , since may be realized as the complement of an essential arrangement in , we have , and consequently . The reverse inequality is obtained by showing that the zero divisor cup length of the cohomology ring is (at least) . See Section 6 for additional complementary discussion.
Remark 2.10*.*
The topological complexity of the configuration space of ordered points in a higher dimensional Euclidean space is also known:
[TABLE]
The higher topological complexity of the configuration space of ordered points in a higher dimensional (punctured) Euclidean space was computed by González-Grant.
Theorem 2.11** ([27]).**
Let be nonnegative integers with , , and such that if . Then
[TABLE]
2.3. Genus zero
The topological complexity of the configuration space of ordered points in the sphere was determined by Cohen-Farber, using results of Farber, Grant, and Yuzvinsky [19, 22].
Theorem 2.12** ([8]).**
**
For , the configuration space has the homotopy type of itself, and it is well known that .
For , there is a unique Möbius transformation of taking to [math], to and to , and depending continuously on . This yields a homeomorphism from to , the group of Möbius transformations acting on the sphere, and for , a homeomorphism
[TABLE]
taking to . Here, we have identified , is the above transformation, and for . Since deformation retracts onto and , we obtain homotopy equivalences , and, for ,
[TABLE]
Consequently, for , we have , since is a connected Lie group, see [17, Lemma 8.2].
For , the product inequality yields
[TABLE]
using the Farber-Grant-Yuzvinsky result concerning the topological complexity of recorded in Theorem 2.9 above. The reverse inequality may be obtained by showing that the zero divisor cup length of the cohomology ring
[TABLE]
is (at least) .
Similar considerations yield the higher topological complexity of the configuration space of ordered points in the sphere, as determined by González-Gutiérrez.
Theorem 2.13** ([28]).**
For , \operatorname{{\sf TC}}_{s}(F(S^{2},n))=\begin{cases}s+1,&\text{if n=1,2,}\\ sn-2,&\text{if n\geq 3.}\end{cases}
3. Genus one
The topological complexity of the configuration space of ordered points in the torus was determined by Cohen-Farber.
Theorem 3.1** ([8]).**
.
For , we have , and .
For , using the fact that is a group, it is readily checked that the map
[TABLE]
is a homeomorphism .
3.1. Fadell-Neuwirth theorem
The homotopy dimension of the configuration space may be obtained using the classical Fadell-Neuwirth theorem.
Theorem 3.2** ([14]).**
Let be a manifold without boundary of dimension at least two. For , the projection onto the first coordinates, , is a locally trivial bundle, with fiber .
Remark 3.3*.*
The aforementioned Fadell-Neuwirth bundles often admit cross sections. This is the case, for instance,
- (i)
for the bundle , when is a punctured surface; and 2. (ii)
for the bundle , when is a compact manifold with nonvanishing first Betti number.
Let . Taking in the Fadell-Neuwirth theorem, the bundle admits a cross section, and has fiber homotopy equivalent to a bouquet of circles. Using this repeatedly for reveals that is a -space, and that is an iterated semidirect product of (finitely generated) free groups. This being the case, the cohomological and geometric dimensions of are both equal to , , see [10] and Section 6 below. Consequently, . Then the dimension and product inequalities yield .
3.2. Cohen-Taylor/Totaro spectral sequence
The proof of Theorem 3.1 is completed by showing that . The tool here is the Cohen-Taylor/Totaro spectral sequence [12, 38]. For a closed -manifold, let and be the obvious projections. The inclusion yields a Leray spectral sequence converging to . The initial term is the quotient of the algebra by the relations for , , and the generators of from Theorem 2.5. The first nontrivial differential is given by , where is the cohomology class dual to the diagonal. Explicitly, if is a generator, and and are bases for with , then , where is the degree of , and is the Kronecker symbol.
As shown by Totaro [38], for a smooth complex projective variety, this spectral sequence degenerates immediately, above is the only nontrivial differential.
Proposition 3.4** ([38, 8]).**
For a smooth complex projective variety, let , and let be the ideal in generated by . Then is a subalgebra of . Consequently, and .
For , these considerations may be used to obtain the required lower bound on . Since , the algebra is graded commutative with degree-one generators. Denoting these generators by , , the ideal in is generated by the elements . The change of variables , , , for reveals that the quotient is generated by degree-one classes , , , with relations , , , , and their consequences. Recall that, for an element , we denote by the corresponding zero divisor in .
Proposition 3.5** ([8]).**
The zero divisors and , , in satisfy . Consequently, .
With the above considerations, this yields .
The higher topological complexity of the configuration space of the torus was determined by González-Gutiérrez.
Theorem 3.6** ([28]).**
For , .
4. Higher genus
The topological complexity of the configuration space of ordered points in a higher genus surface , , was studied by Cohen-Farber, and González-Gutiérrez.
Theorem 4.1** ([8, 28]).**
**
The results of González-Gutiérrez yield the higher topological complexity of the configuration space of a high genus surface.
Theorem 4.2** ([28]).**
For , .
The discussion below focuses on the classical topological complexity . For , , and , as is well known, see [16, Theorem 9].
For , the configuration space is an Eilenberg-Mac Lane space of type , where is the pure braid group of the surface . As noted in Remark 3.3 (ii), the Fadell–Neuwirth fibration admits a section. Consequently, the surface pure braid group
[TABLE]
is a semidirect product. As in the genus one case, repeated application of the Fadell-Neuwirth theorem shows that the group is an -fold iterated semidirect product of free groups. It follows that the cohomological dimension of is equal to , as is the geometric dimension. Consequently, has the homotopy type of a cell complex of dimension . So .
To complete the proof of Theorem 4.1, it remains to show that the zero divisors cup length is sufficiently large, . As discussed in [28], the proof of this last fact given in [8] contains an oversimplification, invalidating the argument there. A detailed argument establishing may be found in [28]. We put forward below an alternate approach to this argument.
The cohomology ring is generated by degree-one elements , , with relations for , and (a generator of ) for . The cohomology class dual to the diagonal may be expressed as
[TABLE]
Let , with generators , , , where, for instance, , and relations for and for , all for each , . In this notation, for the projection , we have
[TABLE]
If is the ideal in generated by these elements, by Proposition 3.4 it suffices to show that .
4.1. Gröbner bases
Write . This algebra may be realized as the quotient of an exterior algebra by a homogeneous two-sided ideal. Let be the exterior algebra (over ) generated by one-dimensional classes , , , and let be the ideal in given by
[TABLE]
where in . Then , and the ideal and the algebra may be studied using Gröbner basis theory in the exterior algebra, following Aramova-Herzog-Hibi [1]. As in [28], it is convenient to work with a quotient of . Let be the ideal in given by
[TABLE]
write , and consider the algebra
[TABLE]
a quotient of . Observe that, modulo the ideal , the generator of reduces to .
The ordering of the generators of the exterior algebra induces the degree-lexicographic order on the set of standard monomials in . If the generators of are (generically) denoted and is an increasingly ordered subset of , write for the corresponding standard monomial in . If , then if , or if and there exists with so that for and . This order is multiplicative in the sense that if and are nontrivial standard monomials with , then is a standard monomial up to sign, and .
If is an element of , the initial term of is the term in this sum for which is the largest monomial among all for which . This monomial is the initial monomial of , . For an ideal of , the initial ideal of is the ideal generated by the initial terms , . A set of elements is a Gröbner basis of if generate the ideal .
For the specific exterior algebra generated by , , , above, order the generators as follows.
[TABLE]
Proposition 4.3**.**
The set
[TABLE]
is a Gröbner basis for the ideal in the exterior algebra .
Note that the elements of are recorded with their initial terms first, and that we have used in place of . Note also the presence of the cubic elements in .
The proposition may be established using [1, Corollary 1.5], by showing that all - and -polynomials involving elements of reduce to zero with respect to . This (lengthy) process may be inductively sped up, by successively considering the ideals and sets involving the generators , of with first index , for .
Remark 4.4*.*
González-Gutiérrez [28] consider a further quotient of the algebra . In the above notation, they work with the algebra , where is the ideal generated by the elements , . This simplifies the zero divisor calculations carried out in [28], but complicates the above Gröbner basis considerations.
4.2. Zero divisors
The algebras and we consider are quotients of the exterior algebra by ideals generated in degrees greater than or equal to two, so we identify the degree-one generators of all of these algebras and denote them by the same symbols , , , . Let be the ideal in generated by all degree-one zero divisors
[TABLE]
Similarly, denote the ideal generated by degree-one zero divisors in by . To show that , it suffices to show that .
Proposition 4.5**.**
The ideal is nonzero in .
Let . We assert that the image of is nonzero in . Clearly, this image is in . For , this is immediate, as and in this instance. For , as the natural projection takes the generators and powers of to those of , it is enough to show that the image of in is nonzero.
A calculation with the description of the ideal defining given in §4.1 reveals that, for , the image of in is given by
[TABLE]
where and . In particular, and .
The Gröbner basis recorded in Proposition 4.3 may be used to show that this element is nonzero in . For instance, the leading term of this element (in ) is the tensor product of two monomials neither of which reduce to zero with respect to . It follows that (the leading term of) is nonzero in . Consequently, , , and as was required.
5. Orbit configuration spaces
Let be a group and a -space. The orbit configuration space is the space of all ordered -tuples of points in which lie in distinct -orbits,
[TABLE]
Orbit configuration spaces, introduced by Xicoténcatl [39], are natural generalizations of classical configuration spaces. If is trivial, is the classical configuration space.
5.1. Generalized Fadell-Neuwirth theorem
We will focus on the case where is a connected manifold without boundary of positive dimension, and is a finite group acting freely on . Let denote the union of distinct orbits, , in . The Fadell-Neuwirth theorem recorded in Theorem 3.2 was generalized by Xicoténcatl to orbit configuration spaces as follows.
Theorem 5.1** ([39]).**
For , the projection onto the first coordinates,
[TABLE]
is a locally trivial bundle, with fiber .
The proof of this result given in [39] is a modification of that of [14] for classical configuration spaces. In the special case an alternative argument, which informs on the structure of these bundles, is given in [6].
Assume that the order of the finite group is , and write . Define a map from the orbit configuration space to the classical configuration space by sending an -tuple of points in to their orbits. That is, define by
[TABLE]
Theorem 5.2** ([6]).**
The orbit configuration space bundle is equivalent to the pullback of the classical configuration space bundle under the map .
Now specialize to the case where the finite cyclic group acts freely on the manifold by multiplication by the primitive -th root of unity . The associated orbit configuration space is
[TABLE]
which may be realized as the complement in of the hyperplane arrangement consisting of the hyperplanes , , and , , . The arrangement consists of the reflecting hyperplanes of the full monomial group, the complex reflection group isomorphic to the wreath product of the symmetric group and . For instance, when , this is the type B Coxeter group, and is the type B pure braid group. Discussions of reflection arrangements, including the full monomial arrangements , may be found in references including [35, 41].
Theorem 5.3**.**
**
This result may be established using techniques from the theory of hyperplane arrangements as discussed in Section 2 and below, or by using the group theoretic methods presented in Section 6.
5.2. Arrangements, II
Beginning with work of Arnol’d and Brieskorn (see §2.2), the cohomology ring of the complement of a complex hyperplane arrangement is a well-studied object, facilitating analysis of the (higher) zero divisor cup length in this context. Let be an arrangement of hyperplanes in . For convenience, we will assume that is essential, and we will use cohomology with coefficients in .
The Orlik-Solomon theorem [34] shows that is isomorphic to the Orlik-Solomon algebra , the quotient of the exterior algebra generated by one-dimensional classes , , by a homogeneous ideal . Detailed expositions may be found in [35, 40]. Let , refer to the hyperplanes of by their subscripts, and order them accordingly. Given , denote the flat by . If , call independent if the codimension of in is equal to , and dependent if . If is an increasingly ordered subset of , recall that denotes the corresponding standard monomial in the exterior algebra. Define . The Orlik-Solomon ideal is generated by
[TABLE]
A circuit is a minimally dependent subset , that is, is dependent, but every nontrivial subset of is independent. If is dependent and a circuit, then , and . Also, note that if , then for any containing . In light of these two observations, the generating set for the Orlik-Solomon ideal given above may be reduced as follows: The ideal is generated by
[TABLE]
The ordering of the hyperplanes of induces the degree-lexicographic order on the set of standard monomials in the exterior algebra . Call a subset of a broken circuit if there exists so that for all and is a circuit. Broken circuits correspond to the initial monomials of the elements appearing in (5.1). In [40, Theorem 2.8], Yuzvinsky shows that the initial monomials of elements of generate , the ideal generated by the initial terms of elements of , whence is a Gröbner basis for the Orlik-Solomon ideal , see [1]. This yields a basis for the quotient , the Orlik-Solomon algebra of the arrangement .
For , let denote the image of the standard monomial in the Orlik-Solomon algebra . The nbc basis for consists of all elements corresponding to subsets of which contain no broken circuits [35, 40]. This basis has been used to study the (higher) zero divisor cup length of by a number of authors, including [23, 41]. Following these references, we restrict our attention to a central arrangement . Recall that we assume is essential in . Consequently, a maximal independent set (resp., nbc set) has cardinality .
Let be an ordered pair of disjoint subsets of , and let . The pair is said to be basic if and are nbc sets for some linear order on and is a maximal independent set, . The central arrangement is said to be large if there is a basic pair with . In [41], Yuzvinsky uses basic pairs to find lower bounds on the (higher) zero divisor cup length of the Orlik-Solomon algebra, and proves the following.
Theorem 5.4** ([41]).**
Let be an essential central arrangement in with complement , and let be a positive integer. If is a basic pair, then . If is large, then .
The arrangements in associated to the full monomial groups and arising in the context of cyclic group orbit configuration spaces are large. Recall that has hyperplanes and , where , and take and . Thus, Theorem 5.3 follows from Theorem 5.4. More generally, Yuzvinsky establishes an analogous result for the reflection arrangement associated to any irreducible complex reflection group.
A complex reflection in is a finite order linear transformation whose fixed point set is a hyperplane . A reflection group is a finite subgroup of that is generated by reflections. A reflection group is irreducible if its tautological representation in is irreducible. The reflection arrangement associated to the reflection group is the set of hyperplanes .
Theorem 5.5** ([41]).**
Let be an irreducible reflection group of rank , and let be a positive integer. If is the associated reflection arrangement, then .
Remark 5.6*.*
If is a simple graph with vertices , the associated graphic arrangement consists of the hyperplanes in corresponding to the edges of . For instance, if is the complete graph, then is the braid arrangement introduced in Example 2.2. In [24], Fieldsteel uses Yuzvinsky’s result stated in Theorem 5.4 to find conditions on the graph , related to the arboricity, which insure that the (higher) topological complexity of the complement of a graphic arrangement is as large as possible.
6. Some discrete groups
Let X be an aspherical space, that is, a space whose higher homotopy groups vanish: for . Farber [19] poses the problem of computing the topological complexity of such a space in terms of algebraic properties of the fundamental group . In other words, given a discrete group , define the topological complexity of to be , the topological complexity of an Eilenberg-Mac Lane space of type , and express in terms of invariants such as the cohomological or geometric dimension of if possible.
Example 6.1**.**
Associated to a simple graph on vertices is a right-angled Artin group with generators corresponding to the vertices of , and commutator relators corresponding to the edges. For instance, if is the complete graph, then is free abelian, while if has no edges, then is free. For any right-angled Artin group, one has , where is the maximal number of vertices of covered by two (disjoint) cliques in , see [9, 29, 31].
Many of the configuration spaces discussed previously are -spaces, for surface pure braid groups, for pure braid groups associated to reflection groups, etc. For example, is the Artin pure braid group. From the homotopy exact sequence of the Fadell-Neuwirth bundle , with fiber and cross section, we see (inductively) that is a -space, and obtain a split, short exact sequence , where is the free group on generators. Thus,
[TABLE]
is an iterated semidirect product of free groups.
The iterated semidirect product structure of is apparent in the classical presentation of this group. The pure braid group has generators , , and relations
[TABLE]
where denotes the commutator, see, for instance Birman [4]. Observe that, for as in the relations above, the action of on (via the Artin representation) is by conjugation. It follows that the induced action of on is trivial.
6.1. Almost-direct products of free groups
An almost-direct product of free groups is an iterated semidirect product of finitely generated free groups for which acts trivially on for . Thus, is an almost-direct product of free groups. The fundamental groups of the orbit configuration spaces considered in the previous section provide another family of examples.
Let , and . The pure braid group associated to the full monomial group may also be realized as an almost-direct product of free groups. From Theorems 5.1 and 5.2, the map defined by forgetting the last coordinate is a bundle, with fiber . A minor modification of these results is useful in revealing the almost-direct product structure of . Given a configuration of distinct ordered points in , one obtains a configuration of distinct ordered points in , yielding a homotopy equivalence . Using this observation, together with Theorem 5.2, one can check that the bundle may be realized as the pullback of the classical configuration space bundle where , under the map given by
[TABLE]
It follows that the orbit configuration space bundle admits a section, and the fundamental group of the base acts trivially on the homology of the fiber. Hence, an inductive argument reveals that is an almost-direct product of free groups.
Under natural assumptions on the ranks of the constituent free groups, the topological complexity of an almost-direct product of free groups was determined by Cohen.
Theorem 6.2** ([7]).**
If is an almost-direct product of free groups with for each , and is a nonnegative integer, then
[TABLE]
For an arbitrary iterated semidirect product of free groups of cohomological dimension , a -complex of dimension is constructed in [10]. Thus, for such groups, the dimensional upper bound on topological complexity may be stated in terms of the cohomological dimension as .
The integral homology is torsion-free and the Poincaré polynomial is given by , where is the -th Betti number of , see [15]. A minimal, free -resolution of , which we denote by , is constructed in [10].
Let . The abelianization map induces a chain map , where and is the standard -resolution of . The induced map in integral cohomology is surjective, and is an isomorphism in dimension one, see [7, Theorem 2.1].
Let be the ideal in the exterior algebra generated by the elements of the kernel of the surjection , . An explicit Gröbner basis for is exhibited in [7, §3] (in the degree-lexicographic order on a standard basis for the exterior algebra), and this is used to shown that the integral cohomology ring of is given by .
Passing to field coefficients, , if is an almost-direct product of free groups with for each , one can exhibit pairs of generators of corresponding to distinct generators of the free groups , . As shown in [7, Theorem 4.2], this yields zero-divisors in with nonzero product. These considerations yield for as in the statement of the theorem. The general case may be obtained from this, the product inequality, and a straightforward analysis of the zero-divisor cup length of .
6.2. Fiber-type arrangements
The Artin pure braid group associated to the symmetric group, and, more generally, the pure braid groups associated to the full monomial groups may be realized as the fundamental groups of the hyperplane arrangements defined by the polynomials
[TABLE]
Notice that the arrangement here corresponds to the arrangement from Example 2.2, so that the fundamental group is the Artin pure braid group on strands.
The arrangements are examples of (essential) fiber-type arrangements. An arrangement in is said to be strictly linearly fibered if there is a choice of coordinates on so that the restriction, , of the projection , , to the complement is a fiber bundle projection, with base , the complement of an arrangement in , and fiber the complement of finitely many points in . We say is strictly linearly fibered over . Fiber-type arrangements are then defined inductively as follows: An arrangement of finitely many points in is fiber-type. An arrangement of hyperplanes in is fiber-type if is strictly linearly fibered over a fiber-type arrangement in .
The complement of a fiber-type arrangement sits atop a tower of fiber bundles
[TABLE]
where the fiber of is homeomorphic to the complement of points in . Repeated application of the homotopy exact sequence of a bundle shows that is a -space, where . The integers are called the exponents of the fiber-type arrangement .
Suppose is strictly linearly fibered over , and , where . From the definition, a defining polynomial for factors as , where is a product of linear functions. Since has distinct roots for any , the map
[TABLE]
takes values in the configuration space .
Theorem 6.3** ([6]).**
Let be an arrangement of hyperplanes, and let be an arrangement of hyperplanes which is strictly linearly fibered over . Then the bundle is equivalent to the pullback of the classical configuration space bundle under the map .
From this result, it follows that the bundle admits a section, that the structure group of this bundle is the pure braid group , and that the fundamental group of the base acts by conjugation (in fact, by a pure braid action) on the fundamental group of the fiber.
If is a fiber-type arrangement with exponents , repeated application of this theorem and these consequences reveals that
[TABLE]
is an almost-direct product of free groups. Theorem 6.2 yields the following.
Corollary 6.4**.**
Let be a fiber-type arrangement with exponents and let be the fundamental group of the complement of . If the exponents of are all at least two, , , and is a nonnegative integer, then
[TABLE]
Theorem 5.3 may be obtained from this result as follows. From Proposition 2.3 and Remark 2.4, the complement of the essential, central arrangement may be realized as . It is readily checked that the decone (with respect to ) in is fiber-type, with exponents all at least two. So we have
[TABLE]
6.3. Subgroup conditions
Several of the results on the topological complexity of discrete groups mentioned above may also be obtained by other (group-theoretic) means, as shown by Grant-Lupton-Oprea.
Theorem 6.5** ([31]).**
Let be a discrete group. If and are subgroups of which satisfy for every , then .
This may be used to recover the topological complexity of the pure braid group, . The pure braid group has a free abelian subgroup , generated in terms of the standard generators of by , , see, for instance, Birman [4]. Let be the image of the right splitting in the exact sequence . The subgroup consists of pure braids with trivial last strand, and is generated by with . In [31], it is shown geometrically that . This may also be established algebraically using the pure braid relations recorded in (6.1) above. Consequently, .
Theorem 6.5 may additionally be used to recover the topological complexity of the pure monomial braid group , recorded in Theorem 5.3 in terms of that of the orbit configuration space , a -space. From Theorem 5.2 and the discussion in §6.1, the group may be expressed as an almost-direct product , where . Using this, and the presentation of given in [6, Theorem 2.2.4], one can exhibit a rank free abelian subgroup and a cohomological dimension subgroup satisfying . Consequently, . We anticipate that this result may also be used to recover the topological complexity of other almost-direct products of free groups, such as the fundamental groups of complements of other fiber-type hyperplane arrangements.
In [31], Grant-Lupton-Oprea also use Theorem 6.5 to find the topological complexity of right-angled Artin groups, and strikingly, to show that for Higman’s acyclic group .
Remark 6.6*.*
The pure braid group is the kernel of the homomorphism from the full braid group to the symmetric group sending a braid to its induced permutation. If is a subgroup, the preimage is a subgroup of containing . In [32], Grant and Recio-Mitter study the (higher) topological complexity of subgroups of arising in this way. For a subgroup , they use Theorem 6.5 to show that . In particular, this lower bound, together with the upper bound of Grant [30] for a torsion-free discrete group with center embedded in via the diagonal homomorphism, yields when .
7. Sins of omission
We close with some brief remarks regarding two directions not discussed in the previous sections, including comments indicating the reasons for these omissions.
7.1. Graph configuration spaces
Investigation of the collision-free motion of automated guided vehicles on, for instance, a network of wires leads one to study the configuration spaces of distinct points on graphs (see [26]), and the topological complexity of these spaces. Let be a finite, connected graph. In sharp contrast to the behavior discussed in the previous sections, the topological complexity of the ordered configuration space of a graph is, in certain instances, independent of the number of particles . We state results of Farber and Scheirer, which apply in the case where is a tree, along these lines below.
An essential vertex of is a vertex which has at least three incident edges. Let denote the number of essential vertices of . As noted in [20, Lemma 10.1], the configuration space is connected if has at least one essential vertex. This is the case if is not homeomorphic to the closed interval (and ) or to the circle (and ). If , a result of Ghrist [25] shows that the configuration space has the homotopy type of a cell complex of dimension at most . Thus the dimension inequality recorded in the Introduction insures that for any such graph, see Farber [18].
Theorem 7.1** ([20]).**
Let be a tree not homeomorphic to the closed interval , and let be an integer satisfying . If , assume in addition that is not homeomorphic to the letter . Then, .
An arc in is a subspace homeomorphic to the interval . Let be a subset of the vertex set of . Loosely speaking, a collection of oriented arcs is allowable for if no vertex in is an endpoint of any arc, and at each vertex in there is at least one direction in which the orientations of the arcs do not “cancel out.” Refer to Scheirer [37, Definition 2.3] for a precise formulation.
Theorem 7.2** ([37]).**
Let be a tree with , and let be the smallest integer for which there is a collection of oriented arcs in which is allowable for the collection of all vertices in which have exactly three incident edges. Let if there are no such vertices. If , then .
7.2. Unordered configuration spaces
Given a space , the symmetric group acts on by permuting coordinates. This restricts to a free action on the configuration space of distinct ordered points in . The orbit space is the configuration space of distinct unordered points in , with fundamental group the full braid group of . These unordered configuration spaces are sometimes -spaces. For example, is the Artin full braid group, and is an aspherical space, since its covering space is. On the other hand, the full braid group of the sphere has torsion (see [4]), so does not have a finite .
More generally, if is a complex reflection group, with associated reflection arrangement , then the complement is an aspherical space. This fact has a lengthy history, relevant references include [2, 5, 13, 35, 3]. As above, acts freely on , and the orbit space is also aspherical. The fundamental groups and are the pure and full braid groups for .
The reader has likely noted that, prior to this point, the topological complexity of unordered configuration spaces, orbit spaces of reflection groups, and the associated full braid groups has not been mentioned. The reason for this is quite simple. To the best of our knowledge, very little is known concerning the topological complexity in any of these contexts. While group theoretic aspects of full braid groups and cohomological aspects of these groups, configuration spaces, and orbit spaces are well studied, as noted in [32], the lower bounds provided by the zero divisor cup length and by the subgroup conditions of Theorem 6.5 appear to be insufficient to determine the topological complexity. This is the case, in particular, for the Artin full braid group , that is, for the unordered configuration space .
One notable exception is the unordered configuration space of a tree . Under the assumptions of Theorem 7.2, Scheirer [37] shows that the topological complexity of the unordered configuration space is equal to that of the ordered configuration space, .
Acknowledgements
This survey expands on lectures given at the Mathematisches Forschungsinstitut Oberwolfach Mini-Workshop Topological Complexity and Related Topics in the Spring of 2016. We thank the organizers M. Grant, G. Lupton, and L. Vandembroucq for an enjoyable, interesting, and stimulating workshop. We also thank the MFO for its support and hospitality, and for providing a productive mathematical envirnoment. The algebraic geometry and commutative algebra system Macaulay2 [33] and the package Mathematica (from Wolfram Research) were useful in the preparation of the manuscript. Finally, we thank the referee for pertinent remarks and suggestions, and we thank S. He, J. Kona, J. Strummer, M. Jones, P. Simonon, and T. Headon for inspiration.
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