Satellite knots and trivializing bands
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 be a knot or link in the 3-sphere. A banding of is a knot or link obtained from by the following construction. Let be an embedding such that , and then is defined as .
If and are both knots, a band move is also called an -move, see [2]. Then the unknotting number of a knot , , is defined as the minimal number of moves needed to transform into a trivial knot.
Let be a standard solid torus contained in , and a knot embedded in such that is not contained in any -ball contained in nor it is isotopic to a longitude of . Let be a non-trivial knot in and let be a closed regular neighborhood of . Let be a homeomorphism such that a preferred longitude is mapped to a longitude of . Then is called a satellite knot with companion knot and pattern . The torus is called a satellite torus of . 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 be a non-trivial knot with neighborhood . Take a trivial knot inside . Take a band for disjoint from the torus , which wraps around in a complicated manner. The knot obtained by the band move is a satellite knot with companion . By taking a band dual to , we get the trivial knot , and the band is clearly disjoint from the companion torus.
So, it is natural to ask:
Question: if is a satellite knot with satellite torus , which can be unknotted by a single band move, is there an isotopy that makes the corresponding band disjoint from ?
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 , where are integral parameters with some restrictions, such that is a satellite knot with companion a -torus knot , and a banding of it produces the trivial knot. It is shown that the band intersects the satellite torus in two arcs and as the winding number of in is or , it follows easily that the band cannot be made disjoint from the torus .
By taking double branched covers, we get an infinite family of strongly invertible hyperbolic knots , having an integral exceptional Dehn surgery that produces a manifold containing an incompressible torus that intersects the surgered solid tori in disks. In other words, there is an essential four punctured torus properly embedded in the exterior of . 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 be a standard solid torus in and be the pattern shown in Figure 1, where denote integral numbers. An horizontal box labeled by, say , denotes horizontal crossings, and the box labeled denotes vertical crossing. Our convention on the sign of the crossings is given in Figure 1. Assume that , and that is odd; can be any integer. By inspection it can be seen that is in fact a knot if are odd number and is even, or if is odd and are even, or if are even and odd, or if are all even. In the remaining cases is a two components link. The winding number of in is or , depending on an orientation given to . In fact, when is a knot, it has winding number when are odd and is even, and it has winding number in all the other cases.

Consider the disks , , , contained in as shown in Figure 1. These are meridian disks of , each intersecting in 3 points. Note that these disks divide in four regions which we denote by , where is bounded by and , . Note that consists of three arcs, and then can be considered as a 3-tangle, as shown in Figure 2 (a) for . The pair can be seen as the union of a 2-tangle, in fact a rational tangle , and a trivial arc, as shown in Figure 2 (b). In fact, can be seen as the union of the rational tangle and a trivial arc by the right; can be seen as the union of the rational tangle and a trivial arc by the left; can be seen as the union of the rational tangle and a trivial arc by the right; can be seen as the union of the rational tangle and a trivial arc by the left. The tangle will be a braid, that is, it consists of descending arcs going from to , only if , or , or and , or , or .

Note that there is a disk in , whose boundary is contained in , and which intersects in two points, in fact, cuts off the rational tangle , as in Figure 2 (c). Note that is not isotopic to a disk in , except when is a braid. Similarly there is such a disk whose boundary is contained in , also shown in Figure 2 (c). Note also that there is an annulus in , with one boundary component in and other in , which encloses the tangle , as in Figure 2 (d). If is a braid then there are several annuli which enclose two of the arcs of the braid, which we also denote by .
Lemma 2.1.
The wrapping number of in is exactly 3.
Proof.
The winding number of is is or , so the wrapping number is 1 or 3. Suppose that it is 1. Then there is a meridian disk of which intersects in one point. We can assume that is disjoint from for all , hence consists only of simple closed curves. Let be an innermost such curve in . Then bounds a disk in with interior disjoint from the , and it is either disjoint from or intersects it in one point. The disk must be in a region . Then in fact is isotopic to a disk in , and after an isotopy the intersection is removed. We continue until there is no intersection left between and the . Then would be contained in a region , which clearly is not possible. ∎
Lemma 2.2.
The knot has no local knots, that is, if is a sphere in which intersects in two points, then bounds a 3-ball which contains an unknotted spanning arc of .
Proof.
The proof is similar to that of Lemma 2.1, by looking at the intersections between a sphere with the disks . ∎
Lemma 2.3.
If is a disk properly embedded in , whose boundary lies in or and which intersects in two points, then it is either parallel to a disk on or , or it is isotopic to or .
Proof.
Suppose that the 3-tangle is not a braid, for in this case the conclusion is obvious. Let be a disk in , such that , where is an arc in and is an arc in . Suppose that the interior of is disjoint from , and that is disjoint from or intersects it transversely in one point. The arc in cuts off a disk , which is disjoint from or intersects it in one point. If is disjoint from and intersects in one point, then the disk would separate the strings of the tangle determined by , which is not possible. In all other cases, and are parallel, that is, cobound with part of a 3-ball disjoint from , or intersecting it in an unknotted spanning arc.
Suppose is a disk as in the statement of the lemma, whose boundary lies on . Look at the intersections between and . Let be a simple closed curve of intersection which is innermost in . If bounds a disk disjoint from or intersecting it in one point, then this is easily removed, for there are no local knots in . Now suppose that is an outermost arc of intersection in , bounding a disk . Then, by the previous paragraph, this disk would be parallel to a disk in , and by an isotopy the intersection could be removed. The only remaining case is that bounds a disk intersecting twice, and that there are no arcs of intersection. In that case must be parallel to , and then is parallel to a disk in , or it is parallel to . ∎
Lemma 2.4.
If is an annulus properly embedded in , whose boundary lies in , and such that it is disjoint from , then it is either parallel to an annulus on or , or it is isotopic to the annulus , or it is parallel to the part of lying in , or is parallel to the frontier of an arc of .
Proof.
Again, look at the intersections between and , and . ∎
Lemma 2.5.
There is no Conway sphere in .
Proof.
Suppose that is a Conway sphere for in , that is, is a sphere in that intersects transversely in four points, and is incompressible in . Look at the intersections between and the disks . If this intersection is empty, then would be contained in some , but this is not possible for is a trivial tangle. Let be a simple closed curve of intersection which is innermost in . If bounds a disk disjoint from or intersecting it in one point, then this is easily removed. So bounds a disk intersecting twice. It follows that the intersection consists of concentric curves, with two of them, say and , bounding disks and which intersect in two points. Between and there is a collection of annuli , which may be empty. If one of or is parallel to a disk or annulus in some , then the number of curves of intersection could be reduced. Then, say, is in some and by Lemma 2.3 is parallel to the disk , and similarly is in some and is parallel to the disk . The annuli are then spanning annuli in some . Note that and have non-empty intersection, and also and have non-empty intersection, except perhaps if is a braid. By inspection it follows that is not possible to assemble the pieces to get the desired sphere.∎
Lemma 2.6.
If is an incompressible torus in , then it is either parallel to , or parallel to .
Proof.
Let be an incompressible torus in . Look at the intersection between and the disks . This intersection consists of curves that divide into annuli, which we can suppose are not annuli parallel to an annulus lying in some , that is, all are spanning annuli in the . If in some there is an annulus which is parallel to an annulus , then it can be seen that the torus cannot be assembled. Then each such annuli is either an annulus running along an arc of , or is parallel to . We conclude that the torus is parallel to , or parallel to . ∎
Lemma 2.7.
If is an annulus properly embedded in , disjoint from and incompressible in then is parallel to an annulus in . There is no properly embedded Möbius band in disjoint from .
Proof.
Let be an incompressible annulus in . Look at the intersection between and the disks . This intersection consists of arcs, which we can assume divide the annulus into rectangles. That is, the intersection of with each consists of one of more rectangles. But these rectangles cannot be assembled to form an annulus, except perhaps if each tangle is a braid, that is, if is a closed braid in and that is parallel to a curve on . is a closed braid only when , and , or when , and , or when , and . This gives a total of 8 closed braids, and it can be checked that none of them is parallel to a curve contained in . If there is a Möbius band disjoint from , then there is also an incompressible torus disjoint from , which is not possible.∎
Let be a -torus knot, and let be a homeomorphism such that a preferred longitude is mapped to a longitude of of slope . Let be the satellite knot , and let be the satellite torus. See Figure 3, which shows the case .

Let be the banding of shown in Figure 3, an let be the knot so obtained.
Proposition 2.8.
The knot is a trivial knot.
Proof.
To see this in an easy way, note that there is a Möbius band properly embedded in the exterior of with slope . Let be an annulus embedded in whose boundary consists of preferred longitudes of , such that a diagram of can be drawn on . Consider now and note that one of its boundary components coincide with . Then is a Möbius band which contains a diagram of . Consider the band shown in Figure 3 and note that it is contained in , and then we have a diagram of on . Following Figure 4, do isotopies of along to undo the crossing in the boxes , , then undo the crossings in the boxes and , until we get to the penultimate diagram of Figure 4. There the crossings in the box labelled with cancel with the crossings introduced by the Möbius band, and then just undo the crossings in the box labeled by . ∎

Now we show that the band cannot be isotoped to be disjoint from , in fact we can show more.
Proposition 2.9.
No banding of that produces a trivial knot can be disjoint from .
Proof.
Suppose that is a band for which produces by banding a trivial knot and that is disjoint from . Give an orientation to . Remember that the wrapping number of in the solid torus is . Then intersects a meridian disk of in a collection of arcs. So intersects a meridian disk of in points. Then the winding number of in is an odd number. and then cannot be inside a -ball contained in . It follows that is incompressible in the exterior of , then is not trivial. ∎
Lemma 2.10.
The torus is the only incompressible torus in the exterior of , and there is no Conway sphere for .
Proof.
Suppose that is a Conway sphere for . Consider first the intersections between and . We can assume that the intersection consists of curves that are essential on both and . Let be an innermost curve of intersection in . Then bounds a disk in containing one or two points of intersection with . Because the wrapping number of in is , this is not possible. Then is disjoint from , and it must be contained in . By Lemma 2.5 this is not possible.
Suppose now that is an essential torus not isotopic to . Again look at the intersection between and , which then consists of curves which are essential in both and . Let and be a pair of intersection curves that bound an annulus in with interior disjoint from and disjoint from . If is a boundary parallel annulus in the exterior of , , an isotopy reduces the number of arcs of intersection. If is essential in , then its boundary consists of curves of slope on . Then the annulus in adjacent to is boundary parallel in . By an isotopy the number of arcs of intersection are reduced. Then is disjoint from . As is a torus knot, there are not essential tori in its complement. Then is contained in . By Lemma 2.6 this is not possible. ∎
3. Dehn surgery
.
Let be the knot or link defined in the previous section and let the band defined in Proposition 2.8. Let . Then is a 3-ball that intersects in two arcs. Let be the banding of , so is the trivial knot; intersects also in two arcs. Let be the complementary ball of in , and let , so consists of two arcs properly embedded in . That is, the pair can be considered as a 2-tangle, and the knots and can be considered as obtained by filling with rational tangles.
Let be the the double cover of branched along . As is a trivial knot, the double branched cover is the 3-sphere. Let . Then is a solid torus, its core is a knot in which we denote by . By Montesinos trick, the double branched cover of is then obtained by performing -Dehn surgery on for some integral slope ; this surgered manifold is denoted by . Let be the corresponding branched cover. Let , and let , and let . Note that because the winding number of in is an odd number, is then a single torus which is a double cover of . The torus intersects in two disks, which then implies that intersects in four disks. Then is a four-punctured torus properly embedded in the exterior of .
Lemma 3.1.
The decomposition of is given by , where is a hyperbolic manifold and is a Seifert fibered space.
Proof.
The manifold is the double cyclic cover of the exterior of the torus knot , and then by [11] is the Seifert fibered manifold .
If is not an hyperbolic manifold, then by Thurston Hyperbolicity Theorem, 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 which is equivariant, that is, , or , where is the involution defined on by the double branched cover. By taking the projection , there will be a compression disk for disjoint from , a meridian disk intersecting in one point, a decomposing sphere for , a meridian disk intersecting in two points, an essential annulus or Möbius band, or an essential torus or Conway sphere for . None of these can exist by Lemmas 2.1, 2.2, 2.5, 2.6 or 2.7,. ∎
Lemma 3.2.
The knot is hyperbolic.
Proof.
First note that cannot be a torus knot, for it has a Dehn surgery producing a 3-manifold containing a separating incompressible torus. Suppose is a satellite knot, and let be an incompressible torus in its exterior. As is strongly invertible, by the Equivariant Torus Theorem [8], there is an incompressible torus , which is equivariant under the involution defined on . bounds a solid torus which contains . The complement of may contain incompressible tori other than , but applying again the Equivariant Torus Theorem, there will be another equivariant torus in the complement of . Therefore we can assume that there is an equivariant torus , which defines then a companion knot for which is hyperbolic or a torus knot.
Suppose first that compresses after performing -Dehn surgery. Then by [5], is a 0 or 1-bridge braid in , with winding number . It follows from [6] that the manifold is obtained by -Dehn surgery on , for some integer . This is not possible if is a torus knot, for the surgery produces a 3-manifold containing a separating incompressible torus. Also, this is not possible if is an hyperbolic knot, because by [7], we should have .
So we have shown,
Teorema 3.3.
There is a family of hyperbolic strongly invertible knots , 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 can be generalized to , where , and are integers, such that is even and is odd. A pattern for the case is shown in Figure 5. In this case the wrapping number is . The proofs of Sections 2 and 3 would be identical for large subfamilies of these knots.
The examples can also be generalized when 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 in is even, and a new proof would have to be done. Also, when taking double branched covers in this case, the torus 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.

We finish with one question,
If is a satellite knot with satellite torus , and is a band that unknots , is there a universal bound for the minimal number of arcs of intersection between and ? Is this bound just two?
Acknowledgements. Research partially supported by grant PAPIIT-UNAM IN101317.
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