Higher-Order Intersections in
We show how to measure the failure of the Whitney trick in dimension 4 by constructing higher-order intersection invariants of Whitney towers built from iterated Whitney disks on immersed surfaces in 4–manifolds. For Whitney towers on immersed disks in the 4–ball, we identify some of these new invariants with previously known link invariants like Milnor, Sato-Levine and Arf invariants. We also define higher-order Sato-Levine and Arf invariants and show that these invariants detect the obstructions to framing a twisted Whitney tower. Together with Milnor invariants, these higher-order invariants are shown to classify the existence of (twisted) Whitney towers of increasing order in the 4–ball. A conjecture regarding the non-triviality of the higher-order Arf invariants is formulated, and related implications for filtrations of string links and 3-dimensional homology cylinders are described.
Despite how it may appear in high school, mathematics is not all about manipulating numbers or functions in more and more complicated algebraic or analytic ways. In fact, one of the most interesting quests in mathematics is to find a good notion of space. It should be general enough to cover many real life situations and at the same time sufficiently specialized so that one can still prove interesting properties about it. A first candidate was Euclidean -space , consisting of -tuples of real numbers. This covers all dimensions but is too special: the surface of the earth, mathematically modelled by the –sphere , is 2-dimensional but compact, so it can’t be . However, is locally Euclidean: around every point one can find a neighborhood which can be completely described by two real coordinates (but global coordinates don’t exist).
This observation was made into the definition of an -dimensional manifold in 1926 by Kneser: It’s a (second countable) Hausdorff space which looks locally like . The development of this definition started at least with Riemann in 1854 and important contributions were made by Poincaré and Hausdorff at the turn of the 19th century. It is believed to cover many important important physical notions, like the surface of the earth, the universe, and space-time (for and , respectively) but is special enough to allow interesting structure theorems. One such statement is Whitney’s (strong) embedding theorem: Any -manifold can be embedded into (for all ).
The proof in small dimensions is fairly elementary and special, but in all dimensions , Hassler Whitney [Wh] found the following beautiful argument: By general position, one finds an immersion with at worst transverse double points. By adding local cusps, one can assume that all double points can be paired up by Whitney disks as in Figure 2, using the fact that is simply connected. Since and , one can arrange that all Whitney disks are disjointly embedded and also meet the image of only on the boundary (as well as satisfying a certain normal framing condition). Then a sequence of (what today are called) Whitney moves leads to the desired embedding of (Figure 2). To be more precise, one needs to distinguish between topological and smooth manifolds. A topological –manifold is locally homeomorphic to , whereas a smooth manifold is locally diffeomorphic to it (in the given smooth structure). Whitney’s argued in the smooth setting where transversality and isotopy extension theorems were readily available. Kirby and Siebenmann [KS] made these tools available also in the topological category in dimensions , see for example page 122 for the topological Whitney move.
The Whitney move, sometimes also called the Whitney trick, remains a primary tool for turning algebraic information (counting double points) into geometric information (existence of embeddings). It was successfully used in the classification of manifolds of dimension , specifically in Smale’s celebrated h-cobordism theorem [Sm] (implying the Poincaré conjecture) and the surgery theory of Kervaire-Milnor-Browder-Novikov-Wall [Wa]. The failure of the Whitney move in dimension 4 is the main reason that, even today, there is no classification of 4-dimensional manifolds in sight.
Casson realized that in the setting of the 4-dimensional h-cobordism theorem, even though Whitney disks can’t always be embedded (because ), they always fit into what is now called a Casson tower. This is an iterated construction that works in simply connected –manifolds, where one adds more and more layers of disks onto the singularities of a given (immersed) Whitney disk [Ca]. In an amazing tour de force, Freedman [F1, F2] showed that there is always a topologically embedded disk in a neighborhood of certain Casson towers (originally, one needed 7 layers of disks, later this was reduced to 3). This result implied the topological h-cobordism theorem (and hence the topological Poincaré conjecture) in dimension . At the same time, Donaldson used Gauge theory to show that the smooth h-cobordism theorem is wrong [Do], and both results were awarded with a Fields medal in 1982. Surprisingly, the smooth Poincaré conjecture is still open in dimension – the only remaining unresolved case.
In the non-simply connected case, even the topological classification of –manifolds is far from being understood because Casson towers cannot always be constructed. See [FQ, FT1, KQ] for a precise formulation of the problem and a solution for fundamental groups of subexponential growth. However, there is a simpler construction, called a Whitney tower, which can be performed in many more instances. The current authors have developed an obstruction theory for such Whitney towers in a sequence of papers [CST1, CST2, CST3, CST4, CST5, CST, S, ST, ST1]. Even though the existence of a Whitney tower does not lead to an embedded (topological) disk, it is still a necessary condition. Hence our obstruction theory provides higher-order (intersection) invariants for the existence of embedded disks, spheres, or surfaces in –manifolds.
The easiest example of our intersection invariant is Wall’s self-intersection number for disks in 4-manifolds. If has trivial self-intersection number (we say that the order zero invariant vanishes) then all self-intersections can be paired up by Whitney disks . However, the now self-intersect and intersect each other and also the original disk . Our (first order) intersection invariant measures the intersections and vanishes if they all can be paired up by (second order) Whitney disks . This procedure continues with an invariant which measures both and intersections, and the construction of a higher-order Whitney tower if the invariant vanishes. is the union of (at order 0) and all Whitney disks (order 1), (order 2) and continuing with higher-order Whitney disks. If is homotopic (rel. boundary) to an embedding then these constructions can be continued ad infinitum.
The intersection invariants take values in a finitely generated abelian group which is generated by certain trivalent trees that describe the 1-skeleton of a Whitney tower (Figure 3). The relations in correspond to Whitney moves, and quite surprisingly most of these relations can be expressed in terms of the so called IHX-relation which is a geometric incarnation of the Jacobi identity for Lie algebras. All the relations can be realized by controlled manipulations of Whitney towers, and as a result we recover the following approximation of the “algebra implies geometry” principle that is available in high dimensions:
Theorem 1 (Raising the order of a Whitney tower).
If supports an order Whitney tower with vanishing , then is homotopic (rel. boundary) to which supports an order Whitney tower. Compare Theorem 22.
As usual in an obstruction theory, the dependence on the lower order Whitney towers makes it hard to derive explicit invariants that prevent the original disk from being homotopic to an embedding. In this paper we discuss how to solve this problem in the easiest possible ambient manifold , the 4-dimensional ball. We start with maps
which exhibit a fixed link in the boundary –sphere . If this link is slice then the are homotopic (rel. boundary) to disjoint embeddings and our Whitney tower theory gives obstructions to this situation. In the simplest example discussed above we have and the boundary of is just a knot in :
Theorem 2 (The easiest case of knots [Cst2]).
The first order intersection invariant can be identified with the Arf invariant of the knot . It is thus a well-defined invariant that only depends on . Moreover, it is the complete obstruction to finding a Whitney tower of arbitrarily high order with boundary .
There is a very interesting refinement of the theory for knots in the setting of Cochran, Orr, and Teichner’s -solvable filtration: Certain special symmetric Whitney towers of orders which are powers of have a refined measure of complexity called height, and are obstructed by higher-order signatures of associated covering spaces [COT1]. However there are no known algebraic criteria for “raising the height” of a Whitney tower, as given by Theorem 1.
If then the order zero invariant is given by the linking numbers of the components of the link that is the boundary of the given disks. Milnor [M1, M2] showed in 1954 how to generalize linking numbers inductively to higher order. Here we use the total order Milnor invariants which correspond to all length Milnor numbers .
Theorem 3 (Milnor numbers as intersection invariants).
If a link bounds a Whitney tower of order then the Milnor invariants of order vanish. Moreover, the order Milnor invariants of can be computed from the intersection invariant . Compare Theorem 26.
In the remaining sections, we will make these statements precise and explain how to get complete obstructions for the existence of Whitney towers for links. Unlike the case of knots, these get more and more interesting for increasing order. In addition to the above Milnor invariants (higher-order linking numbers), we’ll need higher-order versions of Sato-Levine and Arf invariants. In a fixed order, these are finitely many -valued invariants, so that, surprisingly, the Milnor invariants already detect the problem up to this -torsion information.
Theorem 4 (Classification of Whitney tower concordance).
A link bounds a Whitney tower of order if and only if its Milnor invariants, Sato-Levine invariants and Arf invariants vanish up to order . Compare Corollary 12.
To prove this classification, we use Theorem 1 to show that the intersection invariant leads to a surjective realization map , where consist of links bounding Whitney towers of order , up to order Whitney tower concordance (see the next section). The Milnor invariant can be translated into a homomorphism , where the latter is a group defined from a free Lie algebra (which can be expressed via rooted trivalent trees modulo the Jacobi identity). The composition
is hence a map between purely combinatorial objects both given in terms of trivalent trees. Using a geometric argument (grope duality), we show that it is simply given by summing over all choices of a root in a given tree (which is a more precise statement of Theorem 3). This map was previously studied by Jerry Levine in his work on -dimensional homology cylinders [L1, L2], where he made a precise conjecture about the kernel and cokernel of . He verified the conjecture for the cokernel in [L3], using a generalized Hall algorithm.
In [CST3] we prove Levine’s full conjecture via an application of combinatorial Morse theory to tree homology. In particular, we show that the kernel of consists only of -torsion. This -torsion corresponds to our higher-order Sato-Levine and Arf invariants, and is characterized geometrically in terms of a framing obstruction for twisted Whitney towers (in which certain Whitney disks are not required to be framed).
In the above classification of Whitney tower concordance there remains one key geometric question: Although our higher-order Arf invariants are well-defined, it is not currently known if they are in fact non-trivial. All potential values are indeed realized by simple links, so the question here is whether or not there are any further geometric relations; see Definition 11. We conjecture that there are indeed new higher-order Arf invariants, or equivalently, that our realization maps are isomorphisms for all . Here is a certain quotient of by what we call framing relations which come from IHX-relations on twisted Whitney towers. For we do show that is an isomorphism, implying that in this further quotient the intersection invariant only depends on the link , and not on the choice of Whitney tower . The higher-order Arf invariants appear when , and our conjecture says that the same conclusion holds in these orders.
This conjecture is in turn equivalent to the vanishing of the intersection invariants on all immersed –spheres in . Of course all such maps are null-homotopic, and a general goal of the Whitney tower theory is to extract higher-order invariants of representatives of classes in the second homotopy group . This obstruction theory is still being developed but certain aspects of it appeared in [CST, S3, ST, ST1]. The fundamental group leads to more interesting obstruction groups and a non-trivial leads to more relations to make the intersection invariants only dependent on the order zero surfaces.
In this paper, we will give a survey of the necessary material that is needed to understand the above results for Whitney towers in the 4-ball. More details and proofs can be found in our recent series of five papers [CST1, CST2, CST3, CST4, CST5] from which we’ll also survey here the following aspects of the theory:
Twisted Whitney towers and obstruction to framing them
Geometrically -slice links and vanishing Milnor invariants
String links and the Artin representation
Levine’s Conjecture and filtrations of homology cylinders
2. Whitney towers
We work in the smooth oriented category (with discussions of orientations mostly suppressed), even though all results hold in the locally flat topological category by the basic results on topological immersions in Freedman–Quinn [FQ]. In particular, our techniques do not distinguish smooth from locally flat surfaces.
Order Whitney towers are defined recursively as follows.
A surface of order 0 in an oriented –manifold is a connected oriented surface in with boundary embedded in the boundary and interior immersed in the interior of . A Whitney tower of order 0 is a collection of order 0 surfaces. The order of a (transverse) intersection point between a surface of order and a surface of order is . The order of a Whitney disk is if it pairs intersection points of order . For , a Whitney tower of order is a Whitney tower of order together with (immersed) Whitney disks pairing all order intersection points of .
The Whitney disks in a Whitney tower may self-intersect and intersect each other as well as lower order surfaces but the boundaries of all Whitney disks are required to be disjointly embedded. In addition, all Whitney disks are required to be framed, as will be discussed below.
2.1. Whitney tower concordance
We now specialize to the case , and also assume that a Whitney tower has disks for its order surfaces which have an -component link in as their boundary, denoted . Let be the set of all framed links where is an order Whitney tower, and the link framing is induced by the order disks in . This defines a filtration of the set of framed -component links . Note that consists of links that are evenly framed because a component has even framing if and only if it bounds a framed immersed disk in .
In order to detect what stage of the filtration a particular link lies in, it would be convenient to define a set measuring the difference between and . Because these are sets and not groups, the quotient is not defined. However we can still define an associated graded set in the following way.
Suppose is an order Whitney tower in where each of the order surfaces is an annulus with one boundary component in and one in . Then we say that the link is order Whitney tower concordant to . This allows us to define the associated graded set as modulo order Whitney tower concordance. Knots have a well-defined connected sum operation, but the analogous band-sum operation for links is not well-defined, even up to concordance. This makes the following proposition somewhat surprising; it follows from Theorem 1.
Proposition 6 ([Cst1]).
Band sum of links induces a well-defined operation which makes each into a finitely generated abelian group.
Our goal is to determine these groups .
2.2. Free Lie and quasi-Lie algebras
Let denote the free Lie algebra (over the ground ring ) on generators . It is -graded, , where the degree part is the additive abelian group of length brackets, modulo Jacobi relations and the self-annihilation relation . The free quasi-Lie algebra is gotten from L by replacing the self-annihilation relation with the weaker anti-symmetry relation .
The bracketing map , has a nontrivial kernel, denoted . The analogous bracketing map on the free quasi-Lie algebra is denoted . For later purposes, we now define a homomorphism . Given an element , of , its image under the bracketing map is zero in . However, regarding the bracket as being in , we get an element of the kernel of the projection . This kernel is isomorphic to by [L3], and so we get an element of as desired.
2.3. The total Milnor invariant
Let be a link where all the longitudes lie in , the th term of the lower central series of the link group . By Van Kampen’s Theorem , where is the free group on meridians. Let denote the image of the -th longitude. The total Milnor invariant of order is defined by
It turns out that in fact (by “cyclic symmetry”). The invariant is a convenient way of packaging all Milnor invariants of length in one piece.
Theorem 7 ([Cst4]).
For all , the total Milnor invariant is a well-defined homorphism such that
is an epimorphism for odd ; denote its kernel by .
For even , is a monomorphism with image .
So is an algebraic obstruction for bounding a Whitney tower of order which is a complete invariant in half the cases. In the other half, we’ll need the following additional invariants.
2.4. Higher-order Sato-Levine invariants
Suppose and . This implies that the longitudes lie in , so that is defined. Define the order Sato-Levine invariant by , where is defined above.
Theorem 8 ([Cst4]).
For all , the Sato-Levine invariant gives a well-defined epimorphism . Moreover, it is an isomorphism for even .
The case is the original Sato-Levine [Sa] invariant of a 2-component classical link, and we describe in [CST4] (and below) how the are obstructions to “untwisting” an order twisted Whitney tower.
2.5. Higher-order Arf invariants
We saw above that the structure of the groups is completely determined for by Milnor and higher-order Sato-Levine invariants.
Theorem 9 ([Cst4]).
Let be the kernel of . Then there is an epimorphism .
is an isomorphism.
This conjecture is true when , and indeed the inverse map is given by the classical Arf invariant of each component of the link.
Regardless of whether or not Conjecture 10 is true, induces an isomorphism on .
The higher-order Arf invariants are defined by
Any of the which are non-trivial would the only possible remaining obstructions to a link bounding a Whitney tower of order , following the Milnor and Sato-Levine invariants:
Corollary 12 ([Cst4]).
The associated graded groups are classified by , if is odd, and, for , .
The first unknown Arf invariant is , which in the case of -component links would be a -valued invariant, evaluating non-trivially on the Bing double of any knot with non-trivial classical Arf invariant. Evidence supporting the existence of non-trivial is provided by the fact that such links are known to not be slice [Cha]. All cases for are currently unknown, but if is trivial then all higher-order would also be trivial [CST2].
3. Twisted Whitney towers
The order Sato-Levine invariants are defined as a certain projection of order Milnor invariants, suggesting that a slightly modified version of the Whitney tower filtration would put the Milnor invariants all in the right order, with no more need for the Sato-Levine invariants. In this section we discuss how this corresponds to the geometric notion of twisted Whitney towers.
3.1. Twisted Whitney disks
The normal disk-bundle of a Whitney disk is isomorphic to , and comes equipped with a canonical nowhere-vanishing Whitney section over the boundary given by pushing tangentially along one sheet and normally along the other.
In Figure 4, the Whitney section is indicated by a dotted loop shown on the left for a Whitney disk pairing intersections between surface sheets and in a -dimensional slice of –space. On the right is shown an embedding into –space of the normal disk-bundle over , indicating how the Whitney section determines a nowhere-vanishing section which lies in the -sheet and avoids the -sheet.
The Whitney section determines the relative Euler number which represents the obstruction to extending the Whitney section across . It depends only on a choice of orientation of the tangent bundle of the ambient 4-manifold restricted to the Whitney disk, i.e. a local orientation. Following traditional terminology, when vanishes is said to be framed. (Since has a unique trivialization up to homotopy, this terminology is only mildly abusive.) If , we say that is -twisted, or just twisted if the value of is not specified.
In the definition of an order Whitney tower given above all Whitney disks are required to be framed (-twisted). It turns out that the natural generalization to twisted Whitney towers involves allowing non-trivially twisted Whitney disks only in at least “half the order” as follows:
A twisted Whitney tower of order is just a (framed) Whitney tower of order as in Definition 5 above.
A twisted Whitney tower of order is a Whitney tower having all intersections of order less than paired by Whitney disks, with all Whitney disks of order less than required to be framed, but Whitney disks of order at least allowed to be -twisted for any .
Note that, for any , an order (framed) Whitney tower is also an order twisted Whitney tower. We may sometimes refer to a Whitney tower as a framed Whitney tower to emphasize the distinction, and will always use the adjective “twisted” in the setting of Definition 13.
3.2. Twisted Whitney tower concordance
Let be the set of framed links in which are boundaries of order twisted Whitney towers in , with no requirement that the link framing is induced by the order disks. Notice that . While not immediately obvious, it is true that this defines a filtration . As in the framed setting above, letting be the set modulo order twisted Whitney tower concordance yields a finitely generated abelian group.
Theorem 14 ([Cst2, Cst4]).
The total Milnor invariants give epimorphisms which are isomorphisms for . Moreover, the kernel of is isomorphic to the kernel of the Sato-Levine map from the previous section.
Conjecture 10 hence says that and our Arf-invariants represent the only remaining obstruction to a link bounding an order twisted Whitney tower:
The groups are classified by and, for , .
3.3. Gropes and k-slice links
Roughly speaking, a link is said to be “-slice” if it is the boundary of a surface which “looks like a collection of slice disks modulo -fold commutators in the fundamental group of the complement of the surface”. Precisely, is -slice if bounds an embedded orientable surface such that is a bijection and there is a push-off homomorphism whose image lies in the th term of the lower central series . Igusa and Orr proved the following “-slice conjecture” in [IO]:
Theorem 16 ([Io]).
A link is -slice if and only if for all .
A -fold commutator in has a nice topological model in terms of a continuous map , where is a grope of class . Such 2-complexes (with specified “boundary” circle) are recursively defined as follows. A grope of class is a circle. A grope of class is an orientable surface with one boundary component. A grope of class is formed by attaching to every dual pair of basis curves on a class grope a pair of gropes whose classes add to . A curve in a topological space is a -fold commutator if and only if it extends to a continuous map of a grope of class . Thus one can ask whether being -slice implies there is a basis of curves on that bound disjointly embedded gropes of class in . Call such a link geometrically -slice.
Proposition 17 ([Cst2]).
A link is geometrically -slice if and only if .
This is proven using a construction from [S] which allows one to freely pass between class gropes and order Whitney towers. So the higher-order Arf invariants detect the difference between -sliceness and geometric -sliceness. It turns out that every value can be realized by (internal) band summing iterated Bing doubles of the figure-eight knot. Every Bing double is a boundary link, and one can choose the bands so that the sum remains a boundary link. This implies
Theorem 18 ([Cst2]).
A link has vanishing Milnor invariants of orders up to if and only if it is geometrically -slice after connected sums with internal band sums of iterated Bing doubles of the figure-eight knot.
Here (and in Theorem 20 below), the figure-eight knot can be replaced by any knot with non-trivial (classical) Arf invariant.
The added boundary links in the above theorem bound disjoint surfaces in which clearly allow immersed disks in bounded by curves representing a basis of first homology. In [CST2] we will show that this implies:
A link has vanishing Milnor invariants of orders up to if and only if its components bound disjointly embedded surfaces , with each surface a connected sum of two surfaces and such that
a basis of curves on bound disjointly embedded framed gropes of class in the complement of ,
a basis of curves on bound immersed disks in the complement of , where is the union of all class gropes on the surfaces .
This is an enormous geometric strengthening of Igusa and Orr’s result who, under the same assumption on the vanishing of Milnor invariants, show the existence of a surface and maps of class gropes, with no control on their intersections and self-intersections. Our proof uses the full power of the obstruction theory for Whitney towers, whereas they do a sophisticated computation of the third homology of the groups .
3.4. String links and the Artin representation
Let be a string link with strands embedded in . By Stallings’ Theorem [Sta], the inclusions for induce isomorphisms on all lower central quotients of the fundamental groups. In fact, the induced automorphism of the lower central quotients of the free group is explicitly characterized by conjugating the meridional generators of by longitudes. Let consist of those automorphisms of which are defined by conjugating each generator and which fix the product of generators. This leads to the Artin representation where is the set of concordance classes of pure framed string links.
The set of string links has an advantage over links in that it has a well-defined monoid structure given by stacking. Indeed, modulo concordance, it becomes a (noncommutative) group. Whitney tower filtrations can also be defined in this context, giving rise to filtrations and of this group .
Theorem 20 ([Cst5]).
The sets and are normal subgroups of which are central modulo the next order. We obtain nilpotent groups and and the associated graded are isomorphic to our previously defined groups
Finally, the Artin representation induces a well-defined epimorphism whose kernel is generated by internal band sums of iterated Bing doubles of the figure-eight knot.
The Artin representation is thus an invariant on the whole group , not just on the associated graded groups as in the case of links. It packages the total Milnor invariants on string links together into a group homomorphism.
4. Higher-order intersection invariants
Proofs of the above results depend on two essential ideas: The higher-order intersection theory of Whitney towers comes with an obstruction theory whose associated invariants take values in abelian groups of (un-rooted) trivalent trees. And by mapping to rooted trees, which correspond to iterated commutators, the obstruction theory for Whitney towers in can be identified with algebraic invariants of the bounding link in . A critical connection between these ideas is provided by the resolution of the Levine Conjecture (see below), which says that this map is an isomorphism.
In fact, it can be arranged that all singularities in a Whitney tower are contained in -ball neighborhoods of the associated trivalent trees, which sit as embedded ‘spines’; and all relations among trees in the target group are realized by controlled manipulations of the Whitney disks. Mapping to rooted trees corresponds geometrically to surgering Whitney towers to gropes, and these determine iterated commutators of meridians of the Whitney tower boundaries as in Figure 6.
4.1. Trees and intersections
All trees are unitrivalent, with cyclic orderings of the edges at all trivalent vertices, and univalent vertices labeled from an index set . A rooted tree has one unlabeled univalent vertex designated as the root. Such rooted trees correspond to formal non-associative bracketings of elements from the index set. The rooted product of rooted trees and is the rooted tree gotten by identifying the root vertices of and to a single vertex and sprouting a new rooted edge at . This operation corresponds to the formal bracket, and we identify rooted trees with formal brackets. The inner product of rooted trees and is the unrooted tree gotten by identifying the roots of and to a single non-vertex point. Note that all the univalent vertices of are labeled.
The order of a tree, rooted or unrooted, is defined to be the number of trivalent vertices, and the following associations of trees to Whitney disks and intersection points respects the notion of order given in Definition 5.
To each order zero surface is associated the order zero rooted tree consisting of an edge with one vertex labeled by , and to each transverse intersection is associated the order zero tree consisting of an edge with vertices labeled by and . The order 1 rooted Y-tree , with a single trivalent vertex and two univalent labels and , is associated to any Whitney disk pairing intersections between and . This rooted tree can be thought of as an embedded subset of , with its trivalent vertex and rooted edge sitting in , and its two other edges descending into and as sheet-changing paths.
Recursively, the rooted tree is associated to any Whitney disk pairing intersections between and (see left-hand side of Figure 7); with the understanding that if, say, is just a singleton , then denotes the order zero surface . To any transverse intersection between and any is associated the un-rooted tree (see right-hand side of Figure 7).
4.2. Intersections trees for Whitney towers
The group (for each ) is the free abelian group on (unitrivalent labeled vertex-oriented) order trees, modulo the usual AS (antisymmetry) and IHX (Jacobi) relations:
In even orders we define , and in odd orders is defined to be the quotient of by the framing relations. These framing relations are defined as the image of homomorphisms which are defined for generators by , where denotes the rooted tree gotten by replacing with a root, and the sum is over all univalent vertices of , with the original label of the univalent vertex . For example, in orders 1 and 3 the framing relations are:
The obstruction theory works as follows:
The order intersection tree of an order Whitney tower is defined to be
where the sum is over all order intersections , with the usual sign of a transverse intersection point (via certain orientation conventions, see e.g. [CST1]).
All relations in can be realized by controlled manipulations of Whitney towers, and further maneuvers allow algebraically canceling pairs of tree generators to be converted into intersection-point pairs admitting Whitney disks. As a result, we get the following partial recovery of the “algebraic cancelation implies geometric cancellation” principle available in higher dimensions:
Theorem 22 ([Cst1]).
If a collection of properly immersed surfaces in a simply-connected –manifold supports an order Whitney tower with , then is homotopic (rel ) to which supports an order Whitney tower.
4.3. Intersections trees for twisted Whitney towers
For any rooted tree we define the corresponding -tree (“twisted-tree”), denoted by , by labeling the root univalent vertex with the symbol “ ” (which will represent a “twist” in a Whitney disk normal bundle): .
The abelian group is the quotient of by the boundary-twist relations:
Here ranges over all order rooted trees (and the first equality is just a reminder of notation).
The abelian group is gotten from by including order -trees as new generators and introducing the following new relations (in addition to the IHX and antisymmetry relations on non- trees):
The left-hand symmetry relation corresponds to the fact that the framing obstruction on a Whitney disk is independent of its orientation; the middle twisted IHX relations can be realized by a Whitney move near a twisted Whitney disk, and the right-hand interior twist relations can be realized by cusp-homotopies in Whitney disk interiors. As described in [CST4], the twisted groups can naturally be identified with a universal quadratic refinement of the -valued intersection pairing on framed Whitney disks.
Recalling from Definition 13 that twisted Whitney disks only occur in even order twisted Whitney towers, intersection trees for twisted Whitney towers are defined as follows:
The order intersection tree of an order twisted Whitney tower is defined to be
where the first sum is over all order intersections and the second sum is over all order Whitney disks with twisting (computed from a consistent choice of local orientations).
By “splitting” the twisted Whitney disks [CST1] it can be arranged that , leading to signs like (or zero coefficients). The obstruction theory also holds for twisted Whitney towers:
Theorem 25 ([Cst1]).
If a collection of properly immersed surfaces in a simply-connected –manifold supports an order twisted Whitney tower with , then is homotopic (rel ) to which supports an order twisted Whitney tower.
4.4. Remark on the framing relations
The framing relations in the untwisted groups correspond to the twisted IHX relations among -trees in via a geometric boundary-twist operation which converts an order -tree to an order (untwisted) tree .
4.5. Realization maps
In [CST1] we describe how to construct surjective realization maps and by applying the operation of iterated Bing doubling. This construction is essentially the same as the well-known application of Habiro’s clasper-surgery [H] and Cochran’s realization of Milnor invariants [C], extended to twisted Bing doubling (Figures 8 and 5). To prove the realization maps are well-defined we need to use Theorems 22 and 25 respectively.
The above Conjecture 10 on the non-triviality of the higher-order Arf invariants can be succinctly rephrased as the assertion that the realization maps and are isomorphisms for all . Progress towards confirming this assertion – namely complete answers in of the cases and partial answers in the remaining cases, as described by the above-stated results – has been accomplished by identifying intersection trees with Milnor invariants, as we describe next.
4.6. Intersection trees and Milnor’s link invariants
The connection between intersection trees and Milnor invariants is via a surjective map which converts trees to rooted trees (interpreted as Lie brackets) by summing over all ways of choosing a root:
For a univalent vertex of an order (un-rooted non- ) tree denote by the Lie bracket of generators determined by the formal bracketing of indices which is gotten by considering to be a root of .
Denoting the label of a univalent vertex by , the map is defined on generators by
where the first sum is over all univalent vertices of , and the second expression lies in because the coefficient of is even.
The proof of the following theorem (which implies Theorem 14 above) shows that the map corresponds to a construction which converts Whitney towers into embedded gropes [S], via the grope duality of [KT]:
Theorem 26 ([Cst2]).
If bounds a twisted Whitney tower of order , then the total Milnor invariants vanish for , and .
Thus one needs to understand the kernel of before the obstruction theory can proceed. This is accomplished by resolving [CST3] a closely related conjecture of J. Levine [L2], as discussed next.
4.7. The Levine Conjecture and its implications
The bracket map kernel turns out to be relevant to a variety of topological settings (see e.g. the introduction to [CST3]), and was known to be isomorphic to after tensoring with , when Levine’s study of the cobordism groups of -dimensional homology cylinders [L1, L2] led him to conjecture that is in fact isomorphic to the quasi-Lie bracket map kernel , via the analogous map which sums over all choices of roots (as in the left formula for above).
Levine made progress in [L2, L3], and in [CST3] we affirm his conjecture:
Theorem 27 ([Cst3]).
is an isomorphism for all .
The proof of Theorem 27 uses techniques from discrete Morse theory on chain complexes, including an extension of the theory to complexes containing torsion. A key idea involves defining combinatorial vector fields that are inspired by the Hall basis algorithm for free Lie algebras and its generalization by Levine to quasi-Lie algebras.
As described in [CST4], Theorem 27 has several direct applications to Whitney towers, including the completion of the calculation of in three out of four cases:
Theorem 28 ([Cst4]).
are isomorphisms for . As a consequence, both the total Milnor invariants and the realization maps are isomorphisms for these orders.
The consequences listed in the second statement follow from the fact that is the composition