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Heegaard splittings of 3–manifolds (Haifa 2005) \conferencestart10 July 2005 \conferenceend19 July 2005 \conferencenameHeegaard splittings of 3–manifolds \conferencelocationHaifa \editorCameron Gordon \givennameCameron \surnameGordon \editorYoav Moriah \givennameYoav \surnameMoriah \givennameCameron McA \surnameGordon \urladdr \subjectprimarymsc200057M27 \subjectprimarymsc200057M25 \subjectsecondarymsc200057M07 \volumenumber12 \issuenumber \publicationyear2007 \papernumber16 \startpage401 \endpage411 \MR \Zbl \published3 December 2007 \publishedonline3 December 2007 \proposed \seconded \corresponding \version

{htmlabstract}

These are problems on Heegaard splittings, that were raised at the Workshop, listed according to their contributors: David Bachman, Mario Eudave-Mu#241;oz, John Hempel, Tao Li, Yair Minsky, Yoav Moriah and Richard Weidmann. On pages 285ndash;298 of this monograph Hyam Rubinstein gives a personal collection of problems on 3ndash;manifolds.

Heegaard splittings of 3–manifolds (Haifa 2005)
Problems

Cameron McA Gordon (Editor) University of Texas at Austin
Department of Mathematics

1 University Station – C1200
Austin, TX 78712-0257
USA
gordon@math.utexas.edu
(22 October 2007)
Abstract

These are problems on Heegaard splittings, that were raised at the Workshop, listed according to their contributors: David Bachman, Mario Eudave-Muñoz, John Hempel, Tao Li, Yair Minsky, Yoav Moriah and Richard Weidmann. In [34] Hyam Rubinstein gives a personal collection of problems on 3–manifolds.

keywords:
Problems
keywords:
Heegaard splitting
keywords:
3–manifold
{asciiabstract}

These are problems on Heegaard splittings, that were raised at the Workshop, listed according to their contributors: David Bachman, Mario Eudave-Munoz, John Hempel, Tao Li, Yair Minsky, Yoav Moriah and Richard Weidmann. On pages 285-298 of this monograph Hyam Rubinstein gives a personal collection of problems on 3-manifolds. {webabstract} These are problems on Heegaard splittings, that were raised at the Workshop, listed according to their contributors: David Bachman, Mario Eudave-Muñoz, John Hempel, Tao Li, Yair Minsky, Yoav Moriah and Richard Weidmann. On pages 285–298 of this monograph Hyam Rubinstein gives a personal collection of problems on 3–manifolds.

1 David Bachman

We analyze what is known, and what is not known, about the following question:

Question 1.1.

Which manifolds have infinitely many Heegaard splittings of the same genus, and how are the splittings constructed?

The only known examples of 3–manifolds that admit infinitely many Heegaard splittings of the same genus are given in Sakuma [35], Morimoto and Sakuma [28] and Bachman and Derby-Talbot [3]. By Li’s proof of the Waldhausen conjecture [19], any such manifold must have an essential torus TT. In the presence of such a torus, it is easy to see how an infinite number of Heegaard splittings of the same genus might arise. Simply take any splitting that intersects TT, and Dehn twist the splitting about TT. But is this the only way such an infinite collection might arise? What can be said about the manifold if this construction does not produce an infinite collection of non-isotopic splittings?

We analyze what is known when the torus is separating. (Some of the results described below hold in the non-separating case as well.) Suppose then TT is an essential torus which separates a closed, orientable, irreducible 3–manifold MM into XX and YY. Then we may think of MM as being constructed from XX and YY by gluing by some homeomorphism, ϕ\coXY\phi\co\partial X\to\partial Y.

Fix separate triangulations of XX and YY (these do not have to agree in any way on TT). By a result of Jaco and Sedgwick [13] the sets ΔX\Delta_{X} and ΔY\Delta_{Y} of slopes on X\partial X and Y\partial Y that bound normal or almost normal surfaces in XX and YY are finite (see Bachman [2] for a further discussion of the almost normal case). We may thus define the distance d(T)d(T) of TT to be the distance between the sets ϕ(ΔX)\phi(\Delta_{X}) and ΔY\Delta_{Y}, as measured by the path metric in the Farey graph of Y\partial Y.

Theorem 1.1 (Bachman, Schleimer, Sedgwick [4]).

If d(T)2d(T)\geq 2 then every Heegaard splitting of MM is an amalgamation of Heegaard splittings of XX and YY.

The relevance of this theorem is that Dehn twisting an amalgamation about the torus TT will not produce non-isotopic Heegaard splittings. Hence, when d(T)2d(T)\geq 2 the manifold MM can only admit an infinite collection of non-isotopic Heegaard splittings if XX or YY does. The converse, however, is more subtle. That is, if we know XX or YY has infinitely many non-isotopic Heegaard splittings of the same genus, then does it follow that MM does as well? We conjecture the following:

Conjecture 1.2.

If d(T)3d(T)\geq 3 and XX or YY has infinitely many Heegaard splittings of the same genus then MM does as well.

When d(T)=0d(T)=0 or 11, there is the possibility that there is a strongly irreducible Heegaard splitting of MM. Let HH denote such a splitting surface. By a classic result of Kobayashi, HH can be isotoped to meet TT in a non-empty collection of loops that are essential on both surfaces.

One way Dehn twisting HH about TT can fail to produce a non-isotopic Heegaard splitting is if HXH\cap X is a fiber of a fibration of XX. Then the effect of the Dehn twist can be “undone” by pushing HXH\cap X around the fibration. This is precisely what happens when TT is a separating vertical torus in a Seifert Fibered space. (For a complete resolution of \fullrefMainQuestion in the case of Seifert Fibered spaces, see [3].) A second thing that may happen is that HXH\cap X is the union of two pages of an open book decomposition of XX. Then the effect of the Dehn twist can be undone by spinning HXH\cup X about the open book decomposition. We conjecture that these are the only ways that Dehn twisting HH about TT can fail to produce non-isotopic Heegaard splittings:

Conjecture 1.3.

If MM admits an essential torus TT, separating MM into XX and YY, and a strongly irreducible Heegaard splitting HH, then either Dehn twisting HH about TT produces an infinite collection of non-isotopic Heegaard splittings, or HH can be isotoped so that HXH\cap X or HYH\cap Y is either a fiber of a fibration of XX or YY or two pages of an open book decomposition of XX or YY.

2 Mario Eudave-Muñoz

Let FF be a closed surface of genus 11 standardly embedded in S3S^{3}, that is, it bounds a solid torus on each of its sides. We say that a knot KK has a (1,b)(1,b)presentation or that it is in a (1,b)(1,b)position, if KK has been isotoped to intersect FF transversely in 2b2b points that divide KK into 2b2b arcs, so that the bb arcs in each side can be isotoped, keeping the endpoints fixed, to disjoint arcs on FF. The genus–1–bridge number of KK, b1(K)b_{1}(K), is the smallest integer nn for which KK has a (1,n)(1,n)–presentation. We say that a knot is a (1,n)(1,n)knot if b1(K)nb_{1}(K)\leq n. If KK is a (1,1)(1,1)–knot, then it is easy to see that KK has tunnel number one. On the other hand, if KK has tunnel number one, it seems to be very difficult to determine b1(K)b_{1}(K). It has been of interest to find tunnel number one knots with large genus–1–bridge number, see for example Kobayashi and Rieck [16].

Moriah and Rubinstein [24] showed the existence of tunnel number one knots KK with b1(K)2b_{1}(K)\geq 2. Morimoto, Sakuma and Yokota also showed this, and gave explicit examples of knots KK, with tunnel number one and b1(K)=2b_{1}(K)=2 [29]. It was shown by Eudave-Muñoz [7], that many of the tunnel number one knots KK constructed in [5] are not (1,1)(1,1)–knots; this was extended in [8], where it is shown that many such knots are not (1,2)(1,2)–knots. We remark that such knots can be explicitly described, for example the knot KK shown in Figure 13 of [8] satisfies 3b1(K)43\leq b_{1}(K)\leq 4. Combining results of [6] and [9], it is also possible to give explicit examples of knots KK, with tunnel number one and b1(K)=2b_{1}(K)=2, for example the knot shown in Figure 4 of [6]. Valdez-Sánchez and Ramírez-Losada have also shown explicit examples of tunnel number one knots KK with b1(K)=2b_{1}(K)=2 (personal communication). These knots bound punctured Klein bottles but are not contained in the (1,1)(1,1)–knots bounding Klein bottles determined by the same authors [33].

Johnson and Thompson [14], and independently Minsky, Moriah and Schleimer [22] have shown that for any given nn, there exist tunnel number one knots which are not (1,n)(1,n)–knots. The two papers use similar techniques, prove the existence of such knots, but do not give explicit examples. For a tunnel number one knot, let Σ\Sigma be the Heegaard splitting of the knot exterior determined by the unknotting tunnel, and let d(Σ)d(\Sigma) denote the Hempel distance of the splitting [12]. In [14] and [22] the existence of tunnel number one knots with large Hempel distance is shown, and then results of Scharlemann and Tomova [37], [40] are used to ensure the knots have large genus–1–bridge number.

We propose the following problems:

Problem 2.1.

For a given integer nn, give explicit examples of tunnel number one knots KK with b1(K)nb_{1}(K)\geq n.

Problem 2.2.

For a given integer NN, give explicit examples of tunnel number one knots with d(Σ)Nd(\Sigma)\geq N.

Problem 2.3.

For a given integer nn, give explicit examples of tunnel number one knots KK with b1(K)nb_{1}(K)\geq n, but with bounded Hempel distance, say with d(Σ)=2d(\Sigma)=2.

3 John Hempel

Questions on the curve complex

Let SS be a surface and C(S)C(S) be its curve complex whose vertices are the isotopy classes of essential simple closed curves in SS and whose nn–simplexes are determined by n+1n+1 distinct vertices with pairwise disjoint representatives. The distance between vertices is the number of edges in a minimal edge path joining them. Understanding this distance function is a daunting task – it is hard to tell where one is headed as one moves away from a given vertex:

Question 3.1.

Given vertices x,yx,y of C(S)C(S) is there an “easy” way to find a vertex x1x_{1} with xx1=x\cap x_{1}=\emptyset and d(x1,y)=d(x,y)1d(x_{1},y)=d(x,y)-1?

One answer is given by K Shackleton [38], but it involves extending the curves to multicurves which satisfy an additional “tightness” condition and requires a search space whose size grows very rapidly with the complexity of the problem. Also, the complexity is measured in terms of the intersection numbers of the multicurves involved. This may not be the most natural measure and could be a distraction. I am hoping for something easier. The difficulty will be in making a proof.

If d(x,y)>2d(x,y)>2, then xyx\cup y splits SS into contractible regions, each with an even number of edges, alternating between xx and yy. We assume there are no bigons. Euler characteristic calculations yield that most of these regions are squares. When we look in TT, a component of SS split along xx, we see families of parallel arcs from yy successively in the boundaries of these squares whose unions we call yystacks. TT deforms to a graph Γ\Gamma with one vertex in each large region of SyS-y and one edge crossing each yy–stack (in TT). Choose a maximal tree Δ\Delta in Γ\Gamma. This determines a free basis for π1(T)\pi_{1}(T) whose elements are represented by simple closed curves each of which crosses exactly one of the yy–stacks corresponding to an edge of ΓΔ\Gamma-\Delta and crossing it once. We call any such basis a yy–determined free basis and its elements yy–determined free generators. They are in many ways the most simple, relative to yy, curves in SxS-x. It is natural to ask:

Question 3.2.

Is there some yy–determined free generator x1x_{1} for π1(T)\pi_{1}(T) with d(x1,y)d(x_{1},y) <d(x,y)<d(x,y)? Does every yy–determined free basis contain such an element?

Caution: there are examples in which not every yy–determined free generator, x1x_{1} satisfies d(x1,y)<d(x,y)d(x_{1},y)<d(x,y). If \fullrefQ2 can’t be answered, then:

Question 3.3.

In terms of word length, in a yy–determined free basis, how far must we look in order to find a simple closed curve x1Tx_{1}\subset T with d(x1,y)<d(x,y)d(x_{1},y)<d(x,y)?

4 Tao Li

Let M1M_{1} and M2M_{2} be two manifolds with connected boundary M1M2S\partial M_{1}\cong\partial M_{2}\cong S and ϕ\coM1M2\phi\co\partial M_{1}\to\partial M_{2} a homeomorphism. If one glues M1M_{1} to M2M_{2} by identifying xx to ϕ(x)\phi(x) for each xM1x\in\partial M_{1}, one obtains a closed manifold MM. We say that MM is an amalgamation of M1M_{1} and M2M_{2}.

Let 𝒟i\mathcal{D}_{i} (i=1,2i=1,2) be the set of curves in Mi\partial M_{i} that bound essential disks in MiM_{i}. We propose the following conjecture.

Conjecture 4.1.

There is an essential curve 𝒞i\mathcal{C}_{i} (i=1,2i=1,2) in Mi\partial M_{i} such that if the distance between 𝒟2𝒞2\mathcal{D}_{2}\cup\mathcal{C}_{2} and ϕ(𝒟1𝒞1)\phi(\mathcal{D}_{1}\cup\mathcal{C}_{1}) in the curve complex 𝒞(S)\mathcal{C}(S) (S=M2S=\partial M_{2}) is sufficiently large, then either the minimal-genus Heegaard splitting of M=M1ϕM2M=M_{1}\cup_{\phi}M_{2} is an amalgamation or SS itself is a minimal-genus Heegaard surface in which case both M1M_{1} and M2M_{2} are handlebodies.

\fullref

Camal is a generalization of two recent theorems. In the case that M1M_{1} and M2M_{2} are atoroidal and have incompressible boundaries, ie, 𝒟1=𝒟2=\mathcal{D}_{1}=\mathcal{D}_{2}=\emptyset, the conjecture is proved by Souto [39] and Li [20]. Note that [20] also gives an algorithm to find 𝒞1\mathcal{C}_{1} and 𝒞2\mathcal{C}_{2}.

In the case that both M1M_{1} and M2M_{2} are handlebodies, 𝒞1\mathcal{C}_{1} and 𝒞2\mathcal{C}_{2} can be chosen to be empty and \fullrefCamal follows from a recent theorem of Scharlemann and Tomova [37]. The theorem of Scharlemann and Tomova can be formulated as: if the distance between 𝒟2\mathcal{D}_{2} and ϕ(𝒟1)\phi(\mathcal{D}_{1}) (ie, the Hempel distance) is large, then the genus of any other Heegaard splitting must be large unless it is a stabilized copy of SS.

5 Yair Minsky

For a handlebody HH we have an inclusion of mapping class groups, MCG(H)<MCG(H)MCG(H)<MCG(\partial H). If M=H+SHM=H_{+}\cup_{S}H_{-} is a Heegaard splitting we denote Γ±=MCG(H±)\Gamma_{\pm}=MCG(H_{\pm}) <MCG(S)<MCG(S), and moreover let Γ±0\Gamma^{0}_{\pm} be the kernel of the map MCG(H±)MCG(H_{\pm})\toOut(π1(H±)){\rm Out}(\pi_{1}(H_{\pm})) (ie, Γ±0\Gamma^{0}_{\pm} is the group of mapping classes of H±H_{\pm} that are homotopic to the identity on H±H_{\pm}).

Question 5.1.

When is Γ+Γ\Gamma_{+}\cap\Gamma_{-} finite? … finitely generated? … finitely presented?

Question 5.2.

When is Γ+,Γ\langle\Gamma_{+},\Gamma_{-}\rangle equal to the amalgamation Γ+Γ+ΓΓ\Gamma_{+}*_{\Gamma_{+}\cap\Gamma_{-}}\Gamma_{-}?

Question 5.3.

When is the map Γ+ΓMCG(M)\Gamma_{+}\cap\Gamma_{-}\to MCG(M) injective?

When M=S3M=S^{3} and genus(S)=2{\rm genus}(S)=2, Akbas [1] proved Γ+Γ\Gamma_{+}\cap\Gamma_{-} is finitely presented. (Finitely generated has a longer history starting with Goeritz [11] – for details see Scharlemann [36].)

Let Δ±𝒞(S)\Delta_{\pm}\subset{\cal C}(S) be the set of (isotopy classes of) simple curves in SS which bound disks in H±H_{\pm}. Let Z𝒞(S)Z\subset{\cal C}(S) be the simple curves in SS that are homotopic to the identity in MM. Note that ZZ contains Δ±\Delta_{\pm}, and is invariant under Γ±0\Gamma^{0}_{\pm}.

Namazi [30] showed if the distance of the splitting (dist𝒞(S)(Δ+,Δ){\rm dist}_{{\cal C}(S)}(\Delta_{+},\Delta_{-})) is sufficiently large then Γ+Γ\Gamma_{+}\cap\Gamma_{-} is finite. Note also the Geometrization Theorem plus Hempel [12], plus Mostow rigidity plus Gabai–Meyerhoff–Thurston [10], implies that the image of Γ+Γ\Gamma_{+}\cap\Gamma_{-} in MCG(M)MCG(M) is finite when the splitting distance is at least 3.

Question 5.4.

When is ZZ equal to the orbit Γ+0,Γ0(Δ+Δ)\langle\Gamma^{0}_{+},\Gamma^{0}_{-}\rangle(\Delta_{+}\cup\Delta_{-})?

Remarks\quaWhen M=S3M=S^{3} or a connected sum of S2×S1S^{2}\times S^{1}’s, with the natural splitting, equality holds trivially. If MM is a lens space Lp,qL_{p,q}, with p2p\geq 2, and SS is the torus, then they are not equal – ZZ is all of 𝒞(S)=\Q{}{\cal C}(S)=\Q\cup\{\infty\}, whereas the orbit of Δ+Δ={01,pq}\Delta_{+}\cup\Delta_{-}=\{\frac{0}{1},\frac{p}{q}\} under Γ+0,Γ0<SL(2,\Z)\langle\Gamma^{0}_{+},\Gamma^{0}_{-}\rangle<SL(2,\Z) is strictly smaller than \Q{}\Q\cup\{\infty\}. One might reasonably ask if there is equality when MM is hyperbolic, or if the splitting distance is sufficiently large.

6 Yoav Moriah

Question 6.1.

Give an example of a weakly reducible but non-stabilized non-minimal Heegaard splitting of a closed 3–manifold.

There are plenty of examples for manifolds with strongly irreducible Heegaard splittings of arbitrarily high genus. However there are no examples of manifolds (closed or with a single boundary component) with a weakly reducible but non-stabilized non-minimal Heegaard splitting.

Question 6.2.

Prove that if a manifold has strongly irreducible Heegaard splittings of arbitrarily high genus then the Heegaard splittings are of the form H+nKH+nK where HH and KK are surfaces with KK perhaps not connected. (See Moriah, Schleimer and Sedgwick [25] and Li [19].) Or give a counterexample.

Question 6.3.

There are examples by Kobayashi and Rieck (see below) of a 33–manifold which has both a weakly reducible and strongly irreducible minimal genus Heegaard splitting. These examples are very particular. Are there other such examples of a different nature?

Theorem 6.1 (T Kobayashi and Y Rieck [18]).

There are infinitely many 33–manifolds which have both strongly irreducible and weakly reducible Heegaard splittings of minimal genus.

Proof.

Let X=S3N(K1)X=S^{3}-N(K_{1}), Y=S3N(K2)Y=S^{3}-N(K_{2}) and Z=S3N(K3)Z=S^{3}-N(K_{3}), where K1=T(2,3)K_{1}=T_{(2,3)} the trefoil knot, K2=L(α,β)K_{2}=L(\alpha,\beta) with α\alpha even, is any 22–bridge link which is not the Hopf link and K3=K(2,5)K_{3}=K(2,5) is the figure 88 knot. Let μ1\mu_{1} and μ2\mu_{2} be meridians of the 22–bridge link L(α,β)L(\alpha,\beta), λ\lambda be the longitude of K3K_{3} and γ\gamma be the boundary of the annulus in XX.

Attach XX and ZZ to YY by gluing their tori boundaries so that γ\gamma is mapped to μ1\mu_{1} and λ\lambda to μ2\mu_{2}. We obtain a closed 33–manifold MM with incompressible tori. As the genus two toroidal 33–manifolds are classified by Kobayashi [15] this manifold cannot have genus 2. The surface SS obtained from the bridge sphere Σ\Sigma union the annulus in the trefoil complement and the two genus one Seifert surfaces of the figure 88 complement is a closed surface of genus g=1χ(S)2=1((2)+(2)+0)/2=3g=1-\frac{\chi(S)}{2}=1-((-2)+(-2)+0)/2=3. Hence it is a minimal genus Heegaard splitting if it is a Heegaard surface.

Let V1,V2V_{1},V_{2} be the two components of S3N(K1)S^{3}-N(K_{1}). So on one side of SS we have at the first stage the solid torus V1V_{1}, say, glued to the genus two handlebody W1W_{1}, which is one of the two components W1,W2W_{1},W_{2} of YΣY-\Sigma, along a primitive meridional annulus to obtain a genus two handlebody. This handlebody is glued in the second stage to the genus two handlebody which is a regular neighborhood of the Seifert surface along a primitive meridional annulus. So we get a genus three handlebody U1U_{1}.

On the other side of SS we have V2V_{2} glued to the genus two handlebody W2W_{2} along a primitive meridional annulus to obtain a genus two handlebody which is then glued again along a primitive meridional annulus to a genus two handlebody which is a regular neighborhood of the Seifert surface of the figure 88 knot complement. Thus we get a genus three handlebody U2U_{2} and (U1,U2)(U_{1},U_{2}) is a genus three Heegaard splitting for MM.

In [15, Proposition 3.1] Kobayashi proves that a Heegaard splitting of the form (U1,U2)(U_{1},U_{2}) is always strongly irreducible if the link L(α,β)L(\alpha,\beta) is not trivial or a Hopf link.

Now consider the union along the torus boundary of XX and YY. This is a manifold with a minimal genus two Heegaard splitting and with one torus boundary component. Hence when this Heegaard splitting is amalgamated with the genus two Heegaard splitting of ZZ we obtain a genus three Heegaard splitting for MM which is weakly reducible as it is obtained by amalgamation. ∎

Conjecture 6.2.

Let K1K_{1} and K2K_{2} be prime knots in S3S^{3} then t(K1#K2)t(K1)+t(K2)t(K_{1}\#K_{2})\leq t(K_{1})+t(K_{2}) if and only if one of KiK_{i} has a minimal genus Heegaard splitting with primitive meridian. (See Moriah [23].)

Recently T Kobayashi and Y Rieck disproved the conjecture for knots which are not prime (see [17]). The conjecture is known by work of Morimoto for tunnel number one knots and for knots which are connected sums of two prime knots each of which is also mm–small. (See [23] for more references.)

Conjecture 6.3.

Given a knot KS3K\subset S^{3} which is not γ\gamma–primitive then a boundary stabilization of a minimal genus Heegaard splitting of E(K)E(K) is non-stabilized.

Conjecture 6.4.

All twisted torus knots of type K=T(p,q,2,r)K=T(p,q,2,r) which are not μ\mu–primitive have a unique (minimal) genus two Heegaard splitting. (See Moriah and Sedgwick [26].)

Conjecture 6.5.

What are the properties of meridional essential surfaces which ensure that the tunnel number degenerate? Can these surfaces be classified?

Question 6.4.

Are there knots which are not K1=Kn(2,3,3,2)K_{1}=K^{n}(-2,3,-3,2) and 22–bridge knots so that t(K1#K2)<t(K1)+t(K2)t(K_{1}\#K_{2})<t(K_{1})+t(K_{2})? (See Morimoto [27].)

Question 6.5.

Does rank equal genus for hyperbolic 33–manifolds?

In [21] Lustig and Moriah defined a condition on complete disks systems in a Heegaard splitting, called the double rectangle condition. It was shown that if a manifold has a Heegaard splitting which has some complete disk system which satisfies this condition then there are only finitely many such disk systems with that property. However the double rectangle condition is clearly non-“generic”. Is it possible to define some other condition which will be “generic” in some reasonable sense? The intuition is that if the Heegaard distance of the splitting is sufficiently high then some form of this might be possible.

7 Richard Weidmann

Let (M;V,W)(M;V,W) be a Heegaard splitting of genus nn. Let g1,,gnπ1(M)g_{1},\ldots,g_{n}\in\pi_{1}(M) be the elements corresponding to a spine of VV.

Question 7.1.

When is g1,,gn1\langle g_{1},\ldots,g_{n-1}\rangle a free group of rank n1n-1?

(This would be a kind of “Freiheitsatz”.) For instance, what happens with the Casson–Gordon examples of strongly irreducible splittings of a fixed MM of arbitrarily high genus?

Note that the freeness holds for the examples exhibited by Namazi [31] and Namazi–Souto [32].

Question 7.2.

Find (3–manifold) groups that have only finitely many irreducible Nielsen equivalence classes of generating tuples.

Here a nn–tuple is called irreducible if it is not Nielsen equivalent to a tuple of type (x1,,xn1,1)(x_{1},\ldots,x_{n-1},1). Note that free groups and free Abelian groups have this property, in fact for those groups there is precisely one irreducible Nielsen equivalence class. Note that for Heegaard splittings it has been shown by Tao Li that closed non-Haken 3–manifolds only have finitely many isotopy classes of irreducible Heegaard splittings so those groups might be potential examples.

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