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Satellite knots and trivializing bands

Lorena Armas-Sanabria Lorena Armas-Sanabria
Universidad Tecnológica de Querétaro
Av. Pie de la Cuesta 2501
Querétaro, MEXICO
[email protected]
 and  Mario Eudave-Muñoz Mario Eudave-Muñoz
Instituto de Matemáticas
Universidad Nacional Autónoma de México
Unidad Juriquilla, Querétaro, MEXICO
[email protected]
Abstract.

We show an infinite family of satellite knots that can be unknotted by a single band move, but such that there is no band unknotting the knots which is disjoint from the satellite torus.

1. Introduction

.

Let KK be a knot or link in the 3-sphere. A banding KbK_{b} of KK is a knot or link obtained from KK by the following construction. Let b:I×IS3b:I\times I\rightarrow S^{3} be an embedding such that b(I×I)K=b(I×I)b(I\times I)\cap K=b(\partial I\times I), and then KbK_{b} is defined as Kb=(Kb(I×I))b(I×I)K_{b}=(K-b(\partial I\times I))\cup b(I\times\partial I).

If KK and KbK_{b} are both knots, a band move is also called an H(2)H(2)-move, see [2]. Then the u2u_{2} unknotting number of a knot KK, u2(K)u_{2}(K), is defined as the minimal number of H(2)H(2) moves needed to transform KK into a trivial knot.

Let VV be a standard solid torus contained in S3S^{3}, and KK^{\prime} a knot embedded in VV such that KK^{\prime} is not contained in any 33-ball contained in VV nor it is isotopic to a longitude of VV. Let JJ be a non-trivial knot in S3S^{3} and let N(J)N(J) be a closed regular neighborhood of JJ. Let h:VN(J)h:V\rightarrow N(J) be a homeomorphism such that a preferred longitude λV\lambda\subset V is mapped to a longitude ll of N(J)N(J). Then h(K)=Kh(K^{\prime})=K is called a satellite knot with companion knot JJ and pattern (V,K,l)(V,K^{\prime},l). The torus Q=N(J)Q=\partial N(J) is called a satellite torus of KK. For an example of a satellite knot see Figure 3.

It is easy to construct examples of satellite knots which can be unknotted by a single band move. Let JJ be a non-trivial knot with neighborhood N(J)N(J). Take a trivial knot UU inside N(J)N(J). Take a band bb for UU disjoint from the torus N(J)\partial N(J), which wraps around N(J)N(J) in a complicated manner. The knot KbK_{b} obtained by the band move is a satellite knot with companion JJ. By taking a band bb^{\prime} dual to bb, we get the trivial knot UU, and the band bb^{\prime} is clearly disjoint from the companion torus.

So, it is natural to ask:

Question: if KK is a satellite knot with satellite torus QQ, which can be unknotted by a single band move, is there an isotopy that makes the corresponding band disjoint from QQ?

Note that if instead of doing a band move we do a crossing change, then the answer to the previous question is positive. That is, any crossing change that unknots a satellite knot can be made disjoint from the satellite torus. This was proved by Scharlemann and Thompson [12]. This result can be generalized to any non-integral tangle replacement, see [3].

Here we give a negative answer to that question. We show the existence of an infinite family of knots K(m,n,p;q)K(m,n,p;q), where m,n,p,qm,\,n,\,p\,,q are integral parameters with some restrictions, such that K(m,n,p;q)K(m,n,p;q) is a satellite knot with companion a (2,q)(2,-q)-torus knot JJ, and a banding of it produces the trivial knot. It is shown that the band intersects the satellite torus QQ in two arcs and as the winding number of K(m,n,p;q)K(m,n,p;q) in N(J)N(J) is ±1\pm 1 or ±3\pm 3, it follows easily that the band cannot be made disjoint from the torus QQ.

By taking double branched covers, we get an infinite family of strongly invertible hyperbolic knots K~(m,n,p;q)\tilde{K}(m,n,p;q), having an integral exceptional Dehn surgery that produces a manifold containing an incompressible torus TT that intersects the surgered solid tori in 44 disks. In other words, there is an essential four punctured torus properly embedded in the exterior of K~(m,n,p;q)\tilde{K}(m,n,p;q). Many examples of knots with this type of surgery are already known, see the introduction of [4] for a survey of this topic. The new in these examples is that the essential torus is disjoint from the involution axis of the strongly invertible knot.

2. Main examples

.

Let VV be a standard solid torus in S3S^{3} and KK^{\prime} be the pattern shown in Figure 1, where m,n,p,qm,\,n,\,p,\,q denote integral numbers. An horizontal box labeled by, say [m][m], denotes mm horizontal crossings, and the box labeled [q][q] denotes qq vertical crossing. Our convention on the sign of the crossings is given in Figure 1. Assume that m,n0m,\,n\not=0, and that qq is odd; pp can be any integer. By inspection it can be seen that KK^{\prime} is in fact a knot if m,nm,\,n are odd number and pp is even, or if mm is odd and n,pn,\,p are even, or if m,pm,\,p are even and nn odd, or if m,n,pm,\,n,\,p are all even. In the remaining cases KK^{\prime} is a two components link. The winding number of KK^{\prime} in VV is ±1\pm 1 or ±3\pm 3, depending on an orientation given to KK^{\prime}. In fact, when KK^{\prime} is a knot, it has winding number ±3\pm 3 when m,nm,\,n are odd and pp is even, and it has winding number ±1\pm 1 in all the other cases.

Refer to caption
Figure 1. The pattern knot.

Consider the disks D1D_{1}, D2D_{2}, D3D_{3}, D4D_{4} contained in VV as shown in Figure 1. These are meridian disks of VV, each intersecting KK^{\prime} in 3 points. Note that these disks divide VV in four regions which we denote by H1,H2,H3,H4H_{1},H_{2},H_{3},H_{4}, where HiH_{i} is bounded by DiD_{i} and Di+1D_{i+1}, mod 4\textrm{mod}\,4. Note that ti=HiKt_{i}=H_{i}\cap K^{\prime} consists of three arcs, and then (Hi,ti)(H_{i},t_{i}) can be considered as a 3-tangle, as shown in Figure 2 (a) for H2H_{2}. The pair (Hi,ti)(H_{i},t_{i}) can be seen as the union of a 2-tangle, in fact a rational tangle (B,t)=R(p/q)(B,t)=R(p/q), and a trivial arc, as shown in Figure 2 (b). In fact, H1H_{1} can be seen as the union of the rational tangle R((npq+n+p)/(pq+1))R((npq+n+p)/(pq+1)) and a trivial arc by the right; H2H_{2} can be seen as the union of the rational tangle R(m)R(m) and a trivial arc by the left; H3H_{3} can be seen as the union of the rational tangle R(n)R(-n) and a trivial arc by the right; H4H_{4} can be seen as the union of the rational tangle R(m)R(-m) and a trivial arc by the left. The tangle (Hi,ti)(H_{i},t_{i}) will be a braid, that is, it consists of descending arcs going from DiD_{i} to Di+1D_{i+1}, only if m=±1m=\pm 1, or n=±1n=\pm 1, or p=0p=0 and n=±1n=\pm 1, or p=1,q=3,n=1p=1,q=-3,n=1, or p=1,q=3,n=1p=-1,q=3,n=-1.

Refer to caption
Figure 2. The tangle H2H_{2}.

Note that there is a disk Di1D_{i1} in HiH_{i}, whose boundary is contained in DiD_{i}, and which intersects KK^{\prime} in two points, in fact, Di1D_{i1} cuts off the rational tangle (B,t)(B,t), as in Figure 2 (c). Note that Di1D_{i1} is not isotopic to a disk in DiD_{i}, except when (Hi,ti)(H_{i},t_{i}) is a braid. Similarly there is such a disk Di2D_{i2} whose boundary is contained in Di+1D_{i+1}, also shown in Figure 2 (c). Note also that there is an annulus AiA_{i} in HiH_{i}, with one boundary component in DiD_{i} and other in Di+1D_{i+1}, which encloses the tangle (B,t)(B,t), as in Figure 2 (d). If (Hi,ti)(H_{i},t_{i}) is a braid then there are several annuli which enclose two of the arcs of the braid, which we also denote by AiA_{i}.

Lemma 2.1.

The wrapping number of KK^{\prime} in VV is exactly 3.

Proof.

The winding number of KK^{\prime} is VV is ±1\pm 1 or ±3\pm 3, so the wrapping number is 1 or 3. Suppose that it is 1. Then there is a meridian disk DD of VV which intersects KK^{\prime} in one point. We can assume that D\partial D is disjoint from Di\partial D_{i} for all ii, hence DDiD\cap D_{i} consists only of simple closed curves. Let γ\gamma be an innermost such curve in DD. Then γ\gamma bounds a disk DD^{\prime} in DD with interior disjoint from the DisD_{i}^{\prime}s, and it is either disjoint from KK^{\prime} or intersects it in one point. The disk DD^{\prime} must be in a region HiH_{i}. Then in fact DD^{\prime} is isotopic to a disk in DiD_{i}, and after an isotopy the intersection is removed. We continue until there is no intersection left between DD and the DisD_{i}^{\prime}s. Then DD would be contained in a region HiH_{i}, which clearly is not possible. ∎

Lemma 2.2.

The knot KK^{\prime} has no local knots, that is, if SS is a sphere in VV which intersects KK^{\prime} in two points, then SS bounds a 3-ball which contains an unknotted spanning arc of KK^{\prime}.

Proof.

The proof is similar to that of Lemma 2.1, by looking at the intersections between a sphere with the disks DiD_{i}. ∎

Lemma 2.3.

If EE is a disk properly embedded in HiH_{i}, whose boundary lies in DiD_{i} or Di+1D_{i+1} and which intersects KK^{\prime} in two points, then it is either parallel to a disk on DiD_{i} or Di+1D_{i+1}, or it is isotopic to Di1D_{i1} or Di2D_{i2}.

Proof.

Suppose that the 3-tangle (Hi,ti)(H_{i},t_{i}) is not a braid, for in this case the conclusion is obvious. Let EE^{\prime} be a disk in HiH_{i}, such that E=αβ\partial E^{\prime}=\alpha\cup\beta, where α\alpha is an arc in DiD_{i} and β\beta is an arc in Di1D_{i1}. Suppose that the interior of EE^{\prime} is disjoint from Di1D_{i1}, and that EE^{\prime} is disjoint from KK^{\prime} or intersects it transversely in one point. The arc β\beta in Di1D_{i1} cuts off a disk DD^{\prime}, which is disjoint from KK^{\prime} or intersects it in one point. If EE^{\prime} is disjoint from KK^{\prime} and DD^{\prime} intersects KK^{\prime} in one point, then the disk EE^{\prime} would separate the strings of the tangle (B,t)(B,t) determined by Di1D_{i1}, which is not possible. In all other cases, EE^{\prime} and DD^{\prime} are parallel, that is, cobound with part of DiD_{i} a 3-ball disjoint from KK^{\prime}, or intersecting it in an unknotted spanning arc.

Suppose EE is a disk as in the statement of the lemma, whose boundary lies on DiD_{i}. Look at the intersections between Di1D_{i1} and EE. Let γ\gamma be a simple closed curve of intersection which is innermost in EE. If γ\gamma bounds a disk disjoint from KK^{\prime} or intersecting it in one point, then this is easily removed, for there are no local knots in KK^{\prime}. Now suppose that γ\gamma is an outermost arc of intersection in EE, bounding a disk EE^{\prime}. Then, by the previous paragraph, this disk would be parallel to a disk in Di1D_{i1}, and by an isotopy the intersection could be removed. The only remaining case is that γ\gamma bounds a disk intersecting KK^{\prime} twice, and that there are no arcs of intersection. In that case E\partial E must be parallel to Di1\partial D_{i1}, and then EE is parallel to a disk in DiD_{i}, or it is parallel to Di1D_{i1}. ∎

Lemma 2.4.

If EE is an annulus properly embedded in HiH_{i}, whose boundary lies in DiDi+1D_{i}\cup D_{i+1}, and such that it is disjoint from KK^{\prime}, then it is either parallel to an annulus on DiD_{i} or Di+1D_{i+1}, or it is isotopic to the annulus AiA_{i}, or it is parallel to the part of V\partial V lying in HiH_{i}, or is parallel to the frontier of an arc of tit_{i}.

Proof.

Again, look at the intersections between EE and Di1D_{i1}, Di2D_{i2} and AiA_{i}. ∎

Lemma 2.5.

There is no Conway sphere in VV.

Proof.

Suppose that SS is a Conway sphere for KK^{\prime} in VV, that is, SS is a sphere in VV that intersects KK^{\prime} transversely in four points, and SKS-K^{\prime} is incompressible in VKV-K^{\prime}. Look at the intersections between SS and the disks DiD_{i}. If this intersection is empty, then SS would be contained in some HiH_{i}, but this is not possible for (Hi,ti)(H_{i},t_{i}) is a trivial tangle. Let γ\gamma be a simple closed curve of intersection which is innermost in SS. If γ\gamma bounds a disk disjoint from KK^{\prime} or intersecting it in one point, then this is easily removed. So γ\gamma bounds a disk intersecting KK^{\prime} twice. It follows that the intersection consists of concentric curves, with two of them, say γ1\gamma_{1} and γ2\gamma_{2}, bounding disks E1E_{1} and E2E_{2} which intersect KK^{\prime} in two points. Between E1E_{1} and E2E_{2} there is a collection of annuli F1,,FrF_{1},\dots,F_{r}, which may be empty. If one of EiE_{i} or FjF_{j} is parallel to a disk or annulus in some DiD_{i}, then the number of curves of intersection could be reduced. Then, say, E1E_{1} is in some HiH_{i} and by Lemma 2.3 is parallel to the disk Di2D_{i2}, and similarly E2E_{2} is in some HjH_{j} and is parallel to the disk DjtD_{jt}. The annuli FjF_{j} are then spanning annuli in some HiH_{i}. Note that Di2\partial D_{i2} and D(i+1)1\partial D_{(i+1)1} have non-empty intersection, and also Di2\partial D_{i2} and Ai+1\partial A_{i+1} have non-empty intersection, except perhaps if Hi+1H_{i+1} is a braid. By inspection it follows that is not possible to assemble the pieces to get the desired sphere.∎

Lemma 2.6.

If TT is an incompressible torus in VKV-K^{\prime}, then it is either parallel to V\partial V, or parallel to N(K)\partial N(K^{\prime}).

Proof.

Let TT be an incompressible torus in VKV-K^{\prime}. Look at the intersection between TT and the disks DiD_{i}. This intersection consists of curves that divide TT into annuli, which we can suppose are not annuli parallel to an annulus lying in some DiD_{i}, that is, all are spanning annuli in the HiH_{i}. If in some HiH_{i} there is an annulus which is parallel to an annulus AiA_{i}, then it can be seen that the torus cannot be assembled. Then each such annuli is either an annulus running along an arc of tit_{i}, or is parallel to V\partial V. We conclude that the torus is parallel to V\partial V, or parallel to N(K)\partial N(K^{\prime}). ∎

Lemma 2.7.

If AA is an annulus properly embedded in VV, disjoint from KK^{\prime} and incompressible in VKV-K^{\prime} then AA is parallel to an annulus in V\partial V. There is no properly embedded Möbius band in VV disjoint from KK^{\prime}.

Proof.

Let AA be an incompressible annulus in VKV-K^{\prime}. Look at the intersection between AA and the disks DiD_{i}. This intersection consists of arcs, which we can assume divide the annulus into rectangles. That is, the intersection of AA with each HiH_{i} consists of one of more rectangles. But these rectangles cannot be assembled to form an annulus, except perhaps if each tangle HiH_{i} is a braid, that is, if KK^{\prime} is a closed braid in VV and that KK^{\prime} is parallel to a curve on V\partial V. KK^{\prime} is a closed braid only when m=±1m=\pm 1, n=±1n=\pm 1 and p=0p=0, or when m=±1m=\pm 1, and p=1,q=3,n=1p=1,q=3,n=1, or when m=±1m=\pm 1, and p=1,q=3,n=1p=-1,q=-3,n=-1. This gives a total of 8 closed braids, and it can be checked that none of them is parallel to a curve contained in V\partial V. If there is a Möbius band disjoint from KK^{\prime}, then there is also an incompressible torus disjoint from KK^{\prime}, which is not possible.∎

Let JJ be a (2,q)(2,-q)-torus knot, and let h:VN(J)h:V\rightarrow N(J) be a homeomorphism such that a preferred longitude λV\lambda\subset V is mapped to a longitude ll of N(J)N(J) of slope 2q-2q. Let K=K(m,n,p;q)K=K(m,n,p;q) be the satellite knot h(K)h(K^{\prime}), and let Q=N(J)Q=\partial N(J) be the satellite torus. See Figure 3, which shows the case q=3q=3.

Refer to caption
Figure 3. The satellite knot.

Let b:I×IS3b:I\times I\rightarrow S^{3} be the banding of K(m,n,p;q)K(m,n,p;q) shown in Figure 3, an let KbK_{b} be the knot so obtained.

Proposition 2.8.

The knot KbK_{b} is a trivial knot.

Proof.

To see this in an easy way, note that there is a Möbius band \mathcal{M} properly embedded in the exterior of JJ with slope 2q-2q. Let AA be an annulus embedded in VV whose boundary consists of preferred longitudes of VV, such that a diagram of KK^{\prime} can be drawn on AA. Consider now h(A)h(A) and note that one of its boundary components coincide with \partial\mathcal{M}. Then =h(A)\mathcal{M}^{\prime}=\mathcal{M}\cup h(A) is a Möbius band which contains a diagram of K(m,n,p;q)K(m,n,p;q). Consider the band bb shown in Figure 3 and note that it is contained in \mathcal{M}^{\prime}, and then we have a diagram of KbK_{b} on \mathcal{M}^{\prime}. Following Figure 4, do isotopies of KbK_{b} along \mathcal{M}^{\prime} to undo the crossing in the boxes mm, m-m, then undo the crossings in the boxes nn and n-n, until we get to the penultimate diagram of Figure 4. There the crossings in the box labelled with qq cancel with the crossings introduced by the Möbius band, and then just undo the crossings in the box labeled by pp. ∎

Refer to caption
Figure 4. Obtaining the trivial knot.

Now we show that the band cannot be isotoped to be disjoint from QQ, in fact we can show more.

Proposition 2.9.

No banding of K(m,n,p;q)K(m,n,p;q) that produces a trivial knot can be disjoint from QQ.

Proof.

Suppose that bb is a band for K=K(m,n,p;q)K=K(m,n,p;q) which produces by banding a trivial knot UU and that bb is disjoint from QQ. Give an orientation to KK. Remember that the wrapping number of KK in the solid torus h(V)h(V) is 33. Then bb intersects a meridian disk of h(V)h(V) in a collection of rr arcs. So UU intersects a meridian disk of h(V)h(V) in 3+2r3+2r points. Then the winding number of UU in h(V)h(V) is an odd number. and then UU cannot be inside a 33-ball contained in h(V)h(V). It follows that QQ is incompressible in the exterior of UU, then UU is not trivial. ∎

Lemma 2.10.

The torus QQ is the only incompressible torus in the exterior of KK, and there is no Conway sphere for KK.

Proof.

Suppose that PP is a Conway sphere for KK. Consider first the intersections between PP and QQ. We can assume that the intersection consists of curves that are essential on both PP and QQ. Let γ\gamma be an innermost curve of intersection in PP. Then γ\gamma bounds a disk DD in PP containing one or two points of intersection with KK. Because the wrapping number of KK in h(V)h(V) is 33, this is not possible. Then PP is disjoint from QQ, and it must be contained in h(V)h(V). By Lemma 2.5 this is not possible.

Suppose now that PP is an essential torus not isotopic to QQ. Again look at the intersection between PP and QQ, which then consists of curves which are essential in both PP and QQ. Let γ1\gamma_{1} and γ2\gamma_{2} be a pair of intersection curves that bound an annulus AA in PP with interior disjoint from QQ and disjoint from N(J)N(J). If AA is a boundary parallel annulus in the exterior of JJ, E(J)E(J), an isotopy reduces the number of arcs of intersection. If AA is essential in E(J)E(J), then its boundary consists of curves of slope 2q-2q on QQ. Then the annulus AA^{\prime} in PP adjacent to AA is boundary parallel in h(V)h(V). By an isotopy the number of arcs of intersection are reduced. Then PP is disjoint from QQ. As JJ is a torus knot, there are not essential tori in its complement. Then PP is contained in VV. By Lemma 2.6 this is not possible. ∎

3. Dehn surgery

.

Let K=K(m,n,p;q)K=K(m,n,p;q) be the knot or link defined in the previous section and let bb the band defined in Proposition 2.8. Let B=N(b)B^{\prime}=N(b). Then BB^{\prime} is a 3-ball that intersects KK in two arcs. Let KbK_{b} be the banding of KK, so KbK_{b} is the trivial knot; KbK_{b} intersects BB^{\prime} also in two arcs. Let BB be the complementary ball of BB^{\prime} in S3S^{3}, and let t=KBt=K\cap B, so tt consists of two arcs properly embedded in BB. That is, the pair (B,t)(B,t) can be considered as a 2-tangle, and the knots KK and KbK_{b} can be considered as obtained by filling BB with rational tangles.

Let π:S3S3\pi:S^{3}\rightarrow S^{3} be the the double cover of S3S^{3} branched along KbK_{b}. As KbK_{b} is a trivial knot, the double branched cover is the 3-sphere. Let N=π1(N(b))N=\pi^{-1}(N(b)). Then NN is a solid torus, its core is a knot in S3S^{3} which we denote by K~=K~(m,n,p;q)\tilde{K}=\tilde{K}(m,n,p;q). By Montesinos trick, the double branched cover of KK is then obtained by performing rr-Dehn surgery on K~\tilde{K} for some integral slope rr; this surgered manifold is denoted by K~(r)\tilde{K}(r). Let π~=K~(r)S3\tilde{\pi}=\tilde{K}(r)\rightarrow S^{3} be the corresponding branched cover. Let V~=π~1(V)\tilde{V}=\tilde{\pi}^{-1}(V), and let M~=π~1(E(J))\tilde{M}=\tilde{\pi}^{-1}(E(J)), and let T=π~1(Q)T=\tilde{\pi}^{-1}(Q). Note that because the winding number of KK in h(V)h(V) is an odd number, TT is then a single torus which is a double cover of QQ. The torus QQ intersects BB^{\prime} in two disks, which then implies that TT intersects NN in four disks. Then T~=TE(K~)\tilde{T}=T\cap E(\tilde{K}) is a four-punctured torus properly embedded in the exterior of K~\tilde{K}.

Lemma 3.1.

The JSJJSJ decomposition of K~(r)\tilde{K}(r) is given by K~(r)=V~M~\tilde{K}(r)=\tilde{V}\cup\tilde{M}, where V~\tilde{V} is a hyperbolic manifold and M~\tilde{M} is a Seifert fibered space.

Proof.

The manifold M~\tilde{M} is the double cyclic cover of the exterior of the (2,q)(2,-q) torus knot JJ, and then by [11] is the Seifert fibered manifold (D2;(q1)/2q,(q1)/2q)(D^{2};\frac{(q-1)/2}{q},\frac{(q-1)/2}{q}).

If V~\tilde{V} is not an hyperbolic manifold, then by Thurston Hyperbolicity Theorem, V~\tilde{V} will have a compressing disk, a reducing sphere, an essential annulus or an essential torus. If there is any of these surfaces, by one of the several equivariant results [9], [10], [8], there is a surface SS which is equivariant, that is, τ(S)=S\tau(S)=S, or τ(S)S=\tau(S)\cap S=\emptyset, where τ\tau is the involution defined on V~\tilde{V} by the double branched cover. By taking the projection π~(S)\tilde{\pi}(S), there will be a compression disk for V\partial V disjoint from KK^{\prime}, a meridian disk intersecting KK^{\prime} in one point, a decomposing sphere for KK^{\prime}, a meridian disk intersecting KK^{\prime} in two points, an essential annulus or Möbius band, or an essential torus or Conway sphere for KK^{\prime}. None of these can exist by Lemmas 2.1, 2.2, 2.5, 2.6 or 2.7,. ∎

Lemma 3.2.

The knot K~=K~(m,n,p;q)\tilde{K}=\tilde{K}(m,n,p;q) is hyperbolic.

Proof.

First note that K~\tilde{K} cannot be a torus knot, for it has a Dehn surgery producing a 3-manifold containing a separating incompressible torus. Suppose K~\tilde{K} is a satellite knot, and let RR be an incompressible torus in its exterior. As K~\tilde{K} is strongly invertible, by the Equivariant Torus Theorem [8], there is an incompressible torus R~\tilde{R}, which is equivariant under the involution defined on K~\tilde{K}. R~\tilde{R} bounds a solid torus WW which contains K~\tilde{K}. The complement of WW may contain incompressible tori other than R~\tilde{R}, but applying again the Equivariant Torus Theorem, there will be another equivariant torus in the complement of WW. Therefore we can assume that there is an equivariant torus RR, which defines then a companion knot K¯\overline{K} for K~\tilde{K} which is hyperbolic or a torus knot.

Suppose first that RR compresses after performing rr-Dehn surgery. Then by [5], K~\tilde{K} is a 0 or 1-bridge braid in WW, with winding number w2w\geq 2. It follows from [6] that the manifold K~(r)\tilde{K}(r) is obtained by n2n^{2}-Dehn surgery on K¯\overline{K}, for some integer nn. This is not possible if K¯\overline{K} is a torus knot, for the surgery produces a 3-manifold containing a separating incompressible torus. Also, this is not possible if K¯\overline{K} is an hyperbolic knot, because by [7], we should have w22w^{2}\leq 2.

Suppose now that RR is incompressible in K~(r)\tilde{K}(r). As RR is equivariant, π(R)\pi(R), is a torus or a Conway sphere. But, by Lemma 2.10 there are no Conway spheres for KK. If π(R)\pi(R) is a satellite torus for KK, it would have to be isotopic to QQ by Lemma 2.10. But, as π(R)\pi(R) is disjoint from the band, this is not possible by Proposition 2.9. ∎

So we have shown,

Teorema 3.3.

There is a family of hyperbolic strongly invertible knots K~(m,n,p;q)\tilde{K}(m,n,p;q), which have a toroidal surgery containing a unique incompressible torus which hits the surgered solid torus in four disks. Furthermore, the incompressible torus is disjoint from the axis of the involution.

4. Concluding remarks

.

The knots K(m,n,p;q)K(m,n,p;q) can be generalized to K(a1,a2,K(a_{1},a_{2}, ,aN,p;q)\dots,a_{N},p;q), where a1,a2,,aNa_{1},a_{2},\dots,a_{N}, pp and qq are integers, such that NN is even and qq is odd. A pattern for the case N=4N=4 is shown in Figure 5. In this case the wrapping number is N+1N+1. The proofs of Sections 2 and 3 would be identical for large subfamilies of these knots.

The examples can also be generalized when NN is odd and then the wrapping and winding number are even. But in this case the proof of Proposition 2.9 does not hold, for the winding number of KK^{\prime} in VV is even, and a new proof would have to be done. Also, when taking double branched covers in this case, the torus QQ would lift to two tori, giving then examples of hyperbolic knots having two disjoint, non parallel, incompressible tori after Dehn surgery, each intersecting the surgered solid tori in two disks.

Refer to caption
Figure 5. The generalized pattern knot.

We finish with one question,

If KK is a satellite knot with satellite torus QQ, and bb is a band that unknots KK, is there a universal bound for the minimal number of arcs of intersection between bb and QQ? Is this bound just two?


Acknowledgements. Research partially supported by grant PAPIIT-UNAM IN101317.

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