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Free Groups as End Homogeneity Groups of 33-manifolds

Dennis J. Garity Mathematics Department, Oregon State University, Corvallis, OR 97331, U.S.A. [email protected] http://www.math.oregonstate.edu/~garity  and  Dušan D. Repovš Faculty of Education, and Faculty of Mathematics and Physics, University of Ljubljana
& Institute of Mathematics, Physics and Mechanics, Ljubljana SI-1000, Slovenia
[email protected] http://www.fmf.uni-lj.si/~repovs
Abstract.

For every finitely generated free group FF, we construct an irreducible open 33-manifold MFM_{F} whose end set is homeomorphic to a Cantor set, and with the end homogeneity group of MFM_{F} isomorphic to FF. The end homogeneity group is the group of all self-homeomorphisms of the end set that extend to homeomorphisms of the entire 33-manifold. This extends an earlier result that constructs, for each finitely generated abelian group GG, an irreducible open 33-manifold MGM_{G} with end homogeneity group GG. The method used in the proof of our main result also shows that if GG is a group with a Cayley graph in 3\mathbb{R}^{3} such that the graph automorphisms have certain nice extension properties, then there is an irreducible open 33-manifold MGM_{G} with end homogeneity group GG.

Key words and phrases:
Open 3-manifold, rigidity, manifold end, geometric index, Cantor set, homogeneity group, abelian group, defining sequence
2010 Mathematics Subject Classification:
Primary 54E45, 57M30, 57N12; Secondary 57N10, 54F65

Introduction

Each compact set KK in S3S^{3} (or in 3\mathbb{R}^{3}) has for its complement an open 33-manifold M3M^{3}. There is often a close relation between properties of the embedding of KK in S3S^{3} and properties of this 33-manifold complement. Consider, for example, embeddings of knots and the study of knot complements. See also [21] for a construction of a Cantor set with hyperbolic complement.

If the compact set KK is a Cantor set CC in S3S^{3}, then the complement of CC is an open 33-manifold M3M^{3} with end set CC. The embedding of the Cantor set gives rise to properties of the corresponding complementary 33-manifold M3M^{3} and of the end set CC of M3M^{3}. See [9, 11, 21] for examples of this. There has been extensive study of embeddings of Cantor sets in S3S^{3} or 3\mathbb{R}^{3}. The space of embeddings is extremely complicated. See for example [15].

In [10], the authors showed that for every finitely generated abelian group GG, there is an irreducible open 3-manifold MGM_{G} with end homogeneity group isomorphic to GG. The end homogeneity group is the group of all end homeomorphisms that extend to the entire 3-manifold. This 33-manifold is the complement of a carefully constructed Cantor set CGC_{G} associated with GG in S3S^{3}.

For further examples of properties of embeddings related to properties of the containing 3-manifold or of the 3-manifold arising as the complement, see [16] for a relation of certain group presentations to certain wild embeddings of arcs and [6] for a construction of certain wild Cantor sets that are Julia sets. See also [14] for another example of the use of embeddings to construct certain 3-manifolds.

In this paper, the authors show that for any finitely generated free group FF, there is an irreducible open 3-manifold MFM_{F} with the end homogeneity group FF. The proof leads to a technique which shows that if a group GG has a Cayley graph embeddable in S3S^{3} in a particularly nice way, then there is an irreducible open 3-manifold MGM_{G} with the end homogeneity group isomorphic to GG.

In Section 1 we discuss concepts and results needed in the paper. This includes the concepts of geometric index, local genus, embedding homogeneity groups, end homogeneity groups, Antoine Cantor sets, and rigidly embedded Cantor sets. In Section 2, we carefully construct a specific Cayley graph in 3\mathbb{R}^{3} for the free group on NN generators, FNF_{N}. In Section 3 we construct a specific Cantor set in S3S^{3} related to the Cayley graph constructed in Section 2. In Section 4 we prove the main theorems. We end with some open questions.

1. Preliminaries

Background Information

We refer to [12, 13, 8, 11] for a discussion of Cantor sets in general and of rigid Cantor sets, and to [24] for results about local genus of points in Cantor sets and defining sequences for Cantor sets. The bibliographies in these papers contain additional references to results about Cantor sets. Two Cantor sets XX and YY in 3\mathbb{R}^{3} (or S3S^{3}) are said to be equivalent or equivalently embedded if there is a self-homeomorphism of 3\mathbb{R}^{3} (or S3S^{3}) taking XX to YY. If there is no such homeomorphism, the Cantor sets are said to be inequivalent, or inequivalently embedded. A Cantor set CC is said to be rigidly embedded in 3\mathbb{R}^{3} (or S3S^{3}) if the only self-homeomorphism of CC that extends to a homeomorphism of 3\mathbb{R}^{3} (or S3S^{3}) is the identity.

Geometric Index

We list the results which we will need on geometric index. See Schubert [17, 8] for more details. If KK is a link in the interior of a solid torus TT, the geometric index of KK in TT, denoted by N(K,T)\text{N}(K,T), is the minimum of |KD||K\cap D| over all meridional disks DD of TT intersecting KK transversely. If TT is a solid torus and MM is a finite union of disjoint solid tori so that MIntTM\subset\text{Int}\ T, then the geometric index N(M,T)\text{N}(M,T) of MM in TT is N(K,T)\text{N}(K,T) where KK is a core of MM.

Note: An unknotted solid torus is a solid torus B2×S1B^{2}\times S^{1} with center line {0}×S1\{0\}\times S^{1} an unknotted circle in S3S^{3} .

Theorem 1.1.

([17], [8, Theorem 3.1]) Let T0T_{0} and T1T_{1} be unknotted solid tori in S3S^{3} with T0Int(T1)T_{0}\subset\rm{Int}(T_{1}) and N(T0,T1)=1\rm{N}(T_{0},T_{1})=1. Then T0\partial T_{0} and T1\partial T_{1} are parallel; i.e., the 3-manifold T1Int(T0)T_{1}-\rm{Int}(T_{0}) is homeomorphic to T0×I\partial T_{0}\times I where II is the closed unit interval [0,1][0,1].

Theorem 1.2.

([17], [8, Theorem 3.2]) Let T0T_{0} be a finite union of disjoint solid tori. Let T1T_{1} and T2T_{2} be solid tori so that T0Int(T1)T_{0}\subset\rm{Int}(T_{1}) and T1Int(T2)T_{1}\subset\rm{Int}(T_{2}). Then N(T0,T2)=N(T0,T1)N(T1,T2)\rm{N}(T_{0},T_{2})=\rm{N}(T_{0},T_{1})\cdot\rm{N}(T_{1},T_{2}).

There is one additional result we will need.

Theorem 1.3.

([17], [8, Theorem 3.3]) Let TT be a solid torus in S3S^{3} and let T1,TnT_{1},\ldots T_{n} be unknotted pairwise disjoint solid tori in TT, each of geometric index 0 in TT. Then the geometric index of i=1nTi\bigcup\limits_{i=1}^{n}T_{i} in TT is even.

Defining Sequences and Local Genus

We review the definition and some basic facts from [24] about the local genus of points in a Cantor set. Also see [24] for a discussion of defining sequences.

A defining sequence for a Cantor set XX in 3\mathbb{R}^{3} is a properly nested sequence of handlebodies (Mi)(M_{i}) such that Mi=X\bigcap M_{i}=X. Let 𝒟(X){\mathcal{D}}(X) be the set of all defining sequences for a Cantor set XS3X\subset S^{3}. Let (Mi)𝒟(X)(M_{i})\in{\mathcal{D}}(X) be one of these defining sequences. For AXA\subset X, denote by MiAM_{i}^{A} the union of those components of MiM_{i} which intersect AA. Define

gA(X;(Mi))=sup{g(MiA);i0} and g_{A}(X;(M_{i}))=\sup\{g(M_{i}^{A});\ i\geq 0\}\ \ \mbox{ and }
gA(X)=inf{gA(X;(Mi));(Mi)𝒟(X)}\ g_{A}(X)=\inf\{g_{A}(X;(M_{i}));\ (M_{i})\in{\mathcal{D}}(X)\}

where g(MiA)g(M_{i}^{A}) is the genus of MiAM_{i}^{A}. The number gA(X)g_{A}(X) is called the genus of the Cantor set XX with respect to the subset AA. For A={x}A=\{x\} we call the number g{x}(X)g_{\{x\}}(X) the local genus of the Cantor set XX at the point xx and denote it by gx(X)g_{x}(X).

Remark 1.4.

The genus measures the minimum genus of handlebodies MiM_{i} needed in any defining sequence for the Cantor set. The standard Cantor set has genus 0 at each point since it can be defined as an intersection of genus 0 balls. An Antoine Cantor set (illustrated in Figure 1) has genus 1 at each point since it is defined by genus 1 manifolds (solid tori), but cannot be defined by genus 0 manifolds (balls).

Remark 1.5.

Let xx be an arbitrary point of a Cantor set XX and h:S3S3h\colon S^{3}\to S^{3} a homeomorphism. Then the local genus gx(X)g_{x}(X) is the same as the local genus gh(x)(h(X))g_{h(x)}(h(X)). Also note that if xCCx\in C\subset C^{\prime}, then the local genus of xx in CC is less than or equal to the local genus of xx in CC^{\prime}. See [24, Theorem 2.4].

The following result from [24] is needed to show that certain points in our examples have local genus >1>1.

Theorem 1.6.

[24] Let X,YS3X,Y\subset S^{3} be Cantor sets and pXYp\in X\cap Y. Suppose there exists a 3-ball BB and a 2-disc DBD\subset B such that

  1. (1)

    pIntBp\in\rm{Int}B, D=DB\partial D=D\cap\partial B, D(XY)={p}D\cap(X\cup Y)=\{p\}; and

  2. (2)

    XBBX{p}X\cap B\subset B_{X}\cup\{p\} and YBBY{p}Y\cap B\subset B_{Y}\cup\{p\} where BXB_{X} and BYB_{Y} are the components of BDB-D.

Then gp(XY)=gp(X)+gp(Y)g_{p}(X\cup Y)=g_{p}(X)+g_{p}(Y).

Embedding Homogeneity Groups and End Homogeneity Groups

For background on Freudenthal compactifications and theory of ends, see [4, 7, 20]. For an alternate proof using defining sequences of the result that every homeomorphism of the open 33-manifold extends to a homeomorphism of its Freudenthal compactification, see [9].

Each Cantor set CC in S3S^{3} has for its complement an open 33-manifold M3M^{3} with end set CC. The embedding of the Cantor set gives rise to properties of the corresponding complementary 33-manifold M3M^{3}. See [9, 11, 21] for examples of this.

We investigate possible group actions on the end set CC of the open 33-manifold M3M^{3} in the following sense: The homogeneity group of the end set is the group of homeomorphisms of the end set CC that extend to homeomorphisms of the open 33-manifold M3M^{3}. Referring specifically to the embedding of the Cantor set, this group can also be called the embedding homogeneity group of the Cantor set. See [5, 22] for a discussion and overview of some other types of homogeneity.

The standardly embedded Cantor set is at one extreme here. The embedding homogeneity group is the full group of self-homeomorphisms of the Cantor set, an extremely rich group (there is such a homeomorphism taking any countable dense subset to any other). Cantor sets with this full embedding homogeneity group are called strongly homogeneously embedded. See Daverman [3] for an example of a non-standard Cantor set with this property.

At the other extreme are rigidly embedded Cantor sets, i.e. those Cantor sets for which only the identity homeomorphism extends. Shilepsky [19] constructed Antoine type [2] rigid Cantor sets. Their rigidity is a consequence of Sher’s result [18] that if two Antoine Cantor sets are equivalently embedded, then the stages of their defining sequences must match up exactly. Newer examples [13, 8] of non-standard Cantor sets were constructed that are both rigidly embedded and have simply connected complement. See [23] for additional examples of rigidity.

These examples naturally lead to the question of which types of groups can arise as end homogeneity groups between the two extremes mentioned above. In this paper we show that for each finitely generated free group GG, there is an irreducible open 3-manifold with the end set homeomorphic to a Cantor set and with the end homogeneity group isomorphic to GG.

Remark 1.7.

The Cantor sets produced are unsplittable as are the set of ends, in the sense that no 22-sphere separates points of the Cantor set (respectively, points of the end set). Correspondingly, the complements of the Cantor sets produced are irreducible in the sense that every 2-sphere in the complement bounds a 3-ball.

Antoine Cantor Sets

An Antoine Cantor set is described as follows. Let M0M_{0} be an unknotted solid torus in S3S^{3}. Let M1M_{1} be a chain of at least four linked, pairwise disjoint, unknotted solid tori in M0M_{0} as in Figure 1. Inductively, MiM_{i} consists of pairwise disjoint solid tori in S3S^{3} and Mi+1M_{i+1} is obtained from MiM_{i} by placing a chain of at least four linked, pairwise disjoint, unknotted solid tori in each component of MiM_{i}. If the diameter of the components goes to 0, the Antoine Cantor set is C=i=0MiC=\bigcap\limits_{i=0}^{\infty}M_{i}.

Refer to caption
Figure 1. Two Stages for an Antoine Construction

We refer to Sher’s paper [18] for basic results and description of Antoine Cantor sets. The key result we will need is the following:

Theorem 1.8.

[18, Theorems 1 and 2] Suppose CC and DD are Antoine Cantor sets in S3S^{3} with defining sequences {Mi}\{M_{i}\} and {Ni}\{N_{i}\}, respectively. Then CC and DD are equivalently embedded if and only if there is a self-homeomorphism hh of S3S^{3} with h(Mi)=Nih(M_{i})=N_{i} for each ii.

In particular, the number and adjacency of links in the chains must match up at each stage.

Remark 1.9.

A standard argument shows that Antoine Cantor set cannot be separated by any 22-sphere.

Remark 1.10.

Also note that the homeomorphism in Theorem 1.8 can be realized as the final stage of an ambient isotopy in S3S^{3} since each of the homeomorphisms in the argument can be realized by an ambient isotopy.

2. A Cayley Graph for FNF_{N}

Let FNF_{N} be the free group on generators, a1,,aNa_{1},\ldots,a_{N}. Denote the inverse of aia_{i} by ai¯\overline{\mathstrut a_{i}} and let g(FN)g(F_{N}), the full generating set of FNF_{N}, be {a1,,aN,a1¯,,aN¯}\{a_{1},\ldots,a_{N},\overline{\mathstrut a_{1}},\ldots,\overline{\mathstrut a_{N}}\}. For economy of notation, let βj=αj\beta_{j}=\alpha_{j} for 1jN1\leq j\leq N and let βj=αjN¯\beta_{j}=\overline{\mathstrut\alpha_{j-N}} for N+1j2NN+1\leq j\leq 2N. Note that βk¯=βk+n (mod 2N)\overline{\mathstrut\beta_{k}}=\beta_{k+n\text{ (mod 2N)}}. Elements of FNF_{N} correspond to reduced words using elements of g(FN)g(F_{N}) as letters. Group multiplication corresponds to concatenation and reduction of words. We first describe a specific embedding for the Cayley graph G(FN)G(F_{N}) associated with this presentation of FNF_{N}.

The identity is represented by the empty word and corresponds to a vertex v(e)v(e) at the origin. There are σ(n)=2N(N1)n1\sigma(n)=2N\cdot(N-1)^{n-1} reduced words of length nn. These will be represented by σ(n)\sigma(n) equally spaced vertices on the circle of radius nn centered at the origin, at radial angles:

{n(k)2πσ(n)k2π2σ(n)| 1kσ(n)}\{n(k)\equiv\dfrac{2\pi}{\sigma(n)}k-\dfrac{2\pi}{2\sigma(n)}\ |\ 1\leq k\leq\sigma(n)\}.

Each of these points, p(n,k)nenkip(n,k)\equiv n\cdot e^{n_{k}\cdot i} for 1kσ(n)1\leq k\leq\sigma(n), on the circle of radius nn will be joined by edges to N1N-1 vertices on the circle of radius n+1n+1. Specifically, p(n,k)p(n,k) will be joined to the points:

{p(n+1,j)|(k1)(N1)<j(k)(N1)}.\{p(n+1,j)\ |\ (k-1)(N-1)<j\leq(k)(N-1)\}.

Figure 2 show the first two stages of the Cayley graph for F2F_{2} and F3F_{3}. The colored directed edges correspond to generators and will be described in more detail in the next subsection.

Refer to caption
(a) F2F_{2} Stage 2
Refer to caption
(b) F2F_{2} Stage 3
Refer to caption
(c) F3F_{3} Stage 2
Refer to caption
(d) F3F_{3} Stage 3
Figure 2. Cayley Graphs for F2F_{2} and F3F_{3}

Labeling Edges and Vertices

We inductively describe how to label the vertices and how to label and orient the edges of the graph described above.

Remark 2.1.

Note that an edge oriented from vv to ww labeled with the generator aia_{i} is regarded the same as that edge oriented from ww to vv and labeled with the generator ai¯\overline{\mathstrut a_{i}}.

Begin by labeling the vertex at the origin corresponding to the identity as v(e)v(e). Label the vertex at p(1,j)p(1,j) for 1j2N1\leq j\leq 2N as v(βj)v(\beta_{j}).

Label the edge from v(e)v(e) to v(βj)v(\beta_{j}), 1j2N1\leq j\leq 2N with the generator βj\beta_{j} and orient it from v(e)v(e) to v(βj)v(\beta_{j}). Note that this is equivalent to labeling the edge from v(βj)v(\beta_{j}) to v(e)v(e) with the generator βj¯\overline{\mathstrut\beta_{j}} and orienting it from v(βj)v(\beta_{j}) to v(e)v(e). For notation, we refer to this edge as E(v(e),βj)E(v(e),\beta_{j}) or E(v(βj),βj¯)E(v(\beta_{j}),\overline{\mathstrut\beta_{j}}) to emphasize the initial vertex and generator needed to get to the other vertex. To emphasize the initial and final vertices, we can use the notation E(v(e),v(βj))=E(v(βj),v(e))E(v(e),v(\beta_{j}))=E(v(\beta_{j}),v(e)).

Note that starting at any point on the circle of radius 1/21/2 centered at the origin and traveling in the counterclockwise direction around this circle, one encounters the labeled edges in the cyclic order E(v(e),β1),,E(v(e),β2N)E(v(e),\beta_{1}),\ldots,E(v(e),\beta_{2N}), or equivalently, by Remark 2.1, in the cyclic order:

E(v(e),β1),,E(v(e),βN),E(v(βN+1),β1),,E(v(β2N),βN)E(v(e),\beta_{1}),\ldots,E(v(e),\beta_{N}),E(v(\beta_{N+1}),\beta_{1}),\ldots,E(v(\beta_{2N}),\beta_{N}).

Inductively assume the vertices at distance mm from the origin, mnm\leq n, have been labeled as v(gi)v(g_{i}), where gig_{i} is a reduced word of length mm. Also assume that edges from vertices v(gi)v(g_{i}) at distance mm from the origin (mn1)(m\leq n-1) to v(g)v(g_{\ell}) at distance m+1m+1 from the origin have been labeled E(v(gi),βk)E(v(g_{i}),\beta_{k}) where g=giβkg_{\ell}=g_{i}\circ\beta_{k}.

Consider v(g)v(g) for some gg of reduced length n. Then g=gβkg=g^{\,\prime}\circ\beta_{k} for some reduced word gg^{\,\prime} of length n1n-1 and some βkg(FN)\beta_{k}\in g(F_{N}). The edge joining v(g)v(g^{\,\prime}) to v(g)v(g) is labeled E(v(g),βk)E(v(g^{\,\prime}),\beta_{k}), or equivalently E(v(g),βk¯)=E(v(g),βk+N(mod 2N))E(v(g),\overline{\mathstrut\beta_{k}})=E(v(g),\beta_{k+N\text{(mod 2N)}}). Let j=k+n(mod 2N)j=k+n\text{(mod 2N)}.

Form a circle of radius 1/21/2 about v(g)v(g). Starting at the edge E(v(g),βj)E(v(g),\beta_{j}), proceed around the circle in the counterclockwise direction labeling the edges encountered as

E(v(g),βj+1),E(v(g),βj+2N1),E(v(g),\beta_{j+1}),\ldots E(v(g),\beta_{j+2N-1}),

all subscripts mod(2N).

Refer to caption
Refer to caption
Figure 3. Inductively Labelling Edges

Label the vertices at distance n+1n+1 from the origin as follows. If vv is such a vertex, then there is an edge E(v(g),βj)E(v(g),\beta_{j}) from a vertex v(g)v(g) at distance nn from the origin to vv. Label the vertex vv as v(gβj)v(g\circ\beta_{j}).

The inductive assumption is easily checked for the newly labeled vertices and edges. See Figure 3 for an illustration, keeping in mind Remark 2.1.

Cayley Graph Automorphisms for 𝑮(𝑭𝑵){\boldsymbol{G(F_{N})}}

For each element gg of FNF_{N} we define a graph automorphism hgh_{g} of G(FN)G(F_{N}) as follows. For a vertex v(gi)v({g_{i}}) of G(FN)G(F_{N}) corresponding to the element gig_{i} of FNF_{N}, hg(v(gi))h_{g}(v({g_{i}})) is defined to be v(ggi)v(g\circ g_{i}). The edge from v(gi)v(g_{i}) to v(giβk)v(g_{i}\circ\beta_{k}) can be labeled E(v(gi),βk)E(v(g_{i}),\beta_{k}) when oriented from v(gi)v(g_{i}) to v(giβk)v(g_{i}\circ\beta_{k}). Define hg(E(v(gi),βk)h_{g}(E(v(g_{i}),\beta_{k}) to be the linear homeomorphism from E(v(gi),βk)E(v(g_{i}),\beta_{k}) to E(v(ggi),βk)E(v(g\circ g_{i}),\beta_{k}).

Remark 2.2.

Note that these graph automorphisms define homeomorphisms from G(FN)G(F_{N}) to itself. Note also that hg1hg2=hg1g2h_{g_{1}}\circ h_{g_{2}}=h_{g_{1}\circ g_{2}}.

Extending Graph Automorphisms to Homeomorphisms of 3\mathbb{R}^{3}

The graph automorphisms hβih_{\beta_{i}}, for 1iN1\leq i\leq N, can be extended to homeomorphisms hβi{h^{\prime}}_{\beta_{i}} from 2\mathbb{R}^{2} to itself. Note that 2G(FN)\mathbb{R}^{2}-G(F_{N}) consists of a collections of unbounded regions with boundary in G(FN)G(F_{N}). Adding in the point at infinity, each region is a closed disc with boundary consisting of edges in G(FN)G(F_{N}) together with this added point. The graph automorphism hβih_{\beta_{i}} takes the boundary of one of these disc regions to the boundary of another, and can thus be extended to the entire region. There are many choices for these extension homeomorphisms. They coincide up to proper isotopy.

Piecing together these extensions, one gets an extension of hβih_{\beta_{i}} to a self homeomorphism of 2\mathbb{R}^{2}, hβi{h^{\prime}}_{\beta_{i}} for 1iN1\leq i\leq N. Define hβi{h^{\prime}}_{\beta_{i}} for N+1i2NN+1\leq i\leq 2N to be (hβiN)1(h^{\prime}_{\beta_{i-N}})^{-1}. Since hβi=(hβiN)1h_{\beta_{i}}=(h_{\beta_{i-N}})^{-1} for N+1i2NN+1\leq i\leq 2N as graph automorphisms, it follows that hβih^{\prime}_{\beta_{i}} is an extension of hβih_{\beta_{i}} for N+1i2NN+1\leq i\leq 2N.

For a general gFNg\in F_{N}, gg has a unique reduced representation g=βi1βi2βiMg=\beta_{i1}\circ\beta_{i2}\circ\ldots\circ\beta_{iM} where the βij\beta_{ij} are in g(FN)g(F_{N}). Define h(g)h^{\prime}(g) to be:

hg=hβi1hβi2hβiMh^{\prime}_{g}=h^{\prime}_{\beta_{i1}}\circ h^{\prime}_{\beta_{i2}}\circ\ldots\circ h^{\prime}_{\beta_{iM}}

The homeomorphism hg:22h^{\prime}_{g}:\mathbb{R}^{2}\rightarrow\mathbb{R}^{2} can then be extended to a homeomorphism Hg:33H_{g}:\mathbb{R}^{3}\rightarrow\mathbb{R}^{3} by crossing with the identity.

Remark 2.3.

Note that hg1hg2=hg1g2h^{\prime}_{g_{1}}\circ h^{\prime}_{g_{2}}=h^{\prime}_{g_{1}\circ g_{2}}. This follows from the uniqueness of reduced representations of elements of FNF_{N}. The definition of HgH_{g} as the product of hgh^{\prime}_{g} with the identity shows that it is also true that Hg1Hg2=Hg1g2H_{g_{1}}\circ H_{g_{2}}=H_{g_{1}\circ g_{2}}.

3. A Cantor Set C(FN)C(F_{N}) with Embedding Homogeneity Group FNF_{N}

A Collection of Balls and Tubes in 3\mathbb{R}^{3} Containing G(FN)G(F_{N})

In 3\mathbb{R}^{3}, choose a 3-ball B(v(e))B(v(e)) around the origin =v(e)=v(e) so that the homeomorphic copies Hβi(B(v(e)))H_{\beta_{i}}(B(v(e))), 1i2N,1\leq i\leq 2N, together with B(v(e))B(v(e)) are all pairwise disjoint. Let B(v(βi))B(v(\beta_{i})) denote the 3-ball Hβi(B(v(e)))H_{\beta_{i}}(B(v(e))). The original ball B(v(e))B(v(e)) can be chosen so that it is contained in a ball of radius 1/51/5 about v(e)v(e), and so that each B(v(βi))B(v(\beta_{i})) is contained in a ball of radius 1/51/5 about v(βi)v(\beta_{i}).

For a general gFNg\in F_{N}, use the unique reduced representation of gg as βi1βi2βiM\beta_{i1}\circ\beta_{i2}\circ\ldots\circ\beta_{iM} where the βij\beta_{ij} are in g(FN)g(F_{N}). The ball B(v(g))B(v(g)) is then defined to be to be:

Hβi1Hβi2HβiM(B(v(e)))=Hg(B(v(e))).H_{\beta_{i1}}\circ H_{\beta_{i2}}\circ\ldots\circ H_{\beta_{iM}}(B(v(e)))=H_{g}(B(v(e))).

We similarly define a collection of tubes. For each ii, 1iN1\leq i\leq N choose a thin tube D(v(e),βi)D(v(e),\beta_{i}) joining B(v(e))B(v(e)) to B(v(βi))B(v(\beta_{i})) so that B(v(e))D(v(e),βi)B(v(βi))B(v(e))\cup D(v(e),\beta_{i})\cup B(v(\beta_{i})) contains E(v(e),βi)E(v(e),\beta_{i}). Choose the tubes D(v(e),β1),,D(v(e),βN)D(v(e),\beta_{1}),\ldots,D(v(e),\beta_{N}), so as to be pairwise disjoint. For each ii, N+1i2NN+1\leq i\leq 2N let D(v(e),βi)D(v(e),\beta_{i}) be Hβi(D(v(e),βiN))=Hβi(D(v(e),βi¯))H_{\beta_{i}}(D(v(e),\beta_{i-N}))=H_{\beta_{i}}(D(v(e),\overline{\beta_{i}})). See Figure 4 for an illustration for F2F_{2}.

Remark 3.1.

Note that the relationship D(v(e),βi)=Hβi(D(v(e),βi¯))D(v(e),\beta_{i})=H_{\beta_{i}}(D(v(e),\overline{\beta_{i}})) then holds for all ii, 1i2N1\leq i\leq 2N.

Refer to caption
Figure 4. Balls, Tubes around G(F2)G(F_{2})

Rigid Cantor Sets Using G(FN)G(F_{N}) as a Guide.

Refer to caption
Figure 5. Construction of Rigid Cantor Sets Placement for G(F2G(F_{2})

We will now define rigid Antoine Cantor sets associated with each vertex in G(FN)G(F_{N}), and a chain of three linked rigid Cantor sets for each edge in G(Fn)G(F_{n}). See Figure 5 for an illustration of the outer tori in defining sequences for these rigid Cantor sets in the case of F2F_{2}.

To begin, construct a rigid Antoine Cantor set C(v(e))C(v(e)) so the outer torus, T(C(v(e)))T(C(v(e))), of the construction is in B(v(e))B(v(e)). This T(C(v(e)))T(C(v(e))) corresponds to the central torus in Figure 5 in the case of F2F_{2}. Let T(C(v(e)))T^{\prime}(C(v(e))) be the union of the second stage tori in the construction of C(v(e))C(v(e)). See Figure 1 for an illustration of the first and second stages of an Antoine construction.

For a general gFNg\in F_{N}, use the unique reduced representation of gg as βi1βi2βiM\beta_{i1}\circ\beta_{i2}\circ\ldots\circ\beta_{iM} where the βij\beta_{ij} are in g(FN)g(F_{N}). Define a rigid Cantor set C(v(g))B(v(g))C(v(g))\subset B(v(g)) to be:

Hβi1Hβi2HβiM(C(v(e)))=Hg(C(v(e))).H_{\beta_{i1}}\circ H_{\beta_{i2}}\circ\ldots\circ H_{\beta_{iM}}(C(v(e)))=H_{g}(C(v(e))).
Remark 3.2.

Note that C(v(e))C(v(e)) and any C(v(g))C(v(g)) are equivalently embedded.

Similarly, let T(C(v(g)))=Hg(T(C(v(e)))) and T(C(v(g)))=Hg(T(C(v(e)))).T(C(v(g)))=H_{g}(T(C(v(e))))\text{ and }T^{\,\prime}(C(v(g)))=H_{g}(T^{\prime}(C(v(e)))). The four outer tori in Figure 5 correspond to T(C(a1)),T(C(a2)),T(C(a1¯))T(C(a_{1})),T(C(a_{2})),T(C(\overline{\mathstrut a_{1}})), and TC(a2¯)TC(\overline{\mathstrut a_{2}}) in the case of F2F_{2}.

We next construct rigid Cantor sets C1(v(e),βk),C2(v(e),βk),C3(v(e),βk)C_{1}(v(e),\beta_{k}),C_{2}(v(e),\beta_{k}),C_{3}(v(e),\beta_{k}) for each k,1kNk,1\leq k\leq N. Choose a series of three linked tori, T1(v(e),βk),T2(v(e),βk),T_{1}(v(e),\beta_{k}),T_{2}(v(e),\beta_{k}), and T3(v(e),βk)T_{3}(v(e),\beta_{k}) joining T(C(v(e))) and T(C(βk)),1kNT(C(v(e)))\text{ and }T(C(\beta_{k})),1\leq k\leq N and contained in B(v(e))D(v(e),βk)B(v(βk))B(v(e))\cup D(v(e),\beta_{k})\cup B(v(\beta_{k})) as in Figure 5. Label the torus linked to T(C(v(e)))T(C(v(e))) as T1(v(e),βk)T_{1}(v(e),\beta_{k}), and use it as the outer torus for a rigid Antoine Cantor set C1(v(e),βk)C_{1}(v(e),\beta_{k}). Label the torus linked to T(C(βk))T(C(\beta_{k})) as T3(v(e),βk)T_{3}(v(e),\beta_{k}), and use it as the outer torus for a rigid Antoine Cantor set C3(v(e),βk)C_{3}(v(e),\beta_{k}). Label the remaining torus as T2(v(e),βk)T_{2}(v(e),\beta_{k}) and use it as the outer torus for a rigid Antoine Cantor set C2(v(e),βk)C_{2}(v(e),\beta_{k}).

Remark 3.3.

Choose these 3N3N rigid Cantor sets {Ti(v(e),βk),113,1kN}\{T_{i}(v(e),\beta_{k}),1\leq 1\leq 3,1\leq k\leq N\} so that they are all inequivalently embedded, and so that they are all inequivalent to C(v(e))C(v(e)).

For N+1k2NN+1\leq k\leq 2N, and 1j31\leq j\leq 3, let Cj(v(e),βk)=Hβk(Cj(v(e),βk¯))C_{j}(v(e),\beta_{k})=H_{\beta_{k}}(C_{j}(v(e),\overline{\beta_{k}})), and T(Cj(v(e),βk))=Hβk(T(Cj(v(e),βk¯)))T(C_{j}(v(e),\beta_{k}))=H_{\beta_{k}}(T(C_{j}(v(e),\overline{\beta_{k}}))). This completes the definition of the 32N3\cdot 2N rigid Cantor sets along the edges E(v(e),βk)E(v(e),\beta_{k}). See Figure 5 for outer tori corresponding to these Cantor sets in the case F(2)F(2).

For gFNg\in F_{N}, let Ci(v(g),βk)=Hg(Ci(v(e),βk))C_{i}(v(g),\beta_{k})=H_{g}(C_{i}(v(e),\beta_{k})) and T(Ci(v(g),βk))=Hg(T(Ci(v(e),βk)))T(C_{i}(v(g),\beta_{k}))=H_{g}(T(C_{i}(v(e),\beta_{k}))) for 1i31\leq i\leq 3 and 1k2N1\leq k\leq 2N.

For any rigid Antoine Cantor set CC in this construction, T(C)T(C) represents the outer torus in the Antoine Construction and T(C)T^{\prime}(C) represents the union of the second stage tori in the construction.

Remark 3.4.

Because E(v(g),βk) and E(v(gβk),βk¯)E(v(g),\beta_{k})\text{ and }E(v(g\circ\beta_{k}),\overline{\beta_{k}}) are identified, it appears that there are two possible definitions for the CiC_{i} on this edge: Hg(Ci(v(e),βk))H_{g}(C_{i}(v(e),\beta_{k})) and Hgβk(Ci(v(e),βk¯))H_{g\circ\beta_{k}}(C_{i}(v(e),\overline{\beta_{k}})). However, Hgβk(Ci(v(e),βk¯))=Hg(Hβk(Hβk¯(Ci(v(e),βki))))=Hg(Ci(v(e),βk)).H_{g\circ\beta_{k}}(C_{i}(v(e),\overline{\beta_{k}}))=H_{g}(H_{\beta_{k}}(H_{\,\overline{\beta_{k}}}(C_{i}(v(e),\beta_{k_{i}}))))=H_{g}(C_{i}(v(e),\beta_{k})).

Remark 3.5.

Note that none of the Ci(v(g),βk)C_{i}(v(g),\beta_{k}) are equivalent to any C(v(g))C(v(g)), and that Ci(v(g),βk)C_{i}(v(g),\beta_{k}) is equivalent to Cj(v(g),β)C_{j}(v(g^{\,\prime}),\beta_{\ell}) if and only if one of the following two conditions holds:

i=j and βk=β, or i=j and βk=β¯.i=j\text{ and }\beta_{k}=\beta_{\ell}\text{, or }i=j\text{ and }\beta_{k}=\overline{\beta_{\ell}}.

The union of the Cantor sets Ci(g,βk)C_{i}(g,\beta_{k}) together with the union of the Cantor sets C(v(g))C(v(g)) is not a Cantor set since it is not compact. To remedy this, we add the point at infinity, denoted by pp, to 3\mathbb{R}^{3} to get S3S^{3}. We then define the Cantor set 𝒞\mathcal{C} associated with G(FN)G(F_{N}) to be: 𝒞=C(G(FN))={Ci(v(g),βk),gFN,1k2N}{C(v(g)),gFN}{p}.\mathcal{C}=C(G(F_{N}))=\{C_{i}(v(g),\beta_{k}),g\in F_{N},1\leq k\leq 2N\}\cup\{C(v(g)),g\in F_{N}\}\cup\{p\}.

4. Main Theorems

We now have 𝒞S3\mathcal{C}\subset S^{3}. One can show that 𝒞\mathcal{C} cannot be separated by any 2-sphere, by an argument similar to that referred to in Remark 1.9. Let =M(FN)\mathcal{M}=M(F_{N}) be the 3-manifold S3𝒞S^{3}-\mathcal{C}. By Remark 1.7, \mathcal{M} is irreducible.

We will show that the embedding homogeneity group of 𝒞S3\mathcal{C}\subset S^{3} is FNF_{N}, and correspondingly, that the end homogeneity group of \mathcal{M} is FNF_{N}.

We use the following three technical lemmas in the proof of Theorem 4.6 below. In reading the first lemma, think of T1T_{1} and T2T_{2} as two linked tori in a stage of an Antoine construction as in Figure 1. The second lemma shows that homeomorphisms of S3S^{3} taking 𝒞\mathcal{C} to itself necessarily fix the point pp. The third lemma shows that homeomorphisms of S3S^{3} taking some C(v(g))C(v(g)) to some C(v(g))C(v(g^{\,\prime})), when restricted to C(v(g))C(v(g)), agree with some Hg1H_{g_{1}} restricted to C(v(g))C(v(g)).

Lemma 4.1.

Let C1C_{1}, C2C_{2} and C3C_{3} be rigid Antoine Cantor sets in 3\mathbb{R}^{3}. Let TiT_{i} and TiT^{\prime}_{i} be the first and second stages in the construction of CiC_{i}. Assume that T1T_{1} and T2T_{2} are linked (and thus are disjoint). Let h:33h:\mathbb{R}^{3}\rightarrow\mathbb{R}^{3} be a homeomorphism such that

  • **

    h(C1)C3h(C_{1})\cap C_{3}\neq\emptyset.

Assume in addition that

  • a)

    h((T1T2)(T1T2))h\left(\frac{\mathstrut}{\mathstrut}\partial(T_{1}\cup T_{2})\cup\partial(T^{\prime}_{1}\cup T^{\prime}_{2})\right) \cap ((T3)(T3))=\left(\frac{\mathstrut}{\mathstrut}\partial(T_{3})\cup\partial(T^{\prime}_{3})\right)=\emptyset,

  • b)

    h(C1)T3C3h(C_{1})\cap T_{3}\subset C_{3}, and

  • c)

    h(C2)T3C3h(C_{2})\cap T_{3}\subset C_{3}.

If h(T1)T3h(T_{1})\subset T_{3}, then

  • I)

    either the geometric index of h(T1)h(T_{1}) in T3T_{3} is 0, h(T2)h(T_{2}) is also contained in T3T_{3}, and the geometric index of h(T2)h(T_{2}) in T3T_{3} is also 0,

  • II)

    or the geometric index of h(T1)h(T_{1}) in T3T_{3} is 11 and C3h(T1)C_{3}\subset h(T_{1}).

Proof.

We have h(T1)T3h(T_{1})\subset T_{3} and we consider the geometric index of h(T1)h(T_{1}) in T3T_{3}.

Index 0: Assume that the geometric index is 0. Then h(T1)h(T_{1}) is contained in a cell BB in T3T_{3}, and so contracts in T3T_{3}.

If (h(T2))\partial(h(T_{2})) does not intersect (B)\partial(B), then either h(T2)Bh(T_{2})\subset B, Bh(T2)B\subset h(T_{2}) or h(T2)h(T_{2}) misses BB. The last case cannot occur because of the linking of h(T2)h(T_{2}) and h(T1)h(T_{1}). In the first case, h(T2)T3h(T_{2})\subset T_{3} and the geometric index of h(T2)h(T_{2}) in T3T_{3} is 0. So condition (I) holds. The second case cannot occur because h(T1)h(T_{1}) and h(T2)h(T_{2}) are disjoint.

If (h(T2))\partial(h(T_{2})) does intersect (B)\partial(B), then h(T2)T3h(T_{2})\subset T_{3} by (a) above. If the geometric index of h(T2)h(T_{2}) in T3T_{3} is 1\geq 1, then h(T2)h(T_{2}) cannot be contained in any component of T3T^{\prime}_{3} by Theorem 1.2. Thus, by (a), h(T2)h(T_{2}) contains any component of T3T^{\prime}_{3} that it intersects. By (c), h(C2)C3h(C_{2})\cap C_{3}\neq\emptyset. So h(T2)h(T_{2}) intersects and thus contains some component D1D_{1} of T3T^{\prime}_{3}. The geometric index of D1D_{1} in h(T2)h(T_{2}) must be 0 by Theorem 1.2. Thus D1D_{1} is contained in a cell in h(T2)h(T_{2}) and contracts in h(T2)h(T_{2}).

Let D1,D2,DmD_{1},D_{2},\ldots D_{m} be the components of T3T^{\prime}_{3}, listed so that DiD_{i} links Di+1D_{i+1}. Since D1D_{1} and D2D_{2} are linked, the Antoine construction guarantees that any contraction of D1D_{1} intersects C3D2C_{3}\cap D_{2}. So h(T2)h(T_{2}) intersects and thus contains D2D_{2} and D2D_{2} has geometric index 0 in h(T2)h(T_{2}). Continuing inductively, all of the DiD_{i} are contained in h(T(2))h(T(2)) and thus h(T2)h(T_{2}) contains C3C_{3}.

Since h(T1)h(T_{1}) is disjoint from h(T2)h(T_{2}), this contradicts condition **.

Index greater than 1: If the geometric index of h(T1)h(T_{1}) in T3T_{3} is greater than 11, then by Theorem 1.2, h(T1)h(T_{1}) cannot be contained in any component of T3T^{\prime}_{3}. So h(T1)h(T_{1}) contains each component of T3T^{\prime}_{3} that it intersects. Let D1,D2,DmD_{1},D_{2},\ldots D_{m} be the components of T3T^{\prime}_{3}, listed so that DiD_{i} links Di+1D_{i+1}. By condition **, h(T1)h(T_{1}) intersects and thus contains some component of T3T^{\,\prime}_{3}, say D1D_{1}. The geometric index of D1D_{1} in h(T1)h(T_{1}) is 0 by Theorem 1.2.

By an argument similar to that in the Index 0 case above, h(T1)h(T_{1}) contains each DiD_{i}, and each DiD_{i} is of index 0 in h(T1)h(T_{1}). By Theorem 1.3, the geometric index of T3T^{\prime}_{3} in h(T1)h(T_{1}) is even. Since the geometric index of T3T^{\prime}_{3} in T3T_{3} is two [1], the geometric index of T3T^{\prime}_{3} in h(T1)h(T_{1}) cannot be 0 and so is at least two. Theorem 1.2 now implies that the geometric index of T3T^{\prime}_{3} in T3T_{3} is at least 4, which is a contradiction. So the the geometric index of h(T1)h(T_{1}) in T3T_{3} cannot be greater than 11.

Index equal to 1: If the geometric index of h(T1)h(T_{1}) in T3T_{3} is 11, then by Theorem 1.2, h(T1)h(T_{1}) cannot be contained in any component of T3T^{\prime}_{3}. An argument similar to that in the previous two cases shows that h(T1)h(T_{1}) contains each component of T3T^{\prime}_{3}. Thus C3h(T1)C_{3}\subset h(T_{1}). So condition (II) holds. ∎

Lemma 4.2.

Let Γ:𝒞𝒞\Gamma:\mathcal{C}\rightarrow\mathcal{C} be a homeomorphism that extends to a homeomorphism of S3S^{3}. Then Γ(p)=p\Gamma(p)=p.

Proof.

The local genus of any point in 𝒞\mathcal{C} other than pp is less than or equal to one because these points are defined by nested sequences of tori which are of genus one. If we can show the local genus of pp is at least 2, then the results mentioned in Remark 1.5 show that Γ(p)=p\Gamma(p)=p.

Remark 4.3.

The local genus of pp in 𝒞\mathcal{C} cannot be 0 because otherwise, there would be arbitrarily small 3-balls containing pp with boundary missing 𝒞\mathcal{C}. These boundary 2-spheres in the complement of 𝒞\mathcal{C} would separate linked stages of some Antoine construction. This cannot happen.

Refer to caption
Figure 6. Start of construction for 𝒞1\mathcal{C}_{1} and 𝒞2\mathcal{C}_{2} in the case F(2)

To see that the local genus of pp in 𝒞\mathcal{C} is at least 2, consider 2 subsets of 𝒞\mathcal{C} that meet in pp. These subsets are obtained by dividing 𝒞C(v(e))\mathcal{C}-C(v(e)) into two subsets that meet in pp.

For a nonidentity gFNg\in F_{N}, with unique reduced representation as βi1βi2βiM\beta_{i1}\circ\beta_{i2}\circ\ldots\circ\beta_{iM} where the βij\beta_{ij} are in g(FN)g(F_{N}), let g1=βi1g_{1}=\beta_{i1}.

Let 𝒞1=k=1N({C(v(g)),g1=βk}i=13{Ci(v(g),βj),g1=βk}){p}, and \text{Let }\mathcal{C}_{1}=\bigcup_{k=1}^{N}\bigg{(}\{C(v(g)),g_{1}=\beta_{k}\}\cup\bigcup_{i=1}^{3}\{C_{i}(v(g),\beta_{j}),g_{1}=\beta_{k}\}\bigg{)}\cup\{p\},\text{\ and }
𝒞2=k=N+12N({C(v(g)),g1=βk}i=13{Ci(v(g),βj),g1=βk}){p}.\mathcal{C}_{2}=\displaystyle\bigcup_{k=N+1}^{2N}\bigg{(}\{C(v(g)),g_{1}=\beta_{k}\}\cup\bigcup_{i=1}^{3}\{C_{i}(v(g),\beta_{j}),g_{1}=\beta_{k}\}\bigg{)}\cup\{p\}.

Figure 6 illustrates the start of the described construction in the case N=2N=2. The Cantor set 𝒞1\mathcal{C}_{1} arises from tori in the upper half of the figure, and the Cantor set set 𝒞2\mathcal{C}_{2} arises from tori in the lower half of the figure.

Note that 𝒞1\mathcal{C}_{1} and 𝒞2\mathcal{C}_{2} intersect in pp. The local genus of pp in each of these 22 Cantor sets is at least 1 by reasoning similar to that in Remark 4.3.

The 𝒞i\mathcal{C}_{i} satisfy the conditions of Theorem 1.6. It follows that the genus of pp in 𝒞\mathcal{C} is \geq 2.

Note: In fact, the local genus of pp in 𝒞\mathcal{C} is \infty. ∎

Lemma 4.4.

If Γ\Gamma is a self homeomorphism of S3S^{3} and Γ(C(v(g)))=C(v(g))\Gamma(C(v(g)))=C(v(g^{\,\prime})) for some g,gFNg,g^{\,\prime}\in F_{N} with g=gg1g^{\,\prime}=g\circ g_{1} then Γ|C(v(g))=Hg1|C(v(g))\Gamma|_{C(v(g))}=H_{g_{1}}\mathstrut|_{C(v(g))}. In particular, if Γ(C(v(e)))=C(v(g))\Gamma(C(v(e)))=C(v(g)) for some gFNg\in F_{N}, then Γ|C(v(e))=Hg|C(v(e))\Gamma|_{C(v(e))}=H_{g}|_{C(v(e))}.

Proof.

Hg1(C(v(g)))=Hg1(Hg(C(v(e))))=Hg1g(C(v(e)))=Hg(C(v(e)))=C(v(g))H_{g_{1}}(C(v(g)))=H_{g_{1}}\left(H_{g}(C(v(e)))\right)=H_{g_{1}\circ g}(C(v(e)))=H_{g^{\,\prime}}(C(v(e)))=C(v(g^{\,\prime})). So both Hg1H_{g_{1}} and Γ\Gamma take C(v(e))C(v(e)) onto C(v(g))C(v(g^{\,\prime})). Thus Hg1Γ1H_{g_{1}}\circ\Gamma^{-1} takes C(v(e))C(v(e)) onto C(v(e))C(v(e)). The rigidity of C(v(e))C(v(e)) implies that Hg1|C(v(e))=Γ|C(v(e))H_{g_{1}}|_{C(v(e))}=\Gamma|_{C(v(e))}. ∎

Theorem 4.5 (Main Theorem).

\mathcal{M} is an irreducible 3-manifold with end homogeneity group FNF_{N}.

This follows immediately from the next theorem.

Theorem 4.6.

𝒞S3\mathcal{C}\subset S^{3} is unsplittable and the embedding homogeneity group of 𝒞S3\mathcal{C}\subset S^{3} is FNF_{N}.

Proof.

The unsplittability was addressed above. Let \mathcal{H} be the embedding homogeneity group of 𝒞\mathcal{C}. Note that the homeomorphisms Hg:33,gFNH_{g}:\mathbb{R}^{3}\rightarrow\mathbb{R}^{3},g\in F_{N}, extend to homeomorphisms Hg:S3S3,gFNH^{\prime}_{g}:S^{3}\rightarrow S^{3},g\in F_{N}, by fixing the point at infinity.

For each gFNg\in F_{N}, let ηg=Hg|𝒞\eta_{g}=H^{\prime}_{g}|_{\mathcal{C}}. Then each ηg\eta_{g} takes 𝒞\mathcal{C} onto 𝒞\mathcal{C}. This follows directly from the definition of C(v(g))=Hg(C(v(e)))C(v(g))=H_{g}(C(v(e))) and Ci(v(g),βk)=Hg(Ci(v(e),βk))C_{i}(v(g),\beta_{k})=H_{g}(C_{i}(v(e),\beta_{k})). The elements {ηg,gFN}\{\eta_{g},g\in F_{N}\} form a subgroup of \mathcal{H} since Hg1Hg2=Hg1g2H^{\prime}_{g_{1}}\circ H^{\prime}_{g_{2}}=H^{\prime}_{g_{1}\circ g_{2}} by Remark 2.2.

Let γ\gamma be any self homeomorphism of 𝒞\mathcal{C} that extends to a homeomorphism Γ\Gamma of S3S^{3}. We will show that γ=η(g)\gamma=\eta(g) for some gFNg\in F_{N}.

Step 1: We first show that Γ(C(v(e)))=C(v(g))\Gamma(C(v(e)))=C(v(g)) for some gFNg\in F_{N}. If this is true, then the definition of C(v(g))C(v(g)) as Hg(C(v(e)))H_{g}(C(v(e))) and Lemma 4.4 shows that Γ|C(v(e))=ηg|C(v(e))\Gamma|_{C(v(e))}=\eta_{g}|_{C(v(e))} Let:

ΛN={T(C(v(g)))|v(g)N}\displaystyle\Lambda_{N}=\{T(C(v(g)))\ |\parallel v(g)\parallel\leq N\} {T(Cj(v(g),βk))|v(g)N},\displaystyle\ \bigcup\ \{T(C_{j}(v(g),\beta_{k}))\ |\parallel v(g)\parallel\leq N\},
ΔN={C(v(g)),|v(g)N}\displaystyle\Delta_{N}=\{C(v(g)),|\parallel v(g)\parallel\leq N\} {Cj(v(g),βk)|v(g)N},and\displaystyle\ \bigcup\ \{C_{j}(v(g),\beta_{k})\ |\parallel v(g)\parallel\leq N\},\text{and}
ΛN={T(C(v(g)))|v(g)N}\displaystyle\Lambda^{\prime}_{N}=\{T^{\prime}(C(v(g)))\ |\parallel v(g)\parallel\leq N\} {T(Cj(v(g),βk))|v(g)N}.\displaystyle\ \bigcup\ \{T^{\prime}(C_{j}(v(g),\beta_{k}))\ |\parallel v(g)\parallel\leq N\}.

Γ(C(v(e)))\Gamma(C(v(e))) does not contain pp by Lemma 4.2. So there is a positive integer N1N_{1} such that Γ(C(v(e)))ΔN1\Gamma(C(v(e)))\subset\Delta_{N_{1}}. Similarly, there is a positive integer N2>N1N_{2}>N_{1} such that Γ1(ΔN1)ΔN2\Gamma^{-1}(\Delta_{N_{1}})\subset\Delta_{N_{2}}.

Using techniques similar to those in [18], or [11], choose a homeomorphism kk of S3S^{3} to itself, fixed on 𝒞\mathcal{C}, so that

(1) k(Γ((ΛN2+1)(ΛN2+1)))((ΛN2+1)(ΛN2+1))=.\displaystyle k\left(\Gamma\left(\partial(\Lambda_{N_{2}+1})\cup\partial(\Lambda^{\prime}_{N_{2}+1})\right)\right)\cap\left(\partial(\Lambda_{N_{2}+1})\cup\partial(\Lambda^{\prime}_{N_{2}+1})\right)=\emptyset.

Let Γ=kΓ\Gamma^{\,\prime}=k\circ\Gamma. Let cc be a point of C(v(e))C(v(e)) and let Γ(c)=Γ(c)=qC~\Gamma^{\,\prime}(c)=\Gamma(c)=q\in\widetilde{C} where C~=C(v(g))\widetilde{C}=C(v(g)) (or =Ci(v(g),βk)=C_{i}(v(g),\beta_{k})) for some gg and where T=T(C(v(g)))T=T(C(v(g))) (or =T(Ci(v(g),βk))=T(C_{i}(v(g),\beta_{k}))). We will show that in fact, Γ(C(v(e)))=Γ(C(v(e)))=C(v(g))\Gamma^{\,\prime}(C(v(e)))=\Gamma(C(v(e)))=C(v(g)) for some gg, and that the second case above cannot occur. Observe that either Γ(T(C(v(e))))IntT\Gamma^{\,\prime}(T(C(v(e))))\subset{\rm{Int}}T or Int(Γ(T(C(v(e)))))T{\rm{Int}}(\Gamma^{\,\prime}(T(C(v(e)))))\supset T by Equation 1 above.

Step 1a: Assume that Γ(T(C(v(e))))Int(T)\Gamma^{\,\prime}(T(C(v(e))))\subset{\rm{Int}}(T). Lemma 4.1 now applies with T(C(v(e)))=T1, any T1(v(e),βi)=T2, and with T=T3T(C(v(e)))=T_{1},\text{ any }T_{1}(v(e),\beta_{i})=T_{2},\text{ and with }T=T_{3}. If Γ(T(C(v(e))))\Gamma^{\,\prime}(T(C(v(e)))) has geometric index 0 in T3T_{3}, choose a linked chain of tori in the construction of C(G(FN))C(G(F_{N})) joining T(C(v(e)))T(C(v(e))) to a T(C(v(g)))T(C(v(g^{\prime}))) where g=N2+1||g^{\prime}||=N_{2}+1. By repeated applications of Lemma 4.1 it follows that Γ(T(C(v(g))))ΔN1\Gamma^{\,\prime}(T(C(v(g^{\prime}))))\subset\Delta_{N_{1}} which is a contradiction. So Γ(T(C(v(g))))\Gamma^{\,\prime}(T(C(v(g)))) has geometric index greater than or equal to 11 in TT. By Lemma 4.1, this geometric index is 1 and C~Γ(T(C(v(g))))\widetilde{C}\subset\Gamma^{\,\prime}(T(C(v(g)))).

Since Γ(𝒞)=𝒞\Gamma(\mathcal{C})=\mathcal{C}, we have C~=Γ(C(v(e))\widetilde{C}=\Gamma(C(v(e)). Since C(v(e))C(v(e)) in not equivalent to any Ci(v(g),βk)C_{i}(v(g),\beta_{k}) by Remarks 3.3 and 3.5 we get C~=C(v(g))\widetilde{C}=C(v(g)) for some gg. It follows from Lemma 4.4 that Γ|C(v(e))=ηg|C(v(e))\Gamma|_{C(v(e))}=\eta_{g}|_{C(v(e))}.

Step 1b: Assume that Int(Γ(T(C(v(e)))))IntT{\rm{Int}}(\Gamma^{\,\prime}(T(C(v(e)))))\supset{\rm{Int}}T. Then (Γ)1(T)Int(T(C(v(e))){(\Gamma^{\,\prime})^{-1}}(T)\subset{\rm{Int}}(T(C(v(e))). The argument from Case I can now be repeated replacing Γ\Gamma^{\,\prime} by (Γ)1(\Gamma^{\,\prime})^{-1} and interchanging TT and T(C(v(e)))T(C(v(e))). It follows that (Γ)1(C~)=C(v(e))(\Gamma^{\,\prime})^{-1}(\widetilde{C})=C(v(e)) and so Γ(C(v(e))=C(v(g))\Gamma^{\,\prime}(C(v(e))=C(v(g)) for some gg as claimed. Again it follows from Lemma 4.4 that Γ|C(v(e))=ηg|C(v(e))\Gamma|_{C(v(e))}=\eta_{g}|_{C(v(e))}.

Step 2: By an argument similar to that in Step 1, for each giFN,g_{i}\in F_{N}, Γ(C(v(gi)))\Gamma(C(v(g_{i}))) =C(gm(i)gi)=C(g_{m(i)}\circ g_{i}) for some gm(i)FNg_{m(i)}\in F_{N}. Also for each ii, jj and kk,

Γ(Cj(v(gi)βk))\Gamma(C_{j}(v(g_{i})\beta_{k})) =Cj(v(gm(i,k)gi),βk)=C_{j}(v(g_{m(i,k)}\circ g_{i}),\beta_{k}) for some gm(i,k)FNg_{m(i,k)}\in F_{N}.

Working inductively outward from C(v(e))C(v(e)), and using the fact that if T1T_{1} and T2T_{2} are linked tori, then Γ(T1)\Gamma(T_{1}) and Γ(T2)\Gamma(T_{2}) are linked, one sees that each gm(i)=gg_{m(i)}=g and each gm(i,k)=gg_{m(i,k)}=g.

By Lemma 4.4 it follows that each Γ|Cj(v(gi)βk)=ηg|Cj(v(gi)βk)\Gamma|_{C_{j}(v(g_{i})\beta_{k})}=\eta_{g}|_{C_{j}(v(g_{i})\beta_{k})}, and that each Γ|C(v(gi))=ηg|C(v(gi))\Gamma|_{C(v(g_{i}))}=\eta_{g}|_{C(v(g_{i}))} It now follows that Γ=η(g)\Gamma=\eta(g) for the gg from Steps 1 and 2. This shows that {η(g),gFN}\{\eta(g),g\in F_{N}\} is in fact, the group \mathcal{H} and that \mathcal{H} is isomorphic to FNF_{N}. ∎

The method used in the construction of 𝒞\mathcal{C} can be used for any Cayley graph of a finitely generated group FF for which the graph automorphisms have certain extension properties. This observation is given in the next theorem.

Theorem 4.7.

Suppose FF is a finitely presented group with a Cayley Graph G(F)G(F) in S3S^{3}. Suppose the graph automorphisms hgh_{g} for gFg\in F can be extended to homeomorphisms HgH_{g} of S3S^{3}. Suppose also that for every pair of group elements g1,g2g_{1},g_{2}, Hg1Hg2=Hg1g2H_{g_{1}}\circ H_{g_{2}}=H_{g_{1}\circ g_{2}}. Then there is an open irreducible 3-manifold MFM_{F} with embedding homogeneity group isomorphic to FF.

Proof.

The construction of a collection of Cantor sets modeled on the graph, and the proof analogous to the proof of Theorem 4.6 go through in this case. ∎

Questions

In [10], the authors showed that for every finitely generated abelian group GG, there is an irreducible open 3-manifold MGM_{G} with end homogeneity group isomorphic to GG. In this paper, we show that for any finitely generated free group FNF_{N}, there is an irreducible open 3-manifold MFNM_{F_{N}} with end homogeneity group FNF_{N}.

Question (1).

Which non-abelian finitely generated groups can arise as end homogeneity groups of (irreducible) open 3-manifolds?

In light of Theorem 4.7, this leads to the following question.

Question (2).

Which non-abelian finitely generated groups have Cayley graphs embeddable in S3S^{3} with the properties listed in Theorem 4.7?

A related question is the following.

Question (3).

If not all finitely generated non-abelian groups have Cayley graphs with the properties listed in Theorem 4.7, is there a way to characterize which ones do have this property?

Appendix

This section lists some of the important notation used in the paper.

  • FNF_{N} is the free group on N generators.

  • g(FN)={a1,,aN,a1¯,,aN¯}g(F_{N})=\{a_{1},\ldots,a_{N},\overline{\mathstrut a_{1}},\ldots,\overline{\mathstrut a_{N}}\}, is the full set of generators for FNF_{N}.

  • βj=αj\beta_{j}=\alpha_{j} for 1jN1\leq j\leq N and βj=αjN¯\beta_{j}=\overline{\mathstrut\alpha_{j-N}} for N+1j2NN+1\leq j\leq 2N.

  • G(FN)G(F_{N}) is the Cayley graph constructed in 3\mathbb{R}^{3} for FNF_{N}.

  • v(e),v(βj),v(g)v(e),v(\beta_{j}),v(g) are vertices of G(FN)G(F_{N}) associated with group elements.

  • E(v(g),βk)=E((v(g),v(gβk)))E(v(g),\beta_{k})=E((v(g),v(g\circ\beta_{k}))) is the oriented edge labeled βk\beta_{k} from v(g)v(g) to v(gβk)v(g\circ\beta_{k}).
    This edge is the regarded the same as E(v(gβk),βk¯)=E(v(gβk),v(g))E(v(g\circ\beta_{k}),\overline{\beta_{k}})=E(v(g\circ\beta_{k}),v(g)).

  • hgh_{g} is the automorphism of G(FN)G(F_{N}) given by hg(v(gi))=v(ggi)h_{g}(v(g_{i}))=v(g\circ g_{i}),
    hg(E(v(gi),βk))=E(v(ggi),βk)h_{g}(E(v(g_{i}),\beta_{k}))=E(v(g\circ g_{i}),\beta_{k}).

  • HgH_{g} is the extension of hgh_{g} to a homeomorphism of 3\mathbb{R}^{3}.

  • B(v(g))=Hg(B(v(e)))B(v(g))=H_{g}(B(v(e))) is a 3-ball about the vertex v(g)v(g).

  • D(g,βk)=Hg(D(e,βk))D(g,\beta_{k})=H_{g}(D(e,\beta_{k})) is a tube joining B(v(g))B(v(g)) to B(v(gβk))B(v(g\circ\beta-k)).

  • C(v(g))=Hg(C(v(e))C(v(g))=H_{g}(C(v(e)) is a rigid Cantor set in B(v(g))B(v(g)).

  • C1(v(g),βk),C2(v(g),βk),andC3(v(g),βk)C_{1}(v(g),\beta_{k}),C_{2}(v(g),\beta_{k}),andC_{3}(v(g),\beta_{k}), form a linked chain of rigid Cantor sets joining C(v(g))C(v(g)) to C(v(gβk))C(v(g\circ\beta_{k})). Ci(v(g),βk)=Hg(Ci(v(e)),βk)C_{i}(v(g),\beta_{k})=H_{g}(C_{i}(v(e)),\beta_{k}).

  • C(G(FN))=𝒞C(G(F_{N}))=\mathcal{C}. MFN=M_{F_{N}}=\mathcal{M}.

Acknowledgements

The authors would like to thank the referee for many helpful suggestions and comments. These suggestions helped to clarify the arguments in the paper. Both authors were supported in part by the Slovenian Research Agency grant BI-US/19-21-024. The second author was supported in part by the Slovenian Research Agency grants P1-0292, N1-0114, N1-0083, N1-0064, and J1-8131.

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