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A new family of minimal ideal triangulations
of cusped hyperbolic 3–manifolds

J. Hyam Rubinstein    Jonathan Spreer and Stephan Tillmann J. Hyam Rubinstein
School of Mathematics and Statistics, The University of Melbourne, VIC 3010, Australia
[email protected]
—–
Jonathan Spreer
School of Mathematics and Statistics F07, The University of Sydney, NSW 2006 Australia
[email protected]
—–
Stephan Tillmann
School of Mathematics and Statistics F07, The University of Sydney, NSW 2006 Australia
[email protected]
Abstract

Previous work of the authors with Bus Jaco determined a lower bound on the complexity of cusped hyperbolic 33–manifolds and showed that it is attained by the monodromy ideal triangulations of once-punctured torus bundles. This paper exhibits an infinite family of minimal ideal triangulations of Dehn fillings on the link 8938^{3}_{9} that also attain this lower bound on complexity.

keywords:
3–manifold, minimal triangulation, layered triangulation, efficient triangulation, complexity
\primaryclass

57M25, 57N10 \makeshorttitle

1 Introduction

We refer to [10] for background and precise definitions used in this paper and only give a quick summary here. For a cusped orientable hyperbolic 3–manifold MM of finite volume, the norm α||\ \alpha\ || of a non-trivial class αH2(M,2)\alpha\in H_{2}(M,\mathbb{Z}_{2}) is the negative of the maximal Euler characteristic of a properly embedded surface SS (no component of which is a sphere) representing the class. Any surface SS with [S]=α[S]=\alpha and χ(S)=α-\chi(S)=||\ \alpha\ || is taut if no component of SS is a sphere or a torus. A class αH2(M,2)\alpha\in H_{2}(M,\mathbb{Z}_{2}) determines a labelling of the ideal edges of an ideal triangulation of MM by elements in 2={0,1}\mathbb{Z}_{2}=\{0,1\}. These can be interpreted as edge weights of a normal surface, called the canonical normal representative of α.\alpha.

The complexity c(M)c(M) is the minimal number of ideal tetrahedra in an ideal triangulation of M.M. In [10, Theorem 1], the authors and Bus Jaco obtain the following lower bound on the complexity of a cusped hyperbolic 33-manifold:

Theorem 1.

[10] Let 𝒯\mathcal{T} be an ideal triangulation of the cusped orientable hyperbolic 33–manifold MM of finite volume. If HH2(M,2)H\leq H_{2}(M,\mathbb{Z}_{2}) is a rank 22 subgroup, then the number of ideal tetrahedra |𝒯||\mathcal{T}| satisfies

|𝒯|c(M)0αHα.|\mathcal{T}|\geq c(M)\geq\sum\limits_{0\neq\alpha\in H}||\ \alpha\ ||.

Moreover, in the case of equality the triangulation is minimal and each canonical normal representative of a non-zero element in HH2(M,2)H\leq H_{2}(M,\mathbb{Z}_{2}) is taut and meets each tetrahedron in a quadrilateral disc.

It is shown in [10] that the above bound implies that the monodromy ideal triangulations of the hyperbolic once-punctured torus bundles are minimal. This note presents another infinite family of once-cusped hyperbolic 33-manifolds Mk,nM_{k,n}, admitting triangulations 𝒯k,n\mathcal{T}_{k,n} which achieve the lower bound in Theorem 1. These manifolds are shown to arise from Dehn surgery on the link 893.8^{3}_{9}. What makes these triangulations interesting is that their structure is different from the structure of the monodromy ideal triangulations, and that they do not feature layered solid tori as Dehn fillings (as, for instance, the canonical triangulations exhibited by Guéritaud and Schleimer [7]). We now state the main theorem of this paper (the relevant definitions and an outline of the proof are given in Section 2):

Theorem 2.

Let k,n3k,n\geq 3 be odd integers. The identification space Mk,nM_{k,n} of the triangulation 𝒯k,n\mathcal{T}_{k,n} is hyperbolic and homeomorphic to the manifold obtained from the complement of 8938^{3}_{9} by Dehn filling the symmetric cusp with slope (k,1)(-k,1) and one of the other cusps with slope (n+1,1)(n+1,1). Here, the natural geometric framing is used for the cusps. The triangulation 𝒯k,n\mathcal{T}_{k,n} achieves equality in Theorem 1 with H=H2(Mk,n,2)22H=H_{2}(M_{k,n},\mathbb{Z}_{2})\cong\mathbb{Z}_{2}\oplus\mathbb{Z}_{2}, and, in particular, Mk,nM_{k,n} has complexity k+n.k+n.

This theorem, and its proof, have the following consequences.

First, our approach to compute the 2\mathbb{Z}_{2}–norm introduces new techniques that extend the tool kits from [9, 10, 11] and is also applicable to the computation of the Thurston norm of Dehn fillings.

Second, the construction of the minimal triangulations generalises. We do not provide full details, and simply list a further family of triangulations that we conjecture to be minimal in Section 7.

Third, it remains an open problem to classify all ideal triangulations of cusped hyperbolic 3–manifolds that achieve the lower bound in Theorem 1, and to provide a complete list of all underlying cusped hyperbolic 3–manifolds. In contrast, an analogous bound for the complexity of closed 3–manifolds and a complete characterisation of all tight examples are given in [9].

Acknowledgements. Research of the authors is supported in part under the Australian Research Council’s Discovery funding scheme (project number DP190102259).

2 The new infinite family

The first member, 𝒯3,3\mathcal{T}_{3,3}, of the infinite family 𝒯k,n\mathcal{T}_{k,n} was found by experimentation. Of the 9 5969\,596 minimal triangulations of 4 8154\,815 cusped hyperbolic 33–manifolds contained in the orientable cusped hyperbolic census (shipped, for instance, with Regina [3]), there are exactly nine manifolds for which the lower bound in Theorem 1 is attained. Eight of these are monodromy ideal triangulations of once-punctured torus bundles, but the remaining one, a triangulation of manifold s781, is not.

One can check that this minimal ideal triangulation 𝒯3,3\mathcal{T}_{3,3} of s781 achieves the lower bound as follows. It has isomorphism signature gLLMQbeefffehhqxhqq and six ideal tetrahedra. The underlying hyperbolic manifold M3,3M_{3,3} has one cusp and H1(M3,3,)24.H_{1}(M_{3,3},\mathbb{Z})\cong\mathbb{Z}\oplus\mathbb{Z}_{2}\oplus\mathbb{Z}_{4}. The space of all closed normal surfaces has 11 embedded fundamental surfaces consisting of one vertex linking torus, seven orientable surfaces of Euler characteristic at most 2-2 and three non-orientable surfaces of Euler characteristic equal to 2.-2. The non-orientable surfaces represent distinct non-trivial classes in H2(M3,3,2).H_{2}(M_{3,3},\mathbb{Z}_{2}). Since each even torsion class has a taut representative that is isotopic to a normal surface, and all non-trivial fundamental normal surfaces in 𝒯3,3\mathcal{T}_{3,3} have Euler characteristic 2\leq-2, it follows that 𝒯3,3\mathcal{T}_{3,3} attains the lower bound in Theorem 1.

We now briefly describe how this example is extended to the infinite family of triangulations 𝒯k,n\mathcal{T}_{k,n}, k,n3k,n\geq 3 odd.

The ideal triangulation 𝒯k,n\mathcal{T}_{k,n} is build from a kk–tetrahedron solid torus TkT_{k} and an nn–tetrahedron solid torus TnT_{n}, k,n3k,n\geq 3 odd, each with two punctures on the boundary, by identifying the eight boundary triangles (four per solid torus) in pairs. The identification space Mk,nM_{k,n} has the required torsion classes in homology, namely H1(Mk,n,)2k+1H_{1}(M_{k,n},\mathbb{Z})\cong\mathbb{Z}\oplus\mathbb{Z}_{2}\oplus\mathbb{Z}_{k+1} (note that H1(Mk,n,)H_{1}(M_{k,n},\mathbb{Z}) does not depend on nn). Hence we have H2(Mk,n,2)22H_{2}(M_{k,n},\mathbb{Z}_{2})\cong\mathbb{Z}_{2}\oplus\mathbb{Z}_{2}. We remark that we do not consider homology relative to the boundary. The triangulations of the solid tori are described in Section 3, and the triangulations 𝒯k,n\mathcal{T}_{k,n} in Section 4.

Refer to caption

Figure 1: Three component hyperbolic (non-alternating) link 8938^{3}_{9} (Alexander-Briggs (Rolfsen) Number [17, Appendix C]), L8a16 (Thistlethwaite Number [2]). Picture from [2].

In order to apply Theorem 1, we need to show that each Mk,nM_{k,n} is hyperbolic, i.e. has a complete hyperbolic structure of finite volume. To this end, we show in Section 5 that the manifolds Mk,nM_{k,n} are obtained by Dehn surgery on the link 8938^{3}_{9} and determine the surgery coefficients. The complement of the three component link 8938^{3}_{9}, shown in Figure 1, is hyperbolic and admits a symmetry which fixes one of the cusps and interchanges the other two. We refer to the former as the symmetric cusp, and it is shown in red in Figure 1. The manifolds Mk,nM_{k,n} are all obtained from the complement of 8938^{3}_{9} by filling two of its cusps, where one of these must be the symmetric cusp. An application of Lackenby’s combinatorial word hyperbolic Dehn surgery theorem [14, Theorem 4.9] shows that Mk,nM_{k,n} is hyperbolic for all k,n17.k,n\geq 17. A computation with Regina [3] extends this to all k,n3.k,n\geq 3.

We next determine the norm of the non-trivial classes in H2(Mk,n,2).H_{2}(M_{k,n},\mathbb{Z}_{2}). This is achieved in Section 6 by using a different triangulation of Mk,nM_{k,n}, namely a triangulation 𝒯k,n\mathcal{T}^{\prime}_{k,n} that uses the description of Mk,nM_{k,n} as Dehn surgery on the link 893.8^{3}_{9}. This allows us to analyse the space of all normal surfaces representing the homology classes. Namely, it reduces the argument to a calculation of all normal surfaces with a specific boundary pattern in the link complement, together with an analysis of how these surfaces extend to the surgery tori.

This completes the outline of the proof of Theorem 2. Below is a quick guide to the notation used for the various triangulations in this paper:

𝒯ideal triangulation of the complement of the link 893 in 𝕊3\displaystyle\mathcal{T}\;\;\;\;\text{ideal triangulation of the complement of the link }8^{3}_{9}\text{ in }\mathbb{S}^{3}
𝒯triangulation of the exterior of the link 893 in 𝕊3 with one boundary component removed\displaystyle\mathcal{T}^{\prime}\;\;\;\text{triangulation of the exterior of the link }8^{3}_{9}\text{ in }\mathbb{S}^{3}\text{ with one boundary component removed}
Mk,nManifold(’8^3_9’)(,(n+1,1),(k+1,1))\displaystyle M_{k,n}\cong\text{Manifold('8\^{}3\_9')}(\;\infty\;,(n+1,-1),(k+1,1))
𝒯k,n=TkTn ideal triangulation of Mk,n\displaystyle\mathcal{T}_{k,n}=T_{k}\cup T_{n}\text{ ideal triangulation of }M_{k,n}
𝒯k,n=𝒯LST(1,m)LST(1,k1) triangulation of Mk,n with one ideal and two material vertices\displaystyle\mathcal{T}^{\prime}_{k,n}=\mathcal{T}^{\prime}\cup\operatorname{LST}(1,m)\cup\operatorname{LST}(1,k-1)\text{ triangulation of }M_{k,n}\text{ with one ideal and two material vertices }

3 An infinite family of solid tori

The construction of our infinite families of minimal triangulations of once-cusped hyperbolic manifolds is based on a family of solid torus triangulations TmT_{m}. Start with a 2–triangle standard triangulation of the annulus. The two boundary curves of the annulus are edges in this triangulation, and each of the remaining three edges is incident with both boundary edges. One now iteratively layers tetrahedra on one side of this annulus, such that the initial triangulation of the annulus is in the boundary of the solid torus, and each interior edge has degree four. This completely characterises these triangulations combinatorially. In what follows, we mainly introduce notation to make this explicit and we highlight some features that will be relevant later.

Let m1m\geq 1 and Δ1,,Δm\Delta_{1},\dots,\Delta_{m} be a collection of Euclidean 3–simplices. The vertices of each Δj\Delta_{j} are labelled 0,1,2,30,1,2,3, and for each subset Λ{0,1,2,3},\Lambda\subseteq\{0,1,2,3\}, Δj(Λ)\Delta_{j}(\Lambda) is the subsimplex spanned by Λ.\Lambda. The triangulation T1T_{1} is obtained by making the edge identification Δ1(03)=Δ1(12).\Delta_{1}(03)=\Delta_{1}(12). For m>1,m>1, TmT_{m} is obtained from Tm1T_{m-1} by adding Δm\Delta_{m} via the face pairings:

Δm(102)Δm1(013),\displaystyle\Delta_{m}(102)\,\,\mapsto\,\,\Delta_{m-1}(013),
Δm(023)Δm1(023),if m is even,\displaystyle\Delta_{m}(023)\,\,\mapsto\,\,\Delta_{m-1}(023),\;\text{if $m$ is even},
Δm(123)Δm1(123),if m is odd.\displaystyle\Delta_{m}(123)\,\,\mapsto\,\,\Delta_{m-1}(123),\;\text{if $m$ is odd}.

If mm is even, this is a layering of Δm\Delta_{m} on the edge Δm1(03)\Delta_{m-1}(03); and if mm is odd, this is a layering of Δm\Delta_{m} on the edge Δm1(13).\Delta_{m-1}(13).

It follows from the construction that the faces Δ1(012)\Delta_{1}(012) and Δ1(023)\Delta_{1}(023) form an annulus in the boundary of TmT_{m}, and that for m>1,m>1, TmT_{m} is a solid torus obtained from Tm1T_{m-1} by layering a tetrahedron on an edge not contained in the boundary faces Δ1(012)\Delta_{1}(012) and Δ1(023)\Delta_{1}(023). The different pairings for mm odd or even ensure that each interior edge of TmT_{m} has degree four.

The two boundary edges of TmT_{m} corresponding to a longitude of the solid torus are Δ1(01)==Δm(01)\Delta_{1}(01)=\ldots=\Delta_{m}(01) and Δ1(23)==Δm(23)\Delta_{1}(23)=\ldots=\Delta_{m}(23). We denote Δ1(01)==Δm(01)\Delta_{1}(01)=\ldots=\Delta_{m}(01) by λ\lambda, see Figure 2.

We note that TmT_{m} has two vertices Δ1(0)=Δ1(1)==Δm(0)=Δm(1)\Delta_{1}(0)=\Delta_{1}(1)=\ldots=\Delta_{m}(0)=\Delta_{m}(1) and Δ1(2)=Δ1(3)==Δm(2)=Δm(3)\Delta_{1}(2)=\Delta_{1}(3)=\ldots=\Delta_{m}(2)=\Delta_{m}(3).

The boundary of the solid torus TmT_{m} is a 4–triangle, 2–vertex torus. For mm odd this results in boundary faces Δm(013),\Delta_{m}(013), Δm(123),\Delta_{m}(123), Δ1(012),\Delta_{1}(012), and Δ1(023),\Delta_{1}(023), see also Figure 2.

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Refer to caption
Figure 2: Construction of TmT_{m}, longitude, meridian, and meridian disc. Top: the base annulus. Second, third, and fourth row: T1T_{1}, T2T_{2}, and T3T_{3} respectively. In each step, another tetrahedron is layered onto the existing triangulation. Right column: the normal pieces of the corresponding meridian disc.

In order to determine the meridian μ\mu of TmT_{m} we trace the meridian disc of TmT_{m} through the layerings:

  • In the 2–triangle annulus the seed of the meridian disc is a horizontal arc connecting the two boundary components (Figure 2 top row).

  • Layering Δ1\Delta_{1} to the annulus adds a single horizontal quad of type q03/12q_{03/12} in Δ1\Delta_{1} to the seed of the meridian disc (Figure 2, second row).

  • Layering Δ2\Delta_{2} on edge Δ1(03)=Δ1(12)\Delta_{1}(03)=\Delta_{1}(12) adds two normal triangles in Δ2\Delta_{2} (one of type t0t_{0} and one of type t3t_{3}) to the meridian disc (Figure 2, third row).

  • Layering Δ3\Delta_{3} on edge Δ2(02)=Δ2(13)\Delta_{2}(02)=\Delta_{2}(13), adds two normal triangles (of types t1t_{1} and t3t_{3} respectively) and one normal quadrilateral (of type q01/23q_{01/23}) in Δ3\Delta_{3} to the meridian disc (Figure 2, bottom row).

  • Layering Δj\Delta_{j}, j4j\geq 4, adds two more normal triangles (of types as before) and m2m-2 normal quadrilaterals of type q01/23q_{01/23} to the meridian disc. See Figure 3 for the meridian disc in TmT_{m} and its boundary curve.

Refer to caption

Figure 3: Left: boundary of TmT_{m} with longitude and meridian. Right: meridian disc of TmT_{m} as a normal surface.

The triangulation TmT_{m} admits three normal surfaces F1F_{1}, F2F_{2}, and F3F_{3} with exactly one normal quadrilateral per tetrahedron and every normal quadrilateral type features in exactly one of these three surfaces:

  • Starting with quadrilateral q01/23q_{01/23} in Δ1\Delta_{1} we obtain a separating annulus F1F_{1} intersecting the boundary of TmT_{m}, m2m\geq 2 arbitrary, in two longitudes, denoted by γ1\gamma_{1}.

  • Starting with quadrilateral q02/13q_{02/13} in Δ1\Delta_{1} we obtain a one-sided (non-orientable) surface F2F_{2} intersecting the boundary of TmT_{m}, k3k\geq 3 and odd, horizontally in curve γ2\gamma_{2}.

  • Starting with quadrilateral q03/12q_{03/12} in Δ1\Delta_{1} we obtain another one-sided (non-orientable) surface F3F_{3} intersecting the boundary of TmT_{m}, m3m\geq 3 and odd, diagonally in curve γ3\gamma_{3}.

See Figure 4 for an illustration.

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Figure 4: Boundary patterns of normal surfaces F1F_{1}, F2F_{2}, and F3F_{3} in TmT_{m}. The boundary pattern of F1F_{1} does not depend on mm, whereas the boundary patterns of F2F_{2} and F3F_{3} depend on the parity of mm.

Due to the following result, we know when and how a curve on the boundary of a solid torus extends to a one-sided incompressible properly embedded (connected) surface in its interior.

Proposition 3 (Corollary 2.2 in [5]).

Suppose TT is a solid torus, μ\mu a standard meridian and λ\lambda a longitude for T.T. A one-sided connected incompressible surface STS\subset T has boundary a single curve homotopic with 2pλ+qμ2p\lambda+q\mu, for some p,qp,q\in\mathbb{Z} satisfying p0p\neq 0, 2p2p and qq co-prime. Conversely, every simple closed curve on T\partial T homotopic with 2pλ+qμ2p\lambda+q\mu, where p0p\neq 0, 2p2p and qq co-prime, is the boundary of a one-sided incompressible surface in TT.

Moreover, the negative Euler characteristic of SS is determined by [S]=2pλ+qμ[\partial S]=2p\lambda+q\mu and given by the number N(2p,q)N(2p,q) defined by N(2p,q)=N(2(pQ),q2m)+1N(2p,q)=N(2(p-Q),q-2m)+1, where QQ is the smallest positive integer so that there exists an integer mm such that Qq=2pm±1Qq=2pm\pm 1 and N(2p,1)=p1N(2p,1)=p-1.

Corollary 4.

Let m3m\geq 3 be odd. The surface F2F_{2} with boundary γ2\gamma_{2} is an incompressible one-sided surface with negative Euler characteristic (m1)/2(m-1)/2 properly embedded in TmT_{m}, and the surface F3F_{3} with boundary γ3\gamma_{3} is an incompressible one-sided surface with negative Euler characteristic (m3)/2(m-3)/2 properly embedded in Tm.T_{m}.

Proof.

We have

γiγi,μλ+γi,λμ.\gamma_{i}\ \simeq\ \langle\gamma_{i},\mu\rangle\lambda+\langle\gamma_{i},\lambda\rangle\mu.

As can be deduced from Figure 4, this results in γ2=(m+1)λ+μ\gamma_{2}=(m+1)\lambda+\mu and γ3=(m1)λ+μ\gamma_{3}=(m-1)\lambda+\mu.

Proposition 3 applied to γ2\gamma_{2} and γ3\gamma_{3} shows that these curves bound incompressible surfaces of negative Euler characteristic (m1)/2(m-1)/2 and (m3)/2(m-3)/2 respectively. Now F2F_{2} and F3F_{3} have precisely this negative Euler characteristic. Hence they must be incompressible. ∎

4 The family of triangulations

Suppose k,n3k,n\geq 3 odd. Let T1=Tk1=TkT^{1}=T_{k}^{1}=T_{k} and T2=Tn2=TnT^{2}=T_{n}^{2}=T_{n} be triangulations of the solid torus from Section 3. Denote their tetrahedra by Δji,\Delta^{i}_{j}, i=1,2.i=1,2. Glue the boundary of T1T^{1} to the boundary of T2T^{2} in the following way:

Δ11(012)Δ12(120);Δk1(013)1Δ12(032);Δ11(023)Δn2(321);Δk1(123)Δn2(130).\Delta^{1}_{1}(012)\mapsto\Delta^{2}_{1}(120);\,\ \Delta^{1}_{k}(013)_{1}\mapsto\Delta^{2}_{1}(032);\,\ \Delta^{1}_{1}(023)\mapsto\Delta^{2}_{n}(321);\,\ \Delta^{1}_{k}(123)\mapsto\Delta^{2}_{n}(130). (4.1)

We denote the set the face pairings in (4.1) by Φ.\Phi.

This identifies all vertices from both boundary tori, and the link of this single vertex is a torus. The identification space of the resulting triangulation 𝒯k,n\mathcal{T}_{k,n} is an orientable pseudo-manifold having the single vertex as the only non-manifold point, and the complement of the vertex is denoted Mk,n.M_{k,n}. See Figure 10 for the two torus boundaries of T1T^{1} and T2T^{2}.

We refer to the image of the boundaries of T1T^{1} and T2T^{2} in 𝒯k,n\mathcal{T}_{k,n} as the gluing interface, see Figure 6 for a drawing of the associated abstract 22-complex. As observed, this has four triangles, one vertex, and we claim that there are four edges. For the twenty edges involved in the identifications on the boundaries of the tori, we have identifications Δ11(01)=Δk1(01)\Delta_{1}^{1}(01)=\Delta_{k}^{1}(01), Δ11(23)=Δk1(23)\Delta_{1}^{1}(23)=\Delta_{k}^{1}(23), Δ11(03)=Δ11(12)\Delta_{1}^{1}(03)=\Delta_{1}^{1}(12) and Δk1(03)=Δk1(12)\Delta_{k}^{1}(03)=\Delta_{k}^{1}(12) coming from the gluings inside T1T^{1}; and similarly Δ12(01)=Δn2(01)\Delta_{1}^{2}(01)=\Delta_{n}^{2}(01), Δ12(23)=Δn2(23)\Delta_{1}^{2}(23)=\Delta_{n}^{2}(23), Δ12(03)=Δ12(12)\Delta_{1}^{2}(03)=\Delta_{1}^{2}(12) and Δn2(03)=Δn2(12)\Delta_{n}^{2}(03)=\Delta_{n}^{2}(12) coming from the gluings inside T2T^{2}. Combining this with the identifications of the boundaries yields four edge classes in the gluing interface:

e1=\displaystyle e_{1}= Δ11(01)=Δk1(01)=Δ12(03)=Δ12(12),\displaystyle\Delta_{1}^{1}(01)=\Delta_{k}^{1}(01)=\Delta_{1}^{2}(03)=\Delta_{1}^{2}(12),
e2=\displaystyle e_{2}= Δ11(23)=Δk1(23)=Δn2(30)=Δn2(21),\displaystyle\Delta_{1}^{1}(23)=\Delta_{k}^{1}(23)=\Delta_{n}^{2}(30)=\Delta_{n}^{2}(21),
e3=\displaystyle e_{3}= Δ12(01)=Δn2(01)=Δ12(23)=Δn2(23)=Δ11(20)=Δk1(31),\displaystyle\Delta_{1}^{2}(01)=\Delta_{n}^{2}(01)=\Delta_{1}^{2}(23)=\Delta_{n}^{2}(23)=\Delta_{1}^{1}(20)=\Delta_{k}^{1}(31),
e4=\displaystyle e_{4}= Δ11(03)=Δ11(12)=Δk1(30)=Δk1(21)=Δ12(20)=Δn2(31).\displaystyle\Delta_{1}^{1}(03)=\Delta_{1}^{1}(12)=\Delta_{k}^{1}(30)=\Delta_{k}^{1}(21)=\Delta_{1}^{2}(20)=\Delta_{n}^{2}(31).

Denote the quadrilateral normal surfaces in the solid tori TiT^{i} described in Section 3 by FjiF^{i}_{j}, i=1,2i=1,2, j=1,2,3j=1,2,3. Their edge weights (w(e1),w(e2),w(e3),w(e4))(w(e_{1}),w(e_{2}),w(e_{3}),w(e_{4})) in Ti\partial T^{i}, i=1,2i=1,2 are

  • (1,1,0,1)(1,1,0,1) for F21F_{2}^{1} and F12F_{1}^{2};

  • (0,0,1,1)(0,0,1,1) for F11F_{1}^{1} and F32F_{3}^{2};

  • (1,1,1,0)(1,1,1,0) for F31F_{3}^{1} and F22F_{2}^{2}.

It follows that 𝒯k,n\mathcal{T}_{k,n} admits three normal surfaces 𝒮1=F21F12\mathcal{S}_{1}=F_{2}^{1}\cup F_{1}^{2}, 𝒮2=F11F32\mathcal{S}_{2}=F_{1}^{1}\cup F_{3}^{2}, and 𝒮3=F31F22\mathcal{S}_{3}=F_{3}^{1}\cup F_{2}^{2}, each consisting of a single quadrilateral per tetrahedron such that every normal quadrilateral type of 𝒯k,n\mathcal{T}_{k,n} occurs in exactly one of these surfaces.

Their respective Euler characteristics can be computed from Proposition 3. For this, note that the boundary curves of the surfaces FjiF^{i}_{j} inside TiT^{i}, i=1,2i=1,2, j=1,2,3j=1,2,3, are made up of four normal arcs and four midpoints of edges.

In 𝒯k,n\mathcal{T}_{k,n}, the surfaces 𝒮j\mathcal{S}_{j}, j=1,2,3j=1,2,3, still meet the gluing interface T1T2T^{1}\cap T^{2} in four normal arcs, but only three (resp. two) midpoints of edges for 𝒮3\mathcal{S}_{3} and 𝒮1\mathcal{S}_{1} (resp. 𝒮2\mathcal{S}_{2}). This can be seen by looking at their edge weights for the four edges in the gluing interface.

Thus, the Euler characteristic of each surface pieces is the value given in Proposition 3 minus 11 (resp. minus 22). Altogether we have

χ(𝒮1)\displaystyle\chi(\mathcal{S}_{1})\ =(χ(F21)1)+(χ(F12)1)+1\displaystyle=(\chi(F_{2}^{1})-1)+(\chi(F_{1}^{2})-1)+1 =k12+01\displaystyle=-\frac{k-1}{2}+0-1 =k+12\displaystyle=-\frac{k+1}{2} (4.2)
χ(𝒮2)\displaystyle\chi(\mathcal{S}_{2})\ =(χ(F11)2)+(χ(F32)2)+2\displaystyle=(\chi(F_{1}^{1})-2)+(\chi(F_{3}^{2})-2)+2 =0n322\displaystyle=0-\frac{n-3}{2}-2 =n+12\displaystyle=-\frac{n+1}{2} (4.3)
χ(𝒮3)\displaystyle\chi(\mathcal{S}_{3})\ =(χ(F31)1)+(χ(F22)1)+1\displaystyle=(\chi(F_{3}^{1})-1)+(\chi(F_{2}^{2})-1)+1 =k32n121\displaystyle=-\frac{k-3}{2}-\frac{n-1}{2}-1 =k+n22\displaystyle=-\frac{k+n-2}{2} (4.4)

Each of the 𝒮j\mathcal{S}_{j}, j=1,2,3j=1,2,3 is the canonical representative of one of the non-zero 2\mathbb{Z}_{2}–homology classes and we have

χ(𝒮1)+χ(𝒮2)+χ(𝒮3)=(k+n).\chi(\mathcal{S}_{1})+\chi(\mathcal{S}_{2})+\chi(\mathcal{S}_{3})=-(k+n).

In order to apply Theorem 1 to conclude that 𝒯k,n\mathcal{T}_{k,n} is minimal, we need to show that each Mk,nM_{k,n} is hyperbolic (see Section 5) and that each 𝒮j\mathcal{S}_{j} is taut (see Section 6).

5 Hyperbolicity and algebraic topology of Mk,nM_{k,n}

We start by building a 3–cusped manifold using a variant of the construction of 𝒯k,n\mathcal{T}_{k,n} described above. For this, take a cone C^1\widehat{C}^{1} over T1\partial T^{1} and a cone C^2\widehat{C}^{2} over T2\partial T^{2}, where T1=Tk1T^{1}=T_{k}^{1} and T2=Tn2T^{2}=T_{n}^{2} are the solid torus triangulations from Section 4 and k,n3k,n\geq 3 both odd. Now we glue them together using the same face pairings Φ\Phi from (4.1) to obtain a triangulation 𝒯\mathcal{T} with eight tetrahedra of a pseudo-manifold N^\widehat{N} with three vertices having torus links. This is defined by the gluing table given in Table 1 and shown in Figure 5.

Using Regina [3] we can check that the complement N=N^N^(0)N=\widehat{N}\setminus\widehat{N}^{(0)} of the three vertices in N^\widehat{N} is a 3–manifold homeomorphic to the complement of the link 8938^{3}_{9}, and that this is a minimal triangulation of N.N. We refer to C1=C^1N^(0)C^{1}=\widehat{C}^{1}\setminus\widehat{N}^{(0)} and C2=C^2N^(0)C^{2}=\widehat{C}^{2}\setminus\widehat{N}^{(0)} respectively as the (red) cusp 1 and the (blue) cusp 2 of N.N. The red cusp is the symmetric cusp of the link complement, and the blue cusp therefore one of the non-symmetric cusps.

Refer to caption

Figure 5: The ideal triangulation of NN, the complement of the link 8938^{3}_{9}.

Refer to caption

Figure 6: The interface viewed from red and blue cusp
Tet (012)(012) (013)(013) (023)(023) (123)(123)
0 2(013)2(013) 𝟕(𝟎𝟐𝟑){\bf 7(023)} 1(102)1(102) 1(103)1(103)
11 0(203)0(203) 0(213)0(213) 3(123)3(123) 𝟒(𝟏𝟐𝟎){\bf 4(120)}
22 𝟔(𝟏𝟑𝟎){\bf 6(130)} 0(012)0(012) 3(021)3(021) 3(031)3(031)
33 2(032)2(032) 2(132)2(132) 𝟓(𝟐𝟑𝟏){\bf 5(231)} 1(023)1(023)
44 𝟏(𝟑𝟏𝟐){\bf 1(312)} 6(012)6(012) 5(130)5(130) 5(120)5(120)
55 4(312)4(312) 4(302)4(302) 7(123)7(123) 𝟑(𝟑𝟎𝟐){\bf 3(302)}
66 4(013)4(013) 𝟐(𝟐𝟎𝟏){\bf 2(201)} 7(013)7(013) 7(012)7(012)
77 6(123)6(123) 6(023)6(023) 𝟎(𝟎𝟏𝟑){\bf 0(013)} 5(023)5(023)
Table 1: Gluing table for 33-cusped manifold NN, an ideal triangulation homeomorphic to the complement of 8938^{3}_{9}. Bold entries are gluings across the interface, all simplices are coherently oriented.

It follows from the construction that the interface between the red and blue cusps in NN is identical to the interface between the solid tori in Mk,n.M_{k,n}. It is shown in Figure 6. We now truncate the red and blue cusps along vertex linking surfaces. These surfaces are naturally combinatorially isomorphic with T1\partial T^{1} and T2\partial T^{2}. The cusps are then filled with the solid tori Tk1T^{1}_{k} and Tn2T^{2}_{n} respectively, such that the gluing agrees with the natural combinatorial isomorphism (see Figure 7). With respect to the framing indicated in the figure, this results in the manifold

Nk,n=N(,(k,1),(n+1,1)).N_{k,n}=N(\;\infty\;,(-k,1),(n+1,1)).

For the interested reader who wishes to use SnapPy to study these manifolds, we remark that

Nk,n=Manifold(’8^3_9’)(,(n+1,1),(k+1,1)).N_{k,n}=\text{Manifold('8\^{}3\_9')}(\;\infty\;,(n+1,-1),(k+1,1)). (5.1)

The Euclidean equilateral triangles shown in Figure 7 in fact give the Euclidean structures (up to scale) on the cusp cross sections with respect to the complete hyperbolic structure on N.N. Here, each ideal tetrahedron has shape ii and each triangle therefore angles π2,π4,π4\frac{\pi}{2},\frac{\pi}{4},\frac{\pi}{4}. The framing used in this paper is thus the natural geometric framing of the cusps.

Refer to caption

Figure 7: Fillings of cusps of MM; indicated are the peripheral curves on the vertex links and the meridian curves on the solid tori.

Casson observed that if an ideal triangulation admits an angle structure, then the manifold must admit a complete hyperbolic metric of finite volume (see [16, Theorem 10.2]). Using this, computation with Regina [3] confirms that Nk,nN_{k,n} is hyperbolic for all 17k,n3.17\geq k,n\geq 3. The same result could also be obtained with SnapPy [4].

To show that Nk,nN_{k,n} also has a complete hyperbolic metric of finite volume for all k,n17,k,n\geq 17, we note that due to Thurston’s hyperbolisation theorem for Haken manifolds [18, 15, 13], it suffices to show that Nk,nN_{k,n} is irreducible, atoroidal, and not Seifert fibred. This conclusion is achieved by an application of Lackenby’s combinatorial version of the Gromov-Thurston 2π2\pi theorem [14, Theorem 4.9] (see also the sentence after its proof for the case when not all cusps are filled). We refer to [14] for the definitions and statements required to understand the next paragraph.

The hypothesis of [14, Theorem 4.9] is achieved by applying [14, Proposition 4.10], which gives a criterion using angle structures. We use the angle structure on NN determined by the complete hyperbolic structure, where each triangle in the vertex link has angles π2,π4,π4\frac{\pi}{2},\frac{\pi}{4},\frac{\pi}{4}. In particular, Lackenby’s combinatorial length of any curve γ\gamma on a vertex link is estimated from below by the shortest simplicial length |γ||\gamma| of a representative of [γ][\gamma] times π8.\frac{\pi}{8}. The theorem thus applies to any set of filling curves γ\gamma with |γ|π8>2π,|\gamma|\frac{\pi}{8}>2\pi, and hence |γ|17.|\gamma|\geq 17. Examination of the vertex links gives the simple bounds |μ1kλ1|k|\mu_{1}^{-k}\lambda_{1}|\geq k and |μ2n+1λ2|n+1|\mu_{2}^{n+1}\lambda_{2}|\geq n+1. Therefore k,n17k,n\geq 17 are sufficient to ensure hyperbolicity.

Next, we observe that by construction the manifold Nk,nN_{k,n} is homotopy equivalent with Mk,n,M_{k,n}, and that we may choose the homotopy to be the identity in a neighbourhood of the single cusp (corresponding to the vertex on the interface). Now take a sufficiently large compact core of each manifold, and double it along its boundary. Then we have two closed Haken 3–manifolds that are homotopy equivalent, and hence homeomorphic by Waldhausen [19]. Since Nk,nN_{k,n} is hyperbolic and homeomorphism preserves the JSJ decomposition, it follows that Nk,nN_{k,n} is homeomorphic with Mk,n.M_{k,n}. In particular, Mk,nM_{k,n} is also hyperbolic.

It is clear from the description of the normal surfaces in the previous section that Mk,n=Nk,nM_{k,n}=N_{k,n} has homology amenable to an application of Theorem 1 ([10, Theorem 1]). This can be verified using a homology computation using the chosen peripheral framings. Using the triangulation, one computes

π1(N)=a,b,cabcbc1a1cb1c1b1,abc1ab1a1bca1b1\pi_{1}(N)=\langle\;a,b,c\;\mid\;abcbc^{-1}a^{-1}cb^{-1}c^{-1}b^{-1},\;abc^{-1}ab^{-1}a^{-1}bca^{-1}b^{-1}\;\rangle

with the two peripheral subgroups of interest to us (in the geometric framing) generated by:

μ1=c1a,λ1=b1a1bc,μ2=a,λ2=bcbc1\mu_{1}=c^{-1}a,\quad\lambda_{1}=b^{-1}a^{-1}bc,\qquad\mu_{2}=a,\quad\lambda_{2}=bcbc^{-1}

This implies:

H1(Mk,n)a,b,c(a1c)k+1,(a(n+1)/2b)22k+1H_{1}(M_{k,n})\cong\langle\;a,b,c\;\mid\;(a^{-1}c)^{k+1},\;(a^{(n+1)/2}b)^{2}\;\rangle\cong\mathbb{Z}\oplus\mathbb{Z}_{2}\oplus\mathbb{Z}_{k+1}

In particular, this highlights the requirement for both nn and kk to be odd.

6 The norm of the homology classes of Mk,nM_{k,n}

In this section we determine the norm of the non-trivial classes in H2(Mk,n,2)H_{2}(M_{k,n},\mathbb{Z}_{2}). We first provide an overview. Our proofs of correctness of the calculation rely on technical results by Jaco and Sedgwick [12] for normal surfaces with boundary on a single 2–triangle torus and Bachman, Derby-Talbot and Sedgwick [1] for normal surfaces with boundary on two 2–triangle tori.

We consider a triangulation 𝒯\mathcal{T}^{\prime} of the 3–manifold obtained by removing open neighbourhoods of the blue and red cusps of the complement of 8938^{3}_{9} (Section 6.1). This has one cusp and two boundary components, 1\partial_{1} (the boundary of the blue cusp) and 2\partial_{2} (the boundary of the red cusp). The interior of the identification space 𝒯¯\overline{\mathcal{T}} of 𝒯\mathcal{T}^{\prime} is homeomorphic to the complement of 893.8^{3}_{9}. Using the natural geometric framing on 1\partial_{1} and 2\partial_{2} and the surgery description of Mk,nM_{k,n}, we determine how to complete 𝒯\mathcal{T}^{\prime} to a triangulation 𝒯k,n\mathcal{T}^{\prime}_{k,n} of Mk,nM_{k,n} by gluing suitable layered solid tori to 1\partial_{1} and 2\partial_{2} (Section 6.5).

Each non-trivial class αH2(Mk,n,2)\alpha\in H_{2}(M_{k,n},\mathbb{Z}_{2}) associates with each edge in 1\partial_{1} and 2\partial_{2} a parity, which we call its boundary pattern (Section 6.2). This boundary pattern encodes the parities of the number of points in the intersection of the edges with a surface that is transverse to the triangulation and represents the class α.\alpha. There is a taut normal surface SS in 𝒯k,n\mathcal{T}^{\prime}_{k,n} that represents the class α\alpha and its intersection with each of 1\partial_{1} and 2\partial_{2} consists of at most one curve, and these curves of intersection are essential ( Section 6.3).

The norm of α\alpha is the maximum Euler characteristic of any normal surface in 𝒯k,n\mathcal{T}^{\prime}_{k,n} representing α.\alpha. The computation of the norm of α\alpha thus splits into a computation of all normal surfaces of 𝒯\mathcal{T}^{\prime} that have the correct boundary pattern (Section 6.3) and determining how these normal surfaces extend into the layered solid tori attached to 𝒯\mathcal{T}^{\prime} along 1\partial_{1} and 2\partial_{2} (Section 6.6). Normal surfaces in these layered solid tori are well-known (Section 6.4). Moreover, the Euler characteristics of the latter surfaces are determined by their boundary slopes via the Bredon-Wood formula (see Proposition 3 or [5, Corollary 2.2]). The conclusion of these computations in Section 6.6 is that:

α1=k+12,α2=n+12,α3=n+k22||\;\alpha_{1}\;||=\frac{k+1}{2},\qquad||\;\alpha_{2}\;||=\frac{n+1}{2},\qquad||\;\alpha_{3}\;||=\frac{n+k-2}{2}

In particular, this confirms that the surfaces 𝒮1,𝒮2\mathcal{S}_{1},\mathcal{S}_{2} and 𝒮3\mathcal{S}_{3} described in Section 4 are taut. We now supply the missing details.

6.1 A triangulation with two boundary components and one ideal vertex

Starting with the ideal 33-cusped triangulation NN of the complement of 8938^{3}_{9}, see Figure 5 and Table 1, we cut along the vertex links of the blue and red vertex respectively to obtain a 1717-tetrahedra triangulation with two boundary components and one ideal vertex. By construction, the interior of the identification space is homeomorphic with the complement of 893.8^{3}_{9}. We denote this triangulation by 𝒯\mathcal{T}^{\prime}. Its isomorphism signature is

rfLLHMzLPMwQcddghghjnklomqopqrwgrrgfxrvqdabxs

and its gluing table is given in Table 2.

Tet (012)(012) (013)(013) (023)(023) (123)(123)
Δ0\Delta_{0} 3(012)3(012) 1\partial_{1} 2(023)2(023) 1(123)1(123)
Δ1\Delta_{1} 5(012)5(012) 3(230)3(230) 4(023)4(023) 0(123)0(123)
Δ2\Delta_{2} 7(012)7(012) 3(321)3(321) 0(023)0(023) 6(123)6(123)
Δ3\Delta_{3} 0(012)0(012) 1\partial_{1} 1(301)1(301) 2(310)2(310)
Δ4\Delta_{4} 8(012)8(012) 7(230)7(230) 1(023)1(023) 6(023)6(023)
Δ5\Delta_{5} 1(012)1(012) 7(103)7(103) 9(023)9(023) 6(310)6(310)
Δ6\Delta_{6} 10(012)10(012) 5(321)5(321) 4(123)4(123) 2(123)2(123)
Δ7\Delta_{7} 2(012)2(012) 5(103)5(103) 4(301)4(301) 11(123)11(123)
Δ8\Delta_{8} 4(012)4(012) 13(013)13(013) 9(021)9(021) 12(123)12(123)
Δ9\Delta_{9} 8(032)8(032) 10(230)10(230) 5(023)5(023) 13(210)13(210)
Δ10\Delta_{10} 6(012)6(012) 14(013)14(013) 9(301)9(301) 11(120)11(120)
Δ11\Delta_{11} 10(312)10(312) 12(021)12(021) 14(201)14(201) 7(123)7(123)
Δ12\Delta_{12} 11(031)11(031) 16(013)16(013) 15(023)15(023) 8(123)8(123)
Δ13\Delta_{13} 9(321)9(321) 8(013)8(013) 14(032)14(032) 16(123)16(123)
Δ14\Delta_{14} 11(230)11(230) 10(013)10(013) 13(032)13(032) 15(210)15(210)
Δ15\Delta_{15} 14(321)14(321) 2\partial_{2} 12(023)12(023) 16(012)16(012)
Δ16\Delta_{16} 15(123)15(123) 12(013)12(013) 2\partial_{2} 13(123)13(123)
Table 2: Gluing table for triangulation 𝒯\mathcal{T}^{\prime} of the complement of 8938^{3}_{9} with two real boundary components and one ideal vertex.

In particular, the two boundary components 1\partial_{1} (bounding a neighbourhood of the blue cusp in Figure 5 – one of the non-symmetric components of 8938^{3}_{9}) and 2\partial_{2} (bounding a neighbourhood of the red cusp in Figure 5 – the symmetric component of 8938^{3}_{9}) are two 11-vertex tori made up of triangles 0(013)0(013) and 3(013)3(013), and 15(013)15(013) and 16(023)16(023) respectively. We have edge classes

e0=\displaystyle e_{0}= Δ3(01)=Δ0(01),\displaystyle\Delta_{3}(01)=\Delta_{0}(01),
e2=\displaystyle e_{2}= Δ0(03)=Δ2(03)=Δ3(31),\displaystyle\Delta_{0}(03)=\Delta_{2}(03)=\Delta_{3}(31),
e4=\displaystyle e_{4}= Δ3(30)=Δ1(13)=Δ0(13)\displaystyle\Delta_{3}(30)=\Delta_{1}(13)=\Delta_{0}(13)

for 1\partial_{1} and

e18=\displaystyle e_{18}= Δ16(03)=Δ12(03)=Δ15(03),\displaystyle\Delta_{16}(03)=\Delta_{12}(03)=\Delta_{15}(03),
e19=\displaystyle e_{19}= Δ15(01)=Δ14(32)=Δ13(23)=Δ16(23),\displaystyle\Delta_{15}(01)=\Delta_{14}(32)=\Delta_{13}(23)=\Delta_{16}(23),
e20=\displaystyle e_{20}= Δ16(02)=Δ15(13)\displaystyle\Delta_{16}(02)=\Delta_{15}(13)

for 2\partial_{2}.

6.2 Boundary patterns

By construction, a triangulation 𝒯k,n\mathcal{T}^{\prime}_{k,n} of Mk,nM_{k,n} can be obtained from 𝒯\mathcal{T}^{\prime} by gluing two suitable layered solid tori to 1\partial_{1} and 2\partial_{2}. Let α1,α2,α3H2(Mk,n,2)\alpha_{1},\alpha_{2},\alpha_{3}\in H_{2}(M_{k,n},\mathbb{Z}_{2}) be the three non-zero 2\mathbb{Z}_{2}– homology classes corresponding to normal surfaces 𝒮1\mathcal{S}_{1}, 𝒮2\mathcal{S}_{2}, and 𝒮3\mathcal{S}_{3} in 𝒯k,n\mathcal{T}_{k,n} (see Section 4).

The fundamental group of the complement of 8938^{3}_{9} is generated by three meridians. We choose the base point for the fundamental group of 𝒯¯\overline{\mathcal{T}} at the vertex of 1.\partial_{1}. Since 2\mathbb{Z}_{2} is abelian, a homomorphism π1(𝒯¯)2\pi_{1}(\overline{\mathcal{T}})\to\mathbb{Z}_{2} uniquely associates labels in 2\mathbb{Z}_{2} to the edges of 1\partial_{1} and 2.\partial_{2}. Via the inclusion 𝒯¯𝒯k,n¯\overline{\mathcal{T}}\subset\overline{\mathcal{T}^{\prime}_{k,n}}, a class in H2(Mk,n,2)H_{2}(M_{k,n},\mathbb{Z}_{2}) determines a homomorphism π1(𝒯¯)2\pi_{1}(\overline{\mathcal{T}})\to\mathbb{Z}_{2} mapping the meridian of the cusp of 𝒯¯\overline{\mathcal{T}} to zero.

Conversely, any homomorphism π1(𝒯¯)2\pi_{1}(\overline{\mathcal{T}})\to\mathbb{Z}_{2} mapping the meridian of the cusp of 𝒯¯\overline{\mathcal{T}} to zero uniquely determines a class in H2(Mk,n,2)H_{2}(M_{k,n},\mathbb{Z}_{2}) due to the surgery description.

Hence each αi\alpha_{i} associates labels in 2\mathbb{Z}_{2} to the edges in 1\partial_{1} and 2\partial_{2} (and in turn is uniquely determined by these). We call these labels the boundary pattern of αi.\alpha_{i}.

6.3 The normal surfaces of 𝒯\mathcal{T}^{\prime}

Let UiMk,nU_{i}\subset M_{k,n}, [Ui]=αi[U_{i}]=\alpha_{i}, i=1,2,3i=1,2,3 be a taut representative of αi\alpha_{i} in Mk,nM_{k,n}. Since UiU_{i} is incompressible and Mk,nM_{k,n} is irreducible, UiU_{i} is isotopic to a normal surface. Hence we may assume that UiU_{i} is normal. We further assume that amongst all taut normal surfaces representing αi\alpha_{i}, UiU_{i} minimises the total edge weight on 1\partial_{1} and 2.\partial_{2}.

We claim that this implies that U1U_{1} meets 1\partial_{1} in one essential curve and is disjoint from 2\partial_{2}; U2U_{2} meets 2\partial_{2} in one essential curve and is disjoint from 1\partial_{1}; and U3U_{3} meets both 1\partial_{1} and 2\partial_{2} in one essential curve. Indeed, if there are trivial curves in the intersection with 1\partial_{1} or 2\partial_{2}, then one may perform isotopies across balls to reduce the total weight on 1\partial_{1} and 2.\partial_{2}. The resulting surface may not be normal, but normalises to a normal surface that is still taut and has smaller total edge weight on 1\partial_{1} and 2\partial_{2} than the initial surface. Similarly, if there are two parallel essential curves in the intersection with 1\partial_{1} or 2\partial_{2}, then one may perform an annular compression reducing the total edge weight on 1\partial_{1} and 2.\partial_{2}. The resulting surface has the same Euler characteristics, and hence still has a taut component that therefore normalises to a normal surfaces of smaller total weight on 1\partial_{1} and 2\partial_{2} than the initial surface. It follows that there is at most one essential curve in the intersection with each 1\partial_{1} and 2,\partial_{2}, and the claimed numbers now follow from the boundary pattern.

Let Si=Ui𝒯S_{i}=U_{i}\cap\mathcal{T}^{\prime}. We now show that we may assume that S1S_{1} and S2S_{2} are fundamental surfaces in 𝒯.\mathcal{T}.

Since S1S_{1} and S2S_{2} have one essential curve on a 11–vertex torus boundary component, it follows from [12, Proposition 3.7], that there exists a fundamental normal surface with the same boundary curve and with equal or larger Euler characteristic. Using Regina [3] we find that 𝒯\mathcal{T}^{\prime} has 900900 fundamental surfaces in standard coordinates.

First, note that neither 𝒯\mathcal{T}^{\prime} nor the filling tori contain closed normal surfaces of positive Euler characteristic. Hence, to find the norm of α1\alpha_{1} (resp. α2\alpha_{2}) it is sufficient to take the minimum over all fundamental normal surfaces FF in 𝒯\mathcal{T}^{\prime} with boundary a single essential curve in 1\partial_{1} (resp. 2\partial_{2}) of the sum of

  1. (a)

    the negative Euler characteristic of FF, and

  2. (b)

    the negative Euler characteristic of the incompressible surface FF^{\prime} in the filling torus with F=F\partial F^{\prime}=\partial F.

There are only a few candidate surfaces FF to consider.

There are 1010 fundamental surfaces matching the boundary pattern of α1\alpha_{1} and having intersection with 1\partial_{1} one essential curve and empty intersection with 2.\partial_{2}. There are two distinct boundary curves amongst these surfaces, and it suffices to pick a fundamental surface of maximal Euler characteristic for each of these curves.

Refer to caption

Figure 8: Boundary curves and Euler characteristics of candidate surfaces for S1S_{1}.

Similarly, there are 2525 fundamental surfaces matching the boundary pattern of α2\alpha_{2} and having intersection with 2\partial_{2} one essential curve and empty intersection with 1.\partial_{1}. There are three distinct boundary curves amongst these surfaces, and it suffices to pick a fundamental surface of maximal Euler characteristic for each of these curves; see Figure 9.

Refer to caption

Figure 9: Boundary curves and Euler characteristics of candidate surfaces for S2S_{2}.

The second term is determined by F=F\partial F^{\prime}=\partial F via the framing and the Bredon-Wood formula, see Proposition 3 or [5, Corollary 2.2]. However, we take an equivalent approach by analysing the space of all normal surfaces of the layered solid torus realising the filling of the respective cusp.

We show in Section 6.6 that this forces

α1=k+12andα2=n+12||\;\alpha_{1}\;||=\frac{k+1}{2}\qquad\text{and}\qquad||\;\alpha_{2}\;||=\frac{n+1}{2}

We use these norms to determine the norm of α3.\alpha_{3}. The surface S3S_{3} has one essential boundary curve in each of 1\partial_{1} and 2\partial_{2}. Since S3jS_{3}\cap\partial_{j} is a single essential curve, its Haken summands cannot have any trivial boundary components. First suppose a Haken sum of fundamental surfaces in 𝒯\mathcal{T}^{\prime} giving S3S_{3} contains a surface that is disjoint from one of 1\partial_{1} or 2\partial_{2}. It then follows from [1, Lemma 2.10] that there must be exactly one summand H1H_{1} with H11=S31H_{1}\cap\partial_{1}=S_{3}\cap\partial_{1} and H12=H_{1}\cap\partial_{2}=\emptyset; and exactly one summand H2H_{2} with H22=S32H_{2}\cap\partial_{2}=S_{3}\cap\partial_{2} and H21=.H_{2}\cap\partial_{1}=\emptyset. Since S3S_{3} is the intersection with 𝒯\mathcal{T}^{\prime} of the normal surface U3U_{3} in 𝒯k,n,\mathcal{T}^{\prime}_{k,n}, it follows that each H1H_{1} and H2H_{2} extends to a normal surface V1V_{1} and V2V_{2} respectively in 𝒯k,n\mathcal{T}^{\prime}_{k,n} via a subsurface of U2.U_{2}. The boundary pattern implies that [V1]=α1[V_{1}]=\alpha_{1} and [V2]=α2[V_{2}]=\alpha_{2}, and since U3U_{3} is taut, we have α3α1+α2.||\;\alpha_{3}\;||\geq||\;\alpha_{1}\;||+||\;\alpha_{2}\;||. But we already know from the existence of 𝒮3\mathcal{S}_{3} from Section 4 that

α3n+k22<k+12+n+12=α1+α2||\;\alpha_{3}\;||\leq\frac{n+k-2}{2}<\frac{k+1}{2}+\frac{n+1}{2}=||\;\alpha_{1}\;||+||\;\alpha_{2}\;||

Hence every Haken summand HH with non-empty boundary satisfies H1=S31H\cap\partial_{1}=S_{3}\cap\partial_{1} and H2=S32.H\cap\partial_{2}=S_{3}\cap\partial_{2}. Since there is no closed normal surface with positive Euler characteristic, we may assume that every Haken summand in a Haken sum giving S3S_{3} meets each boundary component of 𝒯\mathcal{T}^{\prime} in non-trivial essential curves.

After sorting out duplicates and non-maximal Euler characteristic examples, there are 77 compatibility classes of normal surfaces in 𝒯\mathcal{T}^{\prime} representing α3.\alpha_{3}. In particular, the first class can be reduced to a single fundamental surface, and each of the remaining six classes can be reduced to Haken sums of two fundamental surfaces, i.e. Haken sums of the form w1H1+w2H2w_{1}H_{1}+w_{2}H_{2}. For all pairs H1,H_{1}, H2H_{2} and their possible Haken sums w1H1+w2H2w_{1}H_{1}+w_{2}H_{2}, we list in Table 3 their edge weights on 1\partial_{1} and 2\partial_{2}, their Euler characteristics, and weights w1w_{1} and w2.w_{2}.

#\# w(e0)w(e_{0}) w(e2)w(e_{2}) w(e4)w(e_{4}) w(e18)w(e_{18}) w(e19)w(e_{19}) w(e20)w(e_{20}) χ\chi weight
11 22 11 11 0 11 11 2-2 11
22 22 0 22 22 11 11 2-2 2k+12k+1
22 11 33 22 22 0 3-3 2l+12l+1
4(k+l+1)4(k+l+1) 2l+12l+1 4k+6l+54k+6l+5 4(k+l+1)4(k+l+1) 2k+4l+32k+4l+3 2k+12k+1 4k6l5-4k-6l-5
33 22 0 22 22 11 11 2-2 2k+12k+1
22 11 11 22 0 22 1-1 2l+12l+1
4(k+l+1)4(k+l+1) 2l+12l+1 4k+2l+34k+2l+3 4(k+l+1)4(k+l+1) 2k+12k+1 2k+4l+32k+4l+3 4k2l3-4k-2l-3
44 0 11 11 0 11 11 1-1 2k+12k+1
22 22 0 22 11 33 2-2 2l2l
4l4l 2k+4l+12k+4l+1 2k+12k+1 4l4l 2k+2l+12k+2l+1 2k+6l+12k+6l+1 2k4l1-2k-4l-1
55 22 11 11 22 0 22 1-1 2k+12k+1
22 22 0 22 11 33 2-2 2l+12l+1
4(k+l+1)4(k+l+1) 2k+4l+32k+4l+3 2k+12k+1 4(k+l+1)4(k+l+1) 2l+12l+1 4k+6l+54k+6l+5 2k4l3-2k-4l-3
66 0 11 11 0 11 11 1-1 2k+12k+1
22 11 33 22 22 0 3-3 2l2l
4l4l 2k+2l+12k+2l+1 2k+6l+12k+6l+1 4l4l 2k+4l+12k+4l+1 2k+12k+1 2k6l1-2k-6l-1
77 0 11 11 0 11 11 1-1 2k+12k+1
22 33 11 22 22 44 3-3 2l2l
4l4l 2k+6l+12k+6l+1 2k+2l+12k+2l+1 4l4l 2k+4l+12k+4l+1 2k+8l+12k+8l+1 2k6l1-2k-6l-1
Table 3: Compatibility classes of candidates for a norm minimiser for α3\alpha_{3}.

6.4 Some basic facts on layered solid tori

Layered solid tori denote a two parameter family LST(j,k)\operatorname{LST}(j,k) of 11-vertex triangulations of the solid torus, see [8] for details. Given LST(j,k)\operatorname{LST}(j,k) (jj and kk co-prime), the boundary of the meridian disk has edge weights jj, kk, and j+kj+k on the three boundary edges.

In this section we are only interested in LST(0,1)\operatorname{LST}(0,1), and the family LST(1,m)\operatorname{LST}(1,m), m2m\geq 2. The layered solid torus LST(0,1)\operatorname{LST}(0,1) has three tetrahedra. One of its edges is parallel to the boundary of its meridian disk (the unique edge with edge weight 0). We call this edge the meridional edge of the layered solid torus. The layered solid torus LST(1,m)\operatorname{LST}(1,m) is obtained inductively from the 11-tetrahedron layered solid torus LST(1,2)\operatorname{LST}(1,2) by layering a tetrahedron on the edge of edge weight mm of LST(1,m1).\operatorname{LST}(1,m-1). In particular, for m2m\geq 2 there is a unique boundary edge with edge weight 11, and we call this the longitudinal edge.

It follows from [8, Theorem 5.3] that the only normal surfaces in LST(1,m)\operatorname{LST}(1,m) with connected, essential boundary are the meridian disk (with edge weights 11, mm, and m+1m+1 in the boundary, case (3) in the theorem), and one-sided incompressible normal surfaces with boundary slope what is called the slope of an even ordered edge in LST(1,m)\operatorname{LST}(1,m) (this is an edge in LST(1,m)\operatorname{LST}(1,m) that represents an even multiple of a generator of the fundamental group of the torus, case (6) in the theorem).

For LST(1,m)\operatorname{LST}(1,m) the slopes of even ordered edges have edge weights 11, m2m-2, and m1m-1 (a Möbius strip), 11, m4m-4, and m3m-3 (a surface of Euler characteristic 1-1), all the way down to 11, 11, and 0 for mm odd (a surface of Euler characteristic 1m2\frac{1-m}{2}) and all the way down to 11, 0, and 11 for mm even (a surface of Euler characteristic 2m2\frac{2-m}{2}). In particular, we have the following:

Corollary 5 (Theorem 5.3 from [8]).

Let SS be a normal surface in LST(1,m)\operatorname{LST}(1,m), m2m\geq 2, with connected essential boundary. Then SS has edge weight 11 on the longitudinal edge of LST(1,m).\operatorname{LST}(1,m).

If the layered solid torus triangulation is generated using the standard Regina [3] function, then the surface SS in Corollary 5 has edge weight 11 on the edge e2=Δ0(03)=Δ0(21)e_{2}=\Delta_{0}(03)=\Delta_{0}(21).

6.5 Determining the natural geometric framing on 1\partial_{1} and 2\partial_{2}

Just as in Section 5, we denote the geometric framing of i\partial_{i} by (μi,λi)(\mu_{i},\lambda_{i}), i=1,2i=1,2.

Gluing LST(0,1)\operatorname{LST}(0,1) to 2\partial_{2} with the meridian edge along e19e_{19} produces a manifold with fundamental group free of rank 22 and hence the 22-component unlink. Hence, e19e_{19} runs parallel to the meridian μ2\mu_{2} in the geometric framing of 2\partial_{2}. Gluing in the same layered solid torus along the other two edges demonstrates that e18e_{18} runs parallel to the geometric longitude λ2\lambda_{2} and that e20e_{20} runs parallel to μ21λ2\mu^{-1}_{2}\lambda_{2}.

Gluing LST(0,1)\operatorname{LST}(0,1) with the meridian edge onto the edges e4e_{4} and e2e_{2} yields the fundamental group of the link complement of the remaining two link components (a double twisted Hopf link). Gluing the meridian edge onto e0e_{0} shows that this edge runs parallel to μ12λ1\mu_{1}^{2}\lambda_{1} in the geometric framing. This implies that e4e_{4} runs parallel to μ11\mu_{1}^{-1} and e2e_{2} runs parallel to μ1λ1\mu_{1}\lambda_{1}. This computation is confirmed by noting that the homological longitude has edge weight 22 on e0e_{0} and edge weight 11 on e2e_{2} and e4e_{4} (as observed by an orientable surface with this boundary curve, see Figure 8 on the left) and the fact that this homological longitude coincides with the geometric longitude.

The above computations were verified using SnapPy [4] and SnapPy in sage for the homological longitude. See Figures 9 and 8 for pictures of 1\partial_{1} and 2\partial_{2} with their respective framings.

The information about the natural geometric framing on 1\partial_{1} and 2\partial_{2} combined with Equation 5.1 determine which layered solid tori to glue to 1\partial_{1} and 2\partial_{2} to recover Mk,nM_{k,n}.

In detail, LST(1,k1)\operatorname{LST}(1,k-1) must be glued to 1\partial_{1} with the edge weight-11 boundary edge of the layered solid torus glued to e2e_{2}. Similarly, LST(1,n)\operatorname{LST}(1,n) must be glued to 2\partial_{2} with the edge weight-11 boundary edge of the layered solid torus glued to edge e19e_{19}. See Figure 10 for a detailed picture of the gluings.

Refer to caption

Figure 10: Filling 𝒯\mathcal{T}^{\prime} with suitable layered solid tori.

6.6 Euler characteristic of the completion of SiS_{i}, 1i31\leq i\leq 3.

We are now in a position to determine the norms of αi\alpha_{i}, 1i31\leq i\leq 3.

The triple (a,b,c)(a,b,c) denotes the (parities of the) edge weights of e0e_{0}, e2e_{2}, and e4e_{4} in that order for 1\partial_{1} and (d,e,f)(d,e,f) denotes the (parities of the) edge weights of e18e_{18}, e19e_{19}, and e20e_{20} in that order for 2\partial_{2}.

The boundary pattern of α1\alpha_{1} is (0,1,1)(0,1,1) with respect to the three edges on 1\partial_{1} and (0,0,0)(0,0,0) with respect to 2.\partial_{2}. These parities are realised by the following edge weights of the fundamental surfaces. We have (2,1,1)(2,1,1) (χ=1\chi=-1), and (0,1,1)(0,1,1) (χ=2\chi=-2). The former cannot be continued into the layered solid torus, the latter continues along the canonical surface of Euler characteristic k+32\frac{-k+3}{2}. In total, this yields a surface of Euler characteristic k+322=k12\frac{-k+3}{2}-2=\frac{-k-1}{2}, hence the norm of α1\alpha_{1} is k+12\frac{k+1}{2}.

The boundary pattern of α2\alpha_{2} is (0,1,1)(0,1,1) with respect to the three edges on 2\partial_{2} and (0,0,0)(0,0,0) with respect to 1.\partial_{1}. These parities are realised by the following edge weights of the fundamental surfaces. We have (0,1,1)(0,1,1) (χ=1\chi=-1), (2,1,3)(2,1,3) (χ=2\chi=-2), and (2,1,1)(2,1,1) (χ=2\chi=-2). The first can be completed with canonical surface of Euler characteristic n+12\frac{-n+1}{2}. In total, this produces a surface representing α2\alpha_{2} with Euler characteristic n+121=n12\frac{-n+1}{2}-1=\frac{-n-1}{2}. The second cannot be continued into the layered solid torus. The third bounds a normal surface in the layered solid torus obtained from the canonical normal surface by one boundary compression. It is hence of Euler characteristic n+32\frac{-n+3}{2} yielding, again, a normal surface of total Euler characteristic n+322=n12\frac{-n+3}{2}-2=\frac{-n-1}{2}. Hence, both the first and the third surfaces are taut, and we thus have that the norm of α2\alpha_{2} is n+12\frac{n+1}{2}.

As shown in Section 6.3, having computed the claimed norms of α1\alpha_{1} and α2,\alpha_{2}, we may now restrict ourselves to normal surfaces with the boundary pattern of α3.\alpha_{3}. Since e2e_{2} and e19e_{19} are both glued to edge weight 11-edges of layered solid tori of type LST(1,m)\operatorname{LST}(1,m), it follows from Corollary 5 that a necessary condition for a normal surface in 𝒯\mathcal{T}^{\prime} to extend into the layered solid tori is that it has edge weight 11 on e2e_{2} and e19.e_{19}.

Going through Table 3, compatibility class by compatibility class, this leaves us with the following cases:

Class 1

Edge weights 11 for both e2e_{2} and e19e_{19}, but cannot be extended into layered solid torus at 1\partial_{1} (no normal surface in LST(1,k1)\operatorname{LST}(1,k-1) has edge weights (2,1,1)(2,1,1)).

Class 2

Has w(e19)>1w(e_{19})>1 for all of its members and can thus be disregarded.

Class 3

Has valid edge weights for k=l=0k=l=0. This yields a surface with Euler characteristic 3-3 and edge weights (4,1,3)(4,1,3) on both 1\partial_{1} and 2\partial_{2}. While this surface extends into LST(1,n)\operatorname{LST}(1,n) at 2\partial_{2}, it does not extended into LST(1,k1)\operatorname{LST}(1,k-1) at 1\partial_{1}.

Class 4

Has valid edge weights for k=l=0k=l=0. This yields a surface with Euler characteristic 1-1 and edge weights (0,1,1)(0,1,1) on both 1\partial_{1} and 2\partial_{2}. This surface extends via the canonical 0/10/1-surface into both LST(1,n)\operatorname{LST}(1,n) and LST(1,k1)\operatorname{LST}(1,k-1) and produces a closed 11-sided surface of Euler characteristic

1+1n2+3k2=n+k22.-1+\frac{1-n}{2}+\frac{3-k}{2}=-\frac{n+k-2}{2}.
Class 5

Has w(e2)>1w(e_{2})>1 for all of its members and can thus be disregarded.

Class 6

Has valid edge weights for k=l=0k=l=0. Gives same Euler characteristic and edge weights as Class 4.

Class 7

Has valid edge weights for k=l=0k=l=0. Gives same Euler characteristic and edge weights as Class 4.

Altogether, it follows that the norm of α3\alpha_{3} equals n+k22\frac{n+k-2}{2}.

7 Generalisations

As mentioned in the introduction, the triangulations 𝒯k,n\mathcal{T}_{k,n} can be generalised to further conjecturally minimal triangulations. In this section we present one such family that was again found using experimentation with the census.

Consider the triangulation 𝒰3,3\mathcal{U}_{3,3} with Regina isomorphism signature iLLwQPcbeefgehhhhhqhhqhqx, and given by the gluing table

Tet (012)(012) (013)(013) (023)(023) (123)(123)
0 3(012)3(012) 1(102)1(102) 2(023)2(023) 1(123)1(123)
11 0(103)0(103) 4(102)4(102) 4(023)4(023) 0(123)0(123)
22 6(012)6(012) 5(013)5(013) 0(023)0(023) 4(301)4(301)
33 0(012)0(012) 4(231)4(231) 6(132)6(132) 5(032)5(032)
44 1(103)1(103) 2(231)2(231) 1(023)1(023) 3(301)3(301)
55 7(103)7(103) 2(013)2(013) 3(132)3(132) 7(123)7(123)
66 2(012)2(012) 7(320)7(320) 7(201)7(201) 3(032)3(032)
77 6(230)6(230) 5(102)5(102) 6(310)6(310) 5(123)5(123)

This triangulation coincides with census triangulation t12546 #1\#1 of a once-cusped hyperbolic 33-manifold. Its first homology group is 24\mathbb{Z}\oplus\mathbb{Z}_{2}\oplus\mathbb{Z}_{4}, and its hyperbolic volume is approximately 7.5557.555.

The triangulation contains two copies of solid torus T3T_{3} (tetrahedra 0, 11, 44, and tetrahedra 55, 66, 77). But unlike in 𝒯3,3\mathcal{T}_{3,3}, in 𝒰3,3\mathcal{U}_{3,3} they are not identified along their boundaries. Instead, they attach to a central complex consisting of tetrahedra 22, and 33.

We replace the two copies of T3T_{3} in 𝒰3,3\mathcal{U}_{3,3} by TkT_{k} and TnT_{n}, k,n3k,n\geq 3 odd, to obtain a family of triangulations 𝒰k,n\mathcal{U}_{k,n} with n+k+2n+k+2 tetrahedra, and three non-trivial 2\mathbb{Z}_{2}–torsion classes. The three normal surfaces F1F_{1}, F2F_{2}, and F3F_{3} of each solid torus pair up symmetrically through the central 22–tetrahedra interface. This produces three normal surfaces, each consisting entirely of quadrilaterals. Because of the symmetric pairing of surfaces from the solid tori, 𝒰k,n\mathcal{U}_{k,n} is isomorphic to 𝒰n,k\mathcal{U}_{n,k}. The three quadrilateral normal surfaces have Euler characteristic n+k2-\frac{n+k}{2}, n+k2-\frac{n+k}{2}, and 2-2 respectively. Their sum, hence, equals the negative of the number of tetrahedra in 𝒰k,n\mathcal{U}_{k,n}. We conjecture that these surfaces are taut, and hence these triangulations are minimal due to Theorem 1.

As with the main examples of this paper, the family 𝒰k,n\mathcal{U}_{k,n} arises by Dehn surgery on a thrice-cusped hyperbolic 3–manifold. Indeed, replacing the two solid tori with a cusp each yields a 33-cusped ideal triangulation with Regina isomorphism signature kLLPwLQkceefeijijijiiapuuxptxl. According to SnapPy’s identify function [4] this triangulation is decomposed into ten regular ideal hyperbolic tetrahedra and gives the thrice-cusped Platonic manifold otet10_00015 (see [6]). It follows that the triangulation of the Platonic manifold is minimal.

It is an interesting open problem to determine further generalisations of this construction, using even more ways of identifying the two solid torus triangulations TkT_{k} and TnT_{n} along a subcomplex.

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