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Concordance of decompositions given by defining sequences

Boldizsár Kalmár [email protected]
Abstract.

We study the concordance and cobordism of decompositions associated with defining sequences and we relate them to some invariants of toroidal decompositions and to the cobordism of homology manifolds. These decompositions are often wild Cantor sets and they arise as nested intersections of knotted solid tori. We show that there are at least uncountably many concordance classes of such decompositions in the 33-sphere.

Key words and phrases:
Concordance, decomposition, Antoine’s necklace, cobordism, homology manifold.
2010 Mathematics Subject Classification:
Primary 57N70, 57M30; Secondary 57P99.

1. Introduction

We study equivalence classes of decompositions of S3S^{3} and also decompositions of other manifolds. These decompositions are given by toroidal defining sequences (we use the term toroidal for a subspace of an nn-dimensional manifold being homeomorphic to the disjoint union of finitely many copies of Sn2×D2S^{n-2}\times D^{2}) although more generally it would be possible to get similar results by considering handlebodies instead of solid tori in the defining sequences. The problem of classifying decompositions was studied by many authors. By [Sh68] so-called Antoine decompositions in 3\mathbb{R}^{3} are equivalently embedded if and only if their toroidal defining sequences can be mapped into each other by homeomorphisms of the stages. More generally [ALM68] for a decomposition GG of 3\mathbb{R}^{3} given by an arbitrary defining sequence made of handlebodies the homeomorphism type of the pair (3/G,clπG(HG))(\mathbb{R}^{3}/G,\mathrm{cl}\thinspace\pi_{G}(H_{G})), where πG\pi_{G} is the decomposition map and HGH_{G} is the union of the non-degenerate elements, is determined by the homeomorphism types of the consecutive stages of the defining sequence of GG. By [GRWŽ11] two Bing-Whitehead decompositions of S3S^{3} are equivalently embedded if and only if the stages of the toroidal defining sequences are homeomorphic to each other after some number of iterations (counting only the Bing stages). Decompositions given by defining sequences are upper semi-continuous and many shrinkability conditions are known about them. For example, Bing-Whitehead decompositions are shrinkable under some conditions [AS89, KP14] just like Antoine’s necklaces, which are wild Cantor sets. In [Že05] the maximal genus of handlebodies being associated with a defining sequence is used to study Cantor sets.

In the present paper we define the concordance of decompositions (see Section 2.3) which come with toroidal defining sequences. As for knots, slice decompositions play an important role in the classification: a decomposition is slice if each component of a defining sequence is slice in a way that the Dn1×D2D^{n-1}\times D^{2} thickened slice disk stages are nested into each other. Being concordant means the analogous concordance of the solid tori in the defining sequence and this makes the well-known knot and link concordance invariants possible to apply in order to distinguish between the concordance classes of such decompositions. For example, we show that the concordance group of decompositions of S3S^{3}, where the defining sequences have some intrinsic properties, has at least uncountably many elements, see Theorem 3.7. The uncountably many elements that we find are represented by Antoine’s necklaces.

Decompositions appear in studying manifolds, where cell-like resolutions of homology manifolds [Qu82, Qu83, Qu87, Th84, Th04] provide a tool of obtaining topological manifolds. Decompositions also appear in the proof of the Poincaré conjecture in dimension four, see [Fr82, FQ90, BKKPR21], where a cell-like decomposition of a 44-dimensional manifold yields a decomposition space which is a topological manifold. In higher dimensions the decomposition space given by a cell-like decomposition of a compact topological manifold is a homology manifold being also a topological manifold if it satisfies the disjoint disk property [Ed16]. A particular result [Ca78, Ca79, Ed80, Ed06] is that the double suspension of every integral homology 33-sphere is homeomorphic to S5S^{5}, that is for every homology 33-sphere HH there is a cell-like decomposition GG of S5S^{5} such that the decomposition space is the homology manifold Σ2H\Sigma^{2}H and since Σ2H\Sigma^{2}H satisfies the disjoint disk property, the decomposition GG is shrinkable (and this implies that the decomposition space is S5S^{5}).

Beside concordance, we also define and study another equivalence relation, which is the cobordism of decompositions, see Definition 2.15 and Section 3.2. This yields a cobordism group, which has a natural homomorphism into the cobordism group of homology manifolds [Mi90, Jo99, JR00]. We study how homological manifolds are related to the cobordism group of cell-like decompositions via taking the decomposition space. It turns out that every such decomposition space is cobordant to a topological manifold in the cobordism group of homology manifolds and they generate a subgroup isomorphic to the cobordism group of topological manifolds, see Proposition 3.11. Often we state and prove our results only for unoriented cobordisms but all the arguments obviously work for the oriented cobordisms as well giving the corresponding results.

The paper is organized as follows. In Section 2 we give some basic lemmas and the definitions of the most important notions and in Section 3 we state and prove our main results.

The author would like to thank the referee for the helpful comments, which improved the paper.

2. Preliminaries

2.1. Cell-like decompositions

Throughout the paper we suppose that if XX is a compact manifold with boundary and YY is a compact manifold with corners, then an embedding e:YXe\colon\thinspace Y\to X is such that the corners of YY are mapped into X\partial X and the pairs of boundary components near the corners of YY are mapped into intX\mathrm{int}X and into X\partial X, respectively. We also suppose that e(intY)intXe(\mathrm{int}Y)\subset\mathrm{int}X. If YY has no corners, then Xe(Y)=\partial X\cap e(Y)=\emptyset. We generalize the notions of defining sequence, cellular set and cell-like set in the obvious way for manifolds with boundary as follows. Recall that a decomposition of a topological space XX is a collection of pairwise disjoint subsets of XX whose union is equal to XX.

Definition 2.1 (Defining sequence for a subset).

Let XX be an nn-dimensional manifold with possibly non-empty boundary. A defining sequence for a subset CXC\subset X is a sequence

c:𝒫(X)c\colon\thinspace\mathbb{N}\to\mathcal{P}(X)
C0,C1,C2,,Cn,C_{0},C_{1},C_{2},\ldots,C_{n},\ldots

of compact nn-dimensional submanifolds-with-boundary possibly with corners in XX such that

  1. (1)

    every Cn+1C_{n+1} has a neighbourhood UU such that UCnU\subset C_{n},

  2. (2)

    in every component of CnC_{n} there is a component of Cn+1C_{n+1},

  3. (3)

    n=0Cn=C\cap_{n=0}^{\infty}C_{n}=C and

  4. (4)

    if X\partial X\neq\emptyset, then there is an ε>0\varepsilon>0 such that X×[0,ε)\partial X\times[0,\varepsilon) is a collar neighbourhood of X\partial X and for every CnC_{n} such that CnXC_{n}\cap\partial X\neq\emptyset we have Cn(X×[0,ε))=(CnX)×[0,ε)C_{n}\cap(\partial X\times[0,\varepsilon))=(C_{n}\cap\partial X)\times[0,\varepsilon).

A decomposition of XX defined by the defining sequence cc is the triple (X,𝒟,C)(X,\mathcal{D},C), where C=n=0CnC=\cap_{n=0}^{\infty}C_{n} and the elements of 𝒟𝒫(X)\mathcal{D}\subset\mathcal{P}(X) are

  1. (1)

    the connected components of CC and

  2. (2)

    the points in XCX-C.

We denote the decomposition map by π\pi.

Observe that for a decomposition (X,𝒟,C)(X,\mathcal{D},C) the set CC is non-empty and each of the non-degenerate elements is a subset of CC. There could be singletons in CC as well. For example in the case of an Antoine’s necklace there are no non-degenerate elements, we choose CC to be the Cantor set Antoine’s necklace itself and so CC consists of singletons. Every decomposition defined by some defining sequence is upper semi-continuous. A decomposition 𝒟\mathcal{D} of a manifold induces a decomposition on its boundary by intersecting the decomposition elements with the boundary. The decomposition of the boundary X\partial X induced by a defining sequence in XX is upper semi-continuous. This induced decomposition is given by an induced defining sequence CnXC_{n}\cap\partial X if Dn,kXD_{n,k}\cap\partial X\neq\emptyset for every component Dn,kD_{n,k} of each CnC_{n}. If all CnC_{n} in a defining sequence are connected, then n=0Cn\cap_{n=0}^{\infty}C_{n} is connected.

Definition 2.2 (Cell-like set).

A compact subset CC of a metric space XX is cell-like if for every neighbourhood UU of CC there is a neighbourhood VV of CC in UU such that the inclusion map VUV\to U is homotopic in UU to a constant map. A decomposition is called cell-like if each of its decomposition elements is cell-like.

Cell-like sets given by defining sequences are connected because if the connected components could be separated by open neighbourhoods, then a homotopy could not deform the set into one single point in the neighbourhoods.

A space XX is finite dimensional if for every open cover 𝒰\mathcal{U} of XX there exists a refinement 𝒱\mathcal{V} of 𝒰\mathcal{U} such that no points of XX lies in more than KXK_{X} of the elements of 𝒱\mathcal{V}, where KXK_{X} is a constant depending only on XX.

Lemma 2.3.

Let 𝒟\mathcal{D} be a decomposition of a manifold XX possibly with non-empty boundary given by a defining sequence. Then the decomposition space X/𝒟X/\mathcal{D} is finite dimensional.

Proof.

If XX has no boundary, then the statement follows from Theorem 2 and Proposition 3 in [Da86, Chapter 34]. If XX has non-empty boundary, then the argument is also similar. ∎

2.2. Homology manifolds

Recall that a metric space YY is an absolute neighbourhood retract (or ANR for short) if for every metric space ZZ and embedding i:YZi\colon\thinspace Y\to Z such that i(Y)i(Y) is closed there is a neighbourhood UU of i(Y)i(Y) in ZZ which retracts onto i(Y)i(Y), that is r|i(Y)=idi(Y)r|_{i(Y)}=\mathrm{id}_{i(Y)} for some map r:Ui(Y)r\colon\thinspace U\to i(Y). It is a fact that every manifold is an ANR. A space is called a Euclidean neighbourhood retract (or ENR for short) if it can be embedded into a Euclidean space as a closed subset so that it is a retract of some of its neighbourhoods. It is well-known that a space is an ENR if and only if it is a locally compact, finite dimensional, separable ANR.

Definition 2.4 (Homology manifold).

Let n0n\geq 0 and let XX and YY be finite dimensional ANR spaces, where YY is a closed subset of XX. Suppose that for every xXx\in X we have

  1. (1)

    Hk(X,X{x})=0H_{k}(X,X-\{x\})=0 for knk\neq n and

  2. (2)

    Hn(X,X{x})H_{n}(X,X-\{x\}) is isomorphic to \mathbb{Z} if xXYx\in X-Y and it is isomorphic to 0 if xYx\in Y.

Then XX is an nn-dimensional homology manifold. The set of points xYx\in Y are the boundary points of XX and the set YY is denoted by X\partial X. A homology manifold is called closed if it is compact and has no boundary.

Since locally compact and separable homology manifolds are ENR spaces, a locally compact and separable homology manifold is called an ENR homology manifold. In [Mi90] it is proved that for n1n\geq 1 and for every compact and locally compact nn-dimensional homology manifold XX the set of boundary points X\partial X is an (n1)(n-1)-dimensional homology manifold.

Sometimes a space XX without the ANR property but having Hk(X,X{x})=0H_{k}(X,X-\{x\})=0 for knk\neq n and Hn(X,X{x})=H_{n}(X,X-\{x\})=\mathbb{Z} in the sense of Čech homology is also called a homology manifold. These spaces arise as quotient spaces of acyclic decompositions of topological manifolds [DW83] while ANR homology manifolds are often homeomorphic to quotients of cell-like decompositions [Qu82, Qu83, Qu87].

In the case of cell-like decompositions the decomposition spaces are homology manifolds if they are finite dimensional essentially because of the Vietoris-Begle theorem [DV09, Theorem 0.4.1]. In more detail, we will use the following. Let XX^{\prime} be a compact nn-dimensional manifold with possibly non-empty boundary, let YY be X×[0,1]\partial X^{\prime}\times[0,1] and attach YY to XX^{\prime} as a collar to get a manifold XX.

Lemma 2.5.

Let 𝒟\mathcal{D}^{\prime} be a cell-like decomposition of XX^{\prime} given by a defining sequence such that XX^{\prime} contains a small open set (intersecting the possibly non-empty boundary) which consists of singletons. Suppose that the induced decomposition on X\partial X^{\prime} is cell-like and it is given by the induced defining sequence. Suppose that in YY a cell-like decomposition \mathcal{E} is given, where \mathcal{E} is the product of the decomposition induced by 𝒟\mathcal{D}^{\prime} on X\partial X^{\prime} and the trivial decomposition of [0,1][0,1]. Denote by 𝒟\mathcal{D} the resulting decomposition on XX. Then X/𝒟X/\mathcal{D} is an nn-dimensional ENR homology manifold with possibly non-empty boundary. The boundary points of X/𝒟X/\mathcal{D} are exactly the points of the ENR homology manifold π(X)\pi(\partial X).

Proof.

We have to show that the quotient space

X/𝒟X/\mathcal{D}

is an nn-dimensional homology manifold with boundary the homology manifold π(X)\pi(\partial X). Take the closed manifold

XφX,X\cup_{\varphi}X,

where φ:XX\varphi\colon\thinspace\partial X\to\partial X is the identity map.

The decomposition space X/𝒟X^{\prime}/\mathcal{D}^{\prime} (that is the part of the decomposition space X/𝒟X/\mathcal{D} which is obtained from XX^{\prime}) is finite dimensional by Lemma 2.3. The doubling of the decomposition 𝒟\mathcal{D} on XφXX\cup_{\varphi}X yields a finite dimensional quotient space, we get this by using estimations for the covering dimension, see [HW41] and [Da86, Corollary 2.4A]. So the decomposition space PP obtained by factorizing XφXX\cup_{\varphi}X by the double of 𝒟\mathcal{D} is a closed finite dimensional homology manifold by [DV09, Proposition 8.5.1]. Since a small neighbourhood of a singleton results an open set in PP homeomorphic to n\mathbb{R}^{n}, it is nn-dimensional. We obtain the space X/𝒟X/\mathcal{D} by cutting PP into two pieces along π(X)\pi(\partial X). Because of a similar argument the space π(X)\pi(\partial X) is a closed (n1)(n-1)-dimensional homology manifold. The set π(X)\pi(\partial X) is closed in the decomposition space X/𝒟X/\mathcal{D} since 𝒟\mathcal{D} is upper semi-continuous and X\partial X is closed. Also, the homology group Hn(X/𝒟;X/𝒟{p})H_{n}(X/\mathcal{D};X/\mathcal{D}-\{p\}) is equal to 0 for every pπ(X)p\in\pi(\partial X). So π(X)\pi(\partial X) is the boundary of X/𝒟X/\mathcal{D}.

Moreover the space X/𝒟X/\mathcal{D} is a locally compact separable metric space because XX is so. By [DV09, Corollary 7.4.8] the space X/𝒟X/\mathcal{D} is an ANR so it follows that it is an ENR. The same holds for π(X)\pi(\partial X). ∎

Definition 2.6 (Cobordism of homology manifolds).

The closed nn-dimensional homology manifolds X1X_{1} and X2X_{2} are cobordant if there exists a compact (n+1)(n+1)-dimensional homology manifold WW such that W\partial W is homeomorphic to the disjoint union of X1X_{1} and X2X_{2}. The induced cobordism group (the group operation is the disjoint union) is denoted by 𝔑nH\mathfrak{N}_{n}^{H}. In a similar way the induced oriented cobordism group is denoted by ΩnH\Omega_{n}^{H}.

Note that the connected sum of homology manifolds does not always exist. Analogously let 𝔑nE\mathfrak{N}_{n}^{E} and ΩnE\Omega_{n}^{E} denote the cobordism group and oriented cobordism group of ENR homology manifolds (the cobordisms are also ENR), respectively.

Almost all oriented cobordism groups ΩnH\Omega_{n}^{H} are computed [BFMW96, Jo99, JR00]:

ΩnH={if n=00if n=1,2ΩnTOP[8+1]if n6,\Omega_{n}^{H}=\left\{\begin{array}[]{cc}\mathbb{Z}&\mbox{if $n=0$}\\ 0&\mbox{if $n=1,2$}\\ \Omega_{n}^{TOP}[8\mathbb{Z}+1]&\mbox{if $n\geq 6$},\end{array}\right.

where ΩnTOP\Omega_{n}^{TOP} denotes the cobordism group of topological manifolds and the group

ΩnTOP[8+1]\Omega_{n}^{TOP}[8\mathbb{Z}+1]

denotes the group of finite linear combinations i8+1ωii\sum_{i\in 8\mathbb{Z}+1}\omega_{i}i of cobordism classes of topological manifolds. By [Ma71, Corollary 4.2] the oriented cobordism group of manifolds Ωn\Omega_{n} is always a subgroup of ΩnH\Omega_{n}^{H}.

A resolution of a homology manifold NN is a topological manifold MM and a cell-like decomposition of MM such that the decomposition space is homeomorphic to the homology manifold NN, the quotient map π\pi is proper and π1(N)=M\pi^{-1}(\partial N)=\partial M. By [Qu82, Qu83, Qu87] homology manifolds are resolvable if a local obstruction is equal to 11, more precisely we have the following.

Theorem 2.7 ([Qu82, Qu83, Qu87]).

For every n4n\geq 4 and every non-empty connected nn-dimensional ENR homology manifold NN there is an integer local obstruction i(N)8+1i(N)\in 8\mathbb{Z}+1 such that

  1. (1)

    if UNU\subset N is open, then i(U)=i(N)i(U)=i(N),

  2. (2)

    if N\partial N\neq\emptyset, then i(N)=i(N)i(\partial N)=i(N),

  3. (3)

    i(N×N1)=i(N)i(N1)i(N\times N_{1})=i(N)i(N_{1}) for any other homology manifold N1N_{1},

  4. (4)

    if dimN=4\dim N=4 and N\partial N is a manifold, then there is a resolution if and only if i(N)=1i(N)=1 and

  5. (5)

    if dimN5\dim N\geq 5, then there is a resolution if and only if i(N)=1i(N)=1.

By [Th84, Th04] a closed 33-dimensional ENR homology manifold NN is resolvable if its singular set has general position dimension less than or equal to one, that is any map of a disk into NN can be approximated by one whose image meets the singular set (i.e. the set of non-manifold points) of NN in a 0-dimensional set.

Lemma 2.8.

Let M1M_{1} and M2M_{2} be two closed nn-dimensional manifolds, where n4n\geq 4. If both of them are resolutions of the ENR homology manifold NN, then M1M_{1} and M2M_{2} are cobordant as manifolds.

Proof.

If there are two resolutions f1:M1Nf_{1}\colon\thinspace M_{1}\to N and f2:M2Nf_{2}\colon\thinspace M_{2}\to N of a closed nn-dimensional homology manifold NN, then as in the proof of [Qu82, Theorem 2.6.1] take a resolution

YXf1Xf2Y\to X_{f_{1}}\cup X_{f_{2}}

of the double mapping cylinder Xf1Xf2X_{f_{1}}\cup X_{f_{2}} of the maps f1f_{1} and f2f_{2} by applying [Qu83, Theorem 1.1] and [Qu87]. This resolution exists because Xf1Xf2X_{f_{1}}\cup X_{f_{2}} is an (n+1)(n+1)-dimensional ENR homology manifold and i(Xf1Xf2)=1i(X_{f_{1}}\cup X_{f_{2}})=1. Let

Xf1Xf2N×[1,1]X_{f_{1}}\cup X_{f_{2}}\to N\times[-1,1]

be the natural map of the double mapping cylinder onto N×[1,1]N\times[-1,1], where the target NN of the two mapping cylinders is mapped onto N×{0}N\times\{0\}.

It follows that the composition

YXf1Xf2N×[1,1]Y\to X_{f_{1}}\cup X_{f_{2}}\to N\times[-1,1]

is a resolution, moreover by [Qu83, Theorem 1.1] the cell-like map YXf1Xf2Y\to X_{f_{1}}\cup X_{f_{2}} can be chosen so that it is a homeomorphism over the boundary hence YY is a cobordism between M1M_{1} and M2M_{2}. ∎

2.3. Concordance and cobordism of decompositions

We will study decompositions given by defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots such that each CnC_{n} is a disjoint union of solid tori. We remark that more generally all the following notions work for decompositions whose stages are handlebodies instead of just tori. In a closed nn-dimensional manifold MM instead of decompositions (M,𝒟,A)(M,\mathcal{D},A) we will consider decompositions with some thickened link which contains the set AA so in the following a decomposition in MM is a quadruple (M,𝒟,A,L)(M,\mathcal{D},A,L), where LML\subset M is the thickened link and ALA\subset L. For example an Antoine’s necklace is situated inside an unknotted solid torus while it can be knotted in many different ways in the solid torus.

Definition 2.9 (Concordance of decompositions).

Let M1M_{1} and M2M_{2} be closed nn-dimensional manifolds. The decompositions (M1,𝒟1,A,L1)(M_{1},\mathcal{D}_{1},A,L_{1}) and (M2,𝒟2,B,L2)(M_{2},\mathcal{D}_{2},B,L_{2}) are cylindrically related if there exist toroidal defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots for AA and D0,D1,D2,D_{0},D_{1},D_{2},\ldots for BB and there exists a defining sequence E0,E1,E2,E_{0},E_{1},E_{2},\ldots for a decomposition \mathcal{E} of a compact (n+1)(n+1)-dimensional manifold WW such that

  1. (1)

    C0=L1C_{0}=L_{1} and D0=L2D_{0}=L_{2},

  2. (2)

    W=M1M2\partial W=M_{1}\sqcup M_{2},

  3. (3)

    each EiE_{i} is homeomorphic to Ci×[0,1]C_{i}\times[0,1] and

  4. (4)

    each EiE_{i} bounds the components of CiM1C_{i}\subset M_{1} and DiM2D_{i}\subset M_{2} that is Ci×{0}C_{i}\times\{0\} corresponds to CiC_{i} and Ci×{1}C_{i}\times\{1\} corresponds to DiD_{i}.

Two decompositions (M1,𝒟1,A,L1)(M_{1},\mathcal{D}_{1},A,L_{1}) and (M2,𝒟2,B,L2)(M_{2},\mathcal{D}_{2},B,L_{2}) are concordant if there exist closed nn-dimensional manifolds M1,,MkM_{1}^{\prime},\ldots,M_{k}^{\prime} and decompositions (Mi,𝒟i,Ai,Li)(M_{i}^{\prime},\mathcal{D}_{i}^{\prime},A_{i}^{\prime},L_{i}^{\prime}) for every i=1,,ki=1,\ldots,k such that

  1. (1)

    (M1,𝒟1,A,L1)(M_{1},\mathcal{D}_{1},A,L_{1}) is cylindrically related to (M1,𝒟1,A1,L1)(M_{1}^{\prime},\mathcal{D}_{1}^{\prime},A_{1}^{\prime},L_{1}^{\prime}), also for i=1,,k1i=1,\ldots,k-1 every (Mi,𝒟i,Ai,Li)(M_{i}^{\prime},\mathcal{D}_{i}^{\prime},A_{i}^{\prime},L_{i}^{\prime}) is cylindrically related to (Mi+1,𝒟i+1,Ai+1,Li+1)(M_{i+1}^{\prime},\mathcal{D}_{i+1}^{\prime},A_{i+1}^{\prime},L_{i+1}^{\prime}) and (Mk,𝒟k,Ak,Lk)(M_{k}^{\prime},\mathcal{D}_{k}^{\prime},A_{k}^{\prime},L_{k}^{\prime}) is cylindrically related to (M2,𝒟2,B,L2)(M_{2},\mathcal{D}_{2},B,L_{2}) and

  2. (2)

    for each AiMiA_{i}^{\prime}\subset M_{i}^{\prime}, where i=1,,ki=1,\ldots,k, the two toroidal defining sequences Ci,0,Ci,1,C_{i,0}^{\prime},C_{i,1}^{\prime},\ldots and Ci,0′′,Ci,1′′,C_{i,0}^{\prime\prime},C_{i,1}^{\prime\prime},\ldots in MiM_{i}^{\prime} appearing in these successive cylindrically related decompositions are such that the 0-th stages Ci,0C_{i,0}^{\prime} and Ci,0′′C_{i,0}^{\prime\prime} are equal as subsets of MiM_{i}^{\prime}.

Being concordant is an equivalence relation and the equivalence classes are called concordance classes.

Hence being concordant implies that the two decompositions are in the same equivalence class of the equivalence relation generated by being cylindrically related, that is the two decompositions can be connected by a finite number of cylindrically related decompositions. Being concordant also implies that the 0-th stages of two toroidal defining sequences for the two decompositions are connected by a single concordance in the usual sense. Clearly in the definition each EiE_{i} intersects some fixed collar of W\partial W as the defining sequence in (4) of Definition 2.1. The concordance classes form a commutative semigroup under the operation “disjoint union”. Moreover this semigroup is a monoid because the neutral element is the “empty manifold”, that is the empty set \emptyset. To have a more meaningful neutral element we define the following.

Definition 2.10 (Slice decomposition).

Let MM be a closed nn-dimensional manifold and let (M,𝒟,A,L)(M,\mathcal{D},A,L) be a decomposition of MM such that there exists a toroidal defining sequence C0,C1,C2,C_{0},C_{1},C_{2},\ldots with C0=LC_{0}=L for AA. Then (M,𝒟,A,L)(M,\mathcal{D},A,L) is slice if it is concordant to a decomposition (M,𝒟,A,L)(M^{\prime},\mathcal{D}^{\prime},A^{\prime},L^{\prime}) with defining sequence C0,C1,C2,C_{0}^{\prime},C_{1}^{\prime},C_{2}^{\prime},\ldots with C0=LC_{0}^{\prime}=L^{\prime} such that there exists a defining sequence E0,E1,E2,E_{0},E_{1},E_{2},\ldots for a decomposition \mathcal{E} of the (n+1)(n+1)-dimensional manifold M×[0,1)M^{\prime}\times[0,1), where each EiE_{i} consists of finitely many Dn1×D2D^{n-1}\times D^{2} bounding the torus components Sn2×D2S^{n-2}\times D^{2} of CiM×{0}C_{i}^{\prime}\subset M^{\prime}\times\{0\}.

Analogously to Definitions 2.9 and 2.10, we define the oriented concordance of decompositions by requiring all the manifolds to be oriented in the usual consistent way, in this way we also get a corresponding monoid. Observe that the set of concordance classes of slice decompositions is a submonoid of the monoid of concordance classes of decompositions. To obtain a group we factor out the concordance classes by the classes represented by the slice decompositions and also by the classes of the form

[(M,𝒟,A,L)]+[(M,𝒟,A,L)],[(M,\mathcal{D},A,L)]+[(-M,\mathcal{D},A,L)],

where M-M denotes the opposite orientation. Observe that all these classes form a submonoid.

Definition 2.11 (Decomposition concordance group).

Define the relation \sim on the set of concordance classes of decompositions by the following rule: aba\sim b exactly if there exist slice decompositions s1s_{1} and s2s_{2} and decompositions (M,𝒟,A,L)(M,\mathcal{D},A,L) and (M,𝒟,A,L)(M^{\prime},\mathcal{D}^{\prime},A^{\prime},L^{\prime}) such that

a+[s1]+[(M,𝒟,A,L)]+[(M,𝒟,A,L)]=b+[s2]+[(M,𝒟,A,L)]+[(M,𝒟,A,L)].a+[s_{1}]+[(M,\mathcal{D},A,L)]+[(-M,\mathcal{D},A,L)]=b+[s_{2}]+[(M^{\prime},\mathcal{D}^{\prime},A^{\prime},L^{\prime})]+[(-M^{\prime},\mathcal{D}^{\prime},A^{\prime},L^{\prime})].

The relation \sim is a congruence and we obtain a commutative group by factoring out by this congruence. We call this group the oriented decomposition concordance group and denote it by Γn\Gamma_{n}.

If we confine the closed nn-dimensional manifolds to SnS^{n} and the cobordisms to Sn×[0,1]S^{n}\times[0,1], then we obtain something similar to the classical link concordance. For the convenience of the reader we repeat the definitions.

Definition 2.12 (Concordance group of decompositions in SnS^{n}).

Let (Sn,𝒟1,A,L1)(S^{n},\mathcal{D}_{1},A,L_{1}) and (Sn,𝒟2,B,L2)(S^{n},\mathcal{D}_{2},B,L_{2}) be decompositions of SnS^{n} in the complement of \infty. They are cylindrically related if there exist toroidal defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots for AA and D0,D1,D2,D_{0},D_{1},D_{2},\ldots for BB and there exists a defining sequence E0,E1,E2,E_{0},E_{1},E_{2},\ldots for a decomposition \mathcal{E} of the compact (n+1)(n+1)-dimensional manifold Sn×[0,1]S^{n}\times[0,1] in the complement of {}×[0,1]\{\infty\}\times[0,1] such that

  1. (1)

    C0=L1C_{0}=L_{1} and D0=L2D_{0}=L_{2},

  2. (2)

    each EiE_{i} is homeomorphic to Ci×[0,1]C_{i}\times[0,1] and

  3. (3)

    each EiE_{i} bounds the components of CiSn×{0}C_{i}\subset S^{n}\times\{0\} and DiSn×{1}D_{i}\subset S^{n}\times\{1\}.

Two decompositions are concordant if

  1. (1)

    they are in the same equivalence class of the equivalence relation generated by being cylindrically related so the two decompositions can be connected by a finite number of cylindrically related decompositions and

  2. (2)

    the 0-th stages of the defining sequences appearing in this sequence of cylindrically related decompositions are concordant as thickened links in the usual sense.

The obtained equivalence classes are called concordance classes. If two decompositions of SnS^{n} are given by defining sequences, then in the connected sum (at \infty) of the two nn-spheres the “disjoint union” induces a commutative semigroup operation on the set of concordance classes. Then by factoring out by the submonoid of classes of slice decompositions and classes of the form [(Sn,𝒟,A,L)]+[(Sn,𝒟,A,L)][(S^{n},\mathcal{D},A,L)]+[(-S^{n},\mathcal{D},A,L)] we get a group called the decomposition concordance group in SnS^{n}. We denote this group by Δn\Delta_{n}.

For example, the Whitehead decomposition in S3S^{3} is slice [Fr82] and the Bing decomposition in S3S^{3} is also slice because the Bing double of the unknot is slice. Observe that the Bing decomposition (S3,,C)(S^{3},\mathcal{B},C) has only singletons, where CC is a wild Cantor set. As another example, a defining sequence in S3S^{3} given by the replicating pattern of a solid torus and inside of it a link made of a sequence of ribbon knots linked with each other circularly can yield a slice decomposition.

Since being concordant implies that the two decompositions can be connected by a finite number of cylindrically related decompositions, all invariants of concordance classes defined through defining sequences are invariant under choosing another defining sequence for the same decomposition (while leaving the 0-th stage unchanged). For n=3n=3 in the following we restrict ourselves only to such toroidal defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots of decompositions of the closed nn-dimensional manifolds in Definitions 2.9-2.12 which satisfy the following conditions:

Definition 2.13 (Admissible defining sequences and decompositions).

Suppose

  1. (1)

    for m1m\geq 1 each CmC_{m} has at least four components in a component of Cm1C_{m-1} and each component TT of CmC_{m} is linked to exactly two other components of CmC_{m} in the ambient space S3S^{3} with algebraic linking number non-zero and the splitting number of TT and each of the other components is equal to 0,

  2. (2)

    for m1m\geq 1 the components A1,,AkA_{1},\ldots,A_{k} of CmC_{m} which are in a component DD of Cm1C_{m-1} are linked in such a way that if a component AiA_{i} is null-homotopic in a solid torus TT whose boundary is disjoint from all AiA_{i}, then all AiA_{i} are in this solid torus TT,

  3. (3)

    m=0Cm\cap_{m=0}^{\infty}C_{m} is not separated by and not contained in any 22-dimensional sphere SS for which SCmS\subset C_{m} for some mm,

  4. (4)

    every embedded circle in the boundary of a component of CmC_{m} which bounds no 22-dimensional disk in this boundary cannot be shrunk to a point in the complement of m=0Cm\cap_{m=0}^{\infty}C_{m}.

We call such defining sequences and decompositions admissible.

Proposition 2.14.

In the connected sum (at \infty) of two 33-spheres the “disjoint union” as in Definition 2.12 of two admissible toroidal decompositions is an admissible toroidal decomposition.

Proof.

Checking the conditions (1)-(4) in Definition 2.13 is obvious, details are left to the reader. ∎

Then we denote the arising concordance group in S3S^{3} by Δ3a\Delta_{3}^{a}. For example, Antoine’s necklaces (or Antoine’s decompositions) for n=3n=3 have defining sequences satisfying these conditions [Sh68]. We note that by [Sh68] their defining sequences also have the property of simple chain type, which means that the torus components are unknotted and they are linked like the Hopf link. We have the natural group homomorphisms

Δ3aΔ3 and Δ3Γ3\Delta_{3}^{a}\to\Delta_{3}\mbox{\ \ \ \ \ and\ \ \ \ }\Delta_{3}\to\Gamma_{3}

and also for arbitrary nn the group homomorphism

ΔnΓn.\Delta_{n}\to\Gamma_{n}.

We will show that the number of elements of the group Δ3a\Delta_{3}^{a} is at least uncountable.

Now we define cobordism of decompositions, where we restrict ourselves to cell-like decompositions (not necessarily admissible) at the cobordisms and at the representatives as well.

Definition 2.15 (Cobordism of decompositions).

Let M1M_{1} and M2M_{2} be closed nn-dimensional manifolds and let (M1,𝒟1,A)(M_{1},\mathcal{D}_{1},A) and (M2,𝒟2,B)(M_{2},\mathcal{D}_{2},B) be cell-like decompositions such that there exist toroidal defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots for AA and D0,D1,D2,D_{0},D_{1},D_{2},\ldots for BB. Then (M1,𝒟1,A)(M_{1},\mathcal{D}_{1},A) and (M2,𝒟2,B)(M_{2},\mathcal{D}_{2},B) are coupled if there exists a defining sequence E0,E1,E2,E_{0},E_{1},E_{2},\ldots for a cell-like decomposition \mathcal{E} of a compact (n+1)(n+1)-dimensional manifold WW such that

  1. (1)

    W=M1M2\partial W=M_{1}\sqcup M_{2},

  2. (2)

    each EiE_{i} is homeomorphic to the disjoint union of finitely many manifolds Pjn1×D2P_{j}^{n-1}\times D^{2}, j=1,mij=1,\ldots m_{i}, where all Pjn1P_{j}^{n-1} are compact (n1)(n-1)-dimensional manifolds and

  3. (3)

    each EiE_{i} bounds the components of CiC_{i} and DiD_{i}.

We attach a collar W×[0,1]\partial W\times[0,1] to WW along its boundary and extend the decomposition \mathcal{E} to the collar by taking the product of 𝒟1\mathcal{D}_{1} and 𝒟2\mathcal{D}_{2} with the trivial decomposition on [0,1][0,1], respectively. We say that this extended manifold W(W×[0,1])W\cup(\partial W\times[0,1]) and its decomposition is a coupling between (M1,𝒟1,A)(M_{1},\mathcal{D}_{1},A) and (M2,𝒟2,B)(M_{2},\mathcal{D}_{2},B). Finally, two decompositions are cobordant if they are in the same equivalence class of the equivalence relation generated by being coupled. The generated equivalence classes are called cobordism classes.

Clearly each EiE_{i} intersects some fixed collar of W\partial W as the defining sequence in (4) of Definition 2.1. The cobordism classes form a commutative group under the operation “disjoint union”. Denote this group by n\mathcal{B}_{n}.

We will show that for a cobordism between arbitrary given cell-like decompositions 𝒟1,2\mathcal{D}_{1,2} as in Definition 2.15 if we take the decomposition space, then we get a group homomorphism into the cobordism group of homology manifolds.

3. Results

3.1. Computations in the concordance groups

We are going to define invariants of elements of the group Δ3a\Delta_{3}^{a}. With the help of these invariants, we will show that the group Δ3a\Delta_{3}^{a} has at least uncountably many elements.

Definition 3.1.

For a given defining sequence C0,C1,C2,,Cn,C_{0},C_{1},C_{2},\ldots,C_{n},\ldots in S3S^{3} let

nC0,C1,C2,=(n0,n1,n2,)n_{C_{0},C_{1},C_{2},\ldots}=(n_{0},n_{1},n_{2},\ldots)

be the sequence of the numbers of components of the manifolds C0,C1,C2,C_{0},C_{1},C_{2},\ldots.

If two decompositions of S3S^{3} as in Definition 2.12 are cylindrically related, then they have defining sequences C0,C1,C2,C_{0},C_{1},C_{2},\ldots and D0,D1,D2,D_{0},D_{1},D_{2},\ldots such that

nC0,C1,C2,=nD0,D1,D2,.n_{C_{0},C_{1},C_{2},\ldots}=n_{D_{0},D_{1},D_{2},\ldots}.

By [Sh68, Theorem 3] for canonical defining sequences of an Antoine’s necklace (or an Antoine decomposition) the sequence nC0,C1,C2,n_{C_{0},C_{1},C_{2},\ldots} uniquely exists (note that C0C_{0} is only an unknotted solid torus which is not appearing in [Sh68]).

Proposition 3.2.

Let (S3,𝒟,A,C0)(S^{3},\mathcal{D},A,C_{0}) be an admissible decomposition and let C0,C1,C2,C_{0},C_{1},C_{2},\ldots and D0,D1,D2,D_{0},D_{1},D_{2},\ldots be admissible defining sequences for (S3,𝒟,A,C0)(S^{3},\mathcal{D},A,C_{0}), where we suppose that C0=D0C_{0}=D_{0}. Then we have

nC0,C1,C2,=nD0,D1,D2,.n_{C_{0},C_{1},C_{2},\ldots}=n_{D_{0},D_{1},D_{2},\ldots}.
Proof.

Suppose that C0,C1,C2,C_{0},C_{1},C_{2},\ldots and D0,D1,D2,D_{0},D_{1},D_{2},\ldots are admissible defining sequences for a decomposition (S3,𝒟,A,C0)(S^{3},\mathcal{D},A,C_{0}) such that C0=D0C_{0}=D_{0}. Of course

n=0Cn=A=n=0Dn.\cap_{n=0}^{\infty}C_{n}=A=\cap_{n=0}^{\infty}D_{n}.

We use an algorithm applied in [Sh68, Proof of Theorem 2]. We restrict ourselves to one component of C0C_{0} and to the components of the defining sequences in it, the following argument works the same way for the other components. We can suppose that C1D1\partial C_{1}\cap\partial D_{1} is a closed 11-dimensional submanifold of S3S^{3}. Suppose some component PP of C1D1\partial C_{1}\cap\partial D_{1} bounds a 22-dimensional disk QD1Q\subset\partial D_{1}. Also suppose that PP is an innermost component of C1D1\partial C_{1}\cap\partial D_{1} in D1\partial D_{1} so intQC1=\mathrm{int}Q\cap\partial C_{1}=\emptyset. By (4) in Definition 2.13 if PP does not bound a disk QQ^{\prime} in C1\partial C_{1}, then PP is not homotopic to constant in the complement of AA but then PP cannot bound the disk QD1Q\subset\partial D_{1}. Hence PP bounds a disk QC1Q^{\prime}\subset\partial C_{1} as well. Then the interior of the sphere QQQ\cup Q^{\prime} does not intersect AA because of (3) in Definition 2.13. So we can modify C1C_{1} by pushing QQ^{\prime} through the sphere QQQ\cup Q^{\prime} by a self-homeomorphism of the complement of AA and hence we obtain fewer circles in the new C1D1\partial C_{1}\cap\partial D_{1}. After repeating these steps finitely many times we obtain a new C1C_{1} such that C1D1\partial C_{1}\cap\partial D_{1} contains no circles which bound disks on C1D1\partial C_{1}\cup\partial D_{1}. Similarly, by further adjusting C1C_{1} in the complement of AA as written on [Sh68, page 1198] in order to eliminate the circles in C1D1\partial C_{1}\cap\partial D_{1} which bound annuli we finally obtain a C1C_{1} such that

  • the intersection C1D1\partial C_{1}\cap\partial D_{1} is empty,

  • no component of C1C_{1} is disjoint from all the components of D1D_{1} and vice versa,

  • each component of C1C_{1} is inside a component of D1D_{1} or it contains some components of D1D_{1}.

Then we can see that there is a bijection between the number of components of C1C_{1} and D1D_{1} because of the following.

If a component of C1C_{1} is in intD1\mathrm{int}D_{1} and it is homotopic to constant in intD1\mathrm{int}D_{1}, then all the other components of C1C_{1} are in the same component of intD1\mathrm{int}D_{1} by (2) in Definition 2.13. This would result that no part of AA is in other components of D1D_{1}, which would contradict to (1) in Definition 2.13 so no component of C1C_{1} in intD1\mathrm{int}D_{1} is homotopic to constant in intD1\mathrm{int}D_{1}. The same holds if we switch the roles of C1C_{1} and D1D_{1}. This means that

  • the winding number of a component TT of C1C_{1} in the component of D1D_{1} which contains TT is not equal to 0 and the same holds for D1D_{1} and C1C_{1} with opposite roles.

Furthermore suppose that TT is some component of D1D_{1} and TT contains at least two components T1T_{1} and T2T_{2} of C1C_{1}. Then TT is linking with other component TT^{\prime} of D1D_{1} by (1) in Definition 2.13 with algebraic linking number non-zero. Let T3T_{3} be a component of C1C_{1} such that T3TT_{3}\subset T^{\prime} or TT3T^{\prime}\subset T_{3}. If T3TT_{3}\subset T^{\prime}, then T1T_{1} and T2T_{2} are linking with T3T_{3} with algebraic linking number non-zero. If TT3T^{\prime}\subset T_{3}, then TT is not in T3T_{3} because for example T1T_{1} cannot be in T3T_{3}. But then TT is linking with T3T_{3} with algebraic linking number non-zero since the same holds for TT and TT^{\prime}. So again we obtained that T1T_{1} and T2T_{2} are linking with T3T_{3} with linking number non-zero. Now, there is a T′′T^{\prime\prime} component of D1D_{1} which is linking with TT^{\prime} with linking number non-zero and which is disjoint from all the previously mentioned tori (T,T′′T3T^{\prime},T^{\prime\prime}\subset T_{3} is impossible because then both of T,T′′T^{\prime},T^{\prime\prime} are linking with TT and also with each other and this contradicts to (1) in Definition 2.13). Let T4T_{4} be a component of C1C_{1} such that T4T′′T_{4}\subset T^{\prime\prime} or T′′T4T^{\prime\prime}\subset T_{4}. There are a number of cases to check. If T3TT_{3}\subset T^{\prime} and T4T′′T_{4}\subset T^{\prime\prime}, then T3T_{3} is linking with T4T_{4}. If T3TT_{3}\subset T^{\prime} but T′′T4T^{\prime\prime}\subset T_{4}, then since T4T_{4} cannot contain TT or TT^{\prime}, we have again that T3T_{3} is linking with T4T_{4}. Finally, if TT3T^{\prime}\subset T_{3}, then since T′′T^{\prime\prime} cannot be in T3T_{3}, we have that T4T′′T_{4}\subset T^{\prime\prime} implies that T3T_{3} and T4T_{4} are linking and T′′T4T^{\prime\prime}\subset T_{4} implies that since T4T_{4} is disjoint from all the other tori, again T4T_{4} is linking with T3T_{3}. So we obtain that T1T_{1} and T2T_{2} are linking with T3T_{3} and T3T_{3} is linking with T4T_{4} resulting that T3T_{3} is linking with three other components of C1C_{1} which contradicts to (1) in Definition 2.13. Summarizing, we obtained the following.

  • The intersection C1D1\partial C_{1}\cap\partial D_{1} is empty,

  • no component of C1C_{1} is disjoint from all the components of D1D_{1} and vice versa,

  • every component of C1C_{1} contains one component of D1D_{1} or is contained in one component of D1D_{1},

  • no component of C1C_{1} contains more than one component of D1D_{1} and vice versa.

All of these imply that the number of components of C1C_{1} is equal to the number of components of D1D_{1}. We repeat the same line of arguments for the components of C2C_{2} and D2D_{2} lying in each component of C1C_{1} or D1D_{1} separately, where we perform the previous algorithm in the larger component which contains the smaller one, and so on, in this way we get the result. ∎

Remark 3.3.

If in (1) in Definition 2.13 we require having splitting number greater than 0 instead of having algebraic linking number non-zero, then the previous arguments could be repeated to get a similar result if we could prove that having two solid tori with splitting number greater than 0 and embedding one circle into each of these tori with non-zero winding numbers results that the splitting number of these two knots is greater than 0. For similar results about knots and their unknotting numbers, see [ST88, HLP22].

It follows that if two admissible decompositions of S3S^{3} are in the same equivalence class of the equivalence relation generated by being cylindrically related, then they determine the same sequence of numbers of components. So if we define the operation

(n0,n1,)+(m0,m1,)=(n0+m0,n1+m1,)(n_{0},n_{1},\ldots)+(m_{0},m_{1},\ldots)=(n_{0}+m_{0},n_{1}+m_{1},\ldots)

on the set of sequences, then the induced map

[(S3,𝒟,A,C0)]nC0,C1,C2,,[(S^{3},\mathcal{D},A,C_{0})]\mapsto n_{C_{0},C_{1},C_{2},\ldots},

where C0,C1,C2,C_{0},C_{1},C_{2},\ldots is some admissible defining sequence, is a monoid homomorphism.

Definition 3.4.

For an equivalence class xx represented by the admissible decomposition (S3,𝒟,A,C0)(S^{3},\mathcal{D},A,C_{0}) and for its admissible defining sequence C0,C1,C_{0},C_{1},\ldots let

L(x)=(l1,l2,)L(x)=(l_{1},l_{2},\ldots)

be the sequence of numbers mod 22 of the components of CmC_{m} which have non-zero algebraic linking number with some other component of CmC_{m}.

Lemma 3.5.

The map LL is well-defined i.e. admissible decompositions being concordant through finitely many cylindrically related admissible decompositions have the same value of LL.

Proof.

If decompositions with defining sequences C0,C1,C_{0},C_{1},\ldots and D0,D1,D_{0},D_{1},\ldots are cylindrically related, then for every m0m\geq 0 the pairs of components of CmC_{m} and the pairs of corresponding components of DmD_{m} have the same algebraic linking numbers. Suppose for a decomposition there are two admissible defining sequences C0,C1,C_{0},C_{1},\ldots and D0,D1,D_{0},D_{1},\ldots such that C0=D0C_{0}=D_{0}, we have to show that the linking numbers are equal to 0 simultanously for both of them (for the components of C0C_{0} and D0D_{0} this is obviously true). Of course we know that the components are in bijection with each other by the proof of Proposition 3.2 and in every component of C0C_{0} after some deformation we have that

  • the intersection C1D1\partial C_{1}\cap\partial D_{1} is empty,

  • no component of C1C_{1} is disjoint from all the components of D1D_{1} and vice versa,

  • every component of C1C_{1} contains one component of D1D_{1} or is contained in one component of D1D_{1},

  • no component of C1C_{1} contains more than one component of D1D_{1} and vice versa.

If a component TT of C1C_{1} is linked with a component TT^{\prime} of C1C_{1} with linking number 0, then any knot in TT^{\prime} is linked with TT with linking number 0. Also, if a knot in TT^{\prime} is linked with TT with linking number 0, then TT and TT^{\prime} are linked with linking number 0. For every m1m\geq 1 after a finite number of iterations of the algorithm in the proof of Proposition 3.2 we get the result. ∎

Of course the map LL is a monoid homomorphism moreover for a class xx represented by a slice decomposition we have L(x)=(0,0,)L(x)=(0,0,\ldots). Also, for a class xx of the form [(Sn,𝒟,A)]+[(Sn,𝒟,A)][(S^{n},\mathcal{D},A)]+[(-S^{n},\mathcal{D},A)] we have L(x)=(0,0,)L(x)=(0,0,\ldots) since all the linking components appear twice.

Definition 3.6.

We call the function

ν:Δ3a2\nu\colon\thinspace\Delta_{3}^{a}\to\mathbb{Z}_{2}^{\mathbb{N}}

obtained by ν([x])=L(x)\nu([x])=L(x) the mod 22 component number sequence of the elements of Δ3a\Delta_{3}^{a}.

Theorem 3.7.

There are at least uncountably many different elements in the concordance group Δ3a\Delta^{a}_{3}. These can be represented by Antoine decompositions.

Proof.

For every element (l0,l1,)2(l_{0},l_{1},\ldots)\in\mathbb{Z}_{2}^{\mathbb{N}}, where l0=0l_{0}=0, we have an Antoine decomposition representing a class xx such that ν([x])=(l0,l1,)\nu([x])=(l_{0},l_{1},\ldots). Hence we get uncountably many different classes in the concordance group. ∎

3.2. Computations in the cobordism group

Proposition 3.8.

Suppose that n0n\geq 0 and MM is a closed manifold. A closed nn-dimensional homology manifold NN having a resolution MNM\to N is cobordant in 𝔑nE\mathfrak{N}_{n}^{E} to MM.

Proof.

Take M×[0,1]M\times[0,1] and consider the cell-like decomposition 𝒟\mathcal{D} of MM which results the homology manifold NN. If 𝒮(X)\mathcal{S}(X) denotes the collection of singletons in a space XX, then 𝒟×𝒮([0,1/2])\mathcal{D}\times\mathcal{S}([0,1/2]) union 𝒮(M×(1/2,1])\mathcal{S}(M\times(1/2,1]) is a cell-like decomposition of M×[0,1]M\times[0,1], denote it by \mathcal{E}. We have to show that the quotient space

M×[0,1]/M\times[0,1]/\mathcal{E}

is an (n+1)(n+1)-dimensional homology manifold with boundary homology manifolds NN and MM. Take the closed manifold

M×[0,1]φM×[0,1],M\times[0,1]\cup_{\varphi}M\times[0,1],

where φ:(M×[0,1])(M×[0,1])\varphi\colon\thinspace\partial(M\times[0,1])\to\partial(M\times[0,1]) is the identity map. Since M/𝒟M/\mathcal{D} is nn-dimensional, the doubling of the decomposition \mathcal{E} on M×[0,1]φM×[0,1]M\times[0,1]\cup_{\varphi}M\times[0,1] yields a finite dimensional quotient space, we get this by using estimations for the covering dimension, see [HW41] and [Da86, Corollary 2.4A]. So the decomposition space PP obtained by factorizing M×[0,1]φM×[0,1]M\times[0,1]\cup_{\varphi}M\times[0,1] by the double of \mathcal{E} is a closed finite dimensional homology manifold by [DV09, Proposition 8.5.1]. Since this space has an open set homeomorphic to n+1\mathbb{R}^{n+1}, it is (n+1)(n+1)-dimensional. We obtain the space M×[0,1]/M\times[0,1]/\mathcal{E} by cutting PP into two pieces along two subsets homeomorphic to MM and NN. This means that MM and NN are cobordant in 𝔑nE\mathfrak{N}_{n}^{E}. ∎

So if every 33-dimensional homology manifold is resolvable, then 𝔑3E=0\mathfrak{N}_{3}^{E}=0. Also note that the decomposition space S3/𝒲S^{3}/\mathcal{W} of the Whitehead decomposition 𝒲\mathcal{W} is a null-cobordant 33-dimensional homology manifold, because [S3]=0[S^{3}]=0.

Proposition 3.9.

For n4n\geq 4 the cobordism group 𝔑n\mathfrak{N}_{n} is a subgroup of 𝔑nE\mathfrak{N}_{n}^{E}.

Proof.

Let M1M_{1} and M2M_{2} be closed manifolds. If the two cobordism classes [M1][M_{1}] and [M2][M_{2}] in 𝔑nE\mathfrak{N}_{n}^{E} coincide, then since MiM_{i} are manifolds, we have i(Mi)=1i(M_{i})=1 hence a cobordism in 𝔑nE\mathfrak{N}_{n}^{E} between M1M_{1} and M2M_{2} also has index 11 so this cobordism is resolvable. By [Qu83, Theorem 1.1] and Lemma 2.8 there is a manifold cobordism between M1M_{1} and M2M_{2}. ∎

In Definition 2.15 for i=1,2i=1,2 the space Mi/𝒟iM_{i}/\mathcal{D}_{i} is an nn-dimensional ENR homology manifold and W/W/\mathcal{E} is an (n+1)(n+1)-dimensional ENR homology manifold if we add the appropriate collars by Lemma 2.5. If (M,𝒟)(M,\mathcal{D}) is such a cell-like decomposition, then we can assign the cobordism class of the decomposition space M/𝒟M/\mathcal{D} to the cobordism class of (M,𝒟)(M,\mathcal{D}). This map

βn:n𝔑nE\beta_{n}\colon\thinspace\mathcal{B}_{n}\to\mathfrak{N}_{n}^{E}
[(M,𝒟)][M/𝒟][(M,\mathcal{D})]\mapsto[M/\mathcal{D}]

is a group homomorphism. The image of βn\beta_{n} contains the classes represented by topological manifolds since trivial decompositions always exist and it contains also the classes represented by homology manifolds having appropriate resolutions. For n=1,2n=1,2 all the homology manifolds are topological manifolds [Wi79] so the homomorphism βn\beta_{n} is surjective. Take the natural forgetting homomorphism

Fn:n𝔑nF_{n}\colon\thinspace\mathcal{B}_{n}\to\mathfrak{N}_{n}
[(M,𝒟)][M].[(M,\mathcal{D})]\to[M].

For every n0n\geq 0 the diagram

n\mathcal{B}_{n}𝔑nE\mathfrak{N}_{n}^{E}𝔑n\mathfrak{N}_{n}βn\beta_{n}FnF_{n}φn\varphi_{n}

is commutative by Proposition 3.8, where φn\varphi_{n} is the natural map assigning the cobordism class [M]𝔑nE[M]\in\mathfrak{N}_{n}^{E} to the cobordism class [M]𝔑n[M]\in\mathfrak{N}_{n}.

Proposition 3.10.

For every n0n\geq 0 the image of βn\beta_{n} is equal to the subgroup of 𝔑nE\mathfrak{N}_{n}^{E} generated by the cobordism classes of topological manifolds.

Proof.

The statement follows from the fact that FnF_{n} is surjective. ∎

Proposition 3.11.

For n1n\geq 1, we have βn(n)=𝔑n\beta_{n}(\mathcal{B}_{n})=\mathfrak{N}_{n} in 𝔑nE\mathfrak{N}_{n}^{E}.

Proof.

By Proposition 3.9 and Proposition 3.10 we have βn(n)=𝔑n\beta_{n}(\mathcal{B}_{n})=\mathfrak{N}_{n} for n4n\geq 4. For n=3n=3, since 𝔑3=0\mathfrak{N}_{3}=0, the statement also holds. For n=2n=2, The group 𝔑2\mathfrak{N}_{2} is isomorphic to 2\mathbb{Z}_{2} so by Proposition 3.10 it is enough to show that β2(2)=2\beta_{2}(\mathcal{B}_{2})=\mathbb{Z}_{2}. But [P2][{\mathbb{R}}{P}^{2}] is not null-cobordant in 𝔑2E\mathfrak{N}_{2}^{E} because P2{\mathbb{R}}{P}^{2} has a non-zero characteristic number as a smooth or topological manifold and then by [BH91] it cannot be null-cobordant. For n=1n=1, of course 𝔑1E=𝔑1=0\mathfrak{N}_{1}^{E}=\mathfrak{N}_{1}=0. ∎

Remark 3.12.

Instead of cell-like decompositions, which result homology manifolds, it would be possible to study decompositions which are just homologically acyclic and nearly 11-movable, see [DW83]. These result homology manifolds as well. Without being nearly 11-movable, these can result non-ANR homology manifolds.

As we could see, the class βn([(M,𝒟)])=[M/𝒟]𝔑n\beta_{n}([(M,\mathcal{D})])=[M/\mathcal{D}]\in\mathfrak{N}_{n} could not expose a lot of things about the decomposition 𝒟\mathcal{D}. If we add more details to the homology manifolds and their cobordisms, then we could obtain a finer invariant of the cobordism group of decompositions. Recall that the singular set of a homology manifold is the set of non-manifold points, which is a closed set.

Definition 3.13 (0- and 11-singular homology manifolds).

A homology manifold is 0-singular if its singular set is a 0-dimensional set. A compact homology manifold with collared boundary is 11-singular if its singular set SS consists of properly embedded arcs such that SS is a direct product in the collar. The closed nn-dimensional 0-singular homology manifolds X1X_{1} and X2X_{2} are cobordant if there exists a compact (n+1)(n+1)-dimensional 11-singular homology manifold WW such that W\partial W is homeomorphic to the disjoint union of X1X_{1} and X2X_{2} and WS\partial W\cap S coincides with the singular set of X1X2X_{1}\sqcup X_{2} under this homeomorphism. The set of (oriented) cobordism classes is denoted by 𝔑nS\mathfrak{N}_{n}^{S} (and ΩnS\Omega_{n}^{S}).

The set of cobordism classes 𝔑nS\mathfrak{N}_{n}^{S} and ΩnS\Omega_{n}^{S} are groups with the disjoint union as group operation. Denote by 𝔐n0\mathfrak{M}_{n}^{0} the cobordism group of 0-singular manifolds where the cobordisms are arbitrary but the singular set of the cobordisms is not the entire manifold.

Note that the representatives of the classes in βn(n)\beta_{n}(\mathcal{B}_{n}) are 0-singular and the cobordisms between them have not only singular points because the boundary has not only singular points since the singular set is a compact 0-dimensional set. There are natural homomorphisms

in:n𝔑nSin:n𝔐n0 and nni_{n}^{\prime}\colon\thinspace\mathcal{B}_{n}^{\prime}\to\mathfrak{N}_{n}^{S}\mbox{, \ \ \ \ \ }i_{n}\colon\thinspace\mathcal{B}_{n}\to\mathfrak{M}_{n}^{0}\mbox{\ \ \ \ \ and\ \ \ \ \ }\mathcal{B}^{\prime}_{n}\to\mathcal{B}_{n}

where n\mathcal{B}_{n}^{\prime} is the version of n\mathcal{B}_{n} yielding 0-singular spaces and 11-singular cobordisms, there is the forgetful map

φn:𝔑nS𝔐n0\varphi_{n}\colon\thinspace\mathfrak{N}_{n}^{S}\to\mathfrak{M}_{n}^{0}

and then the diagram

nin𝔑nSφnnin𝔐n0ψn𝔑nE\begin{CD}\mathcal{B}^{\prime}_{n}@>{i_{n}^{\prime}}>{}>\mathfrak{N}_{n}^{S}\\ @V{}V{}V@V{}V{\varphi_{n}}V\\ \mathcal{B}_{n}@>{i_{n}}>{}>\mathfrak{M}_{n}^{0}@>{\psi_{n}}>{}>\mathfrak{N}_{n}^{E}\end{CD}

commutes. Observe that ψn\psi_{n} is injective, φn\varphi_{n} is surjective and since βn(n)=ψnin(n)=𝔑n\beta_{n}(\mathcal{B}_{n})=\psi_{n}\circ i_{n}(\mathcal{B}_{n})=\mathfrak{N}_{n}, the image in(n)i_{n}^{\prime}(\mathcal{B}_{n}^{\prime}) is in φn1ψn1(𝔑n)\varphi^{-1}_{n}\circ\psi^{-1}_{n}(\mathfrak{N}_{n}), which could be a larger group than 𝔑n\mathfrak{N}_{n}.

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