Every knot has characterising slopes

Let K be a knot in the 3-sphere. A slope p / q is said to be characterising for K if whenever p / q surgery on K is homeomorphic, via an orientation-preserving homeomorphism, to p / q surgery on another knot K′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$K'$$\end{document} in the 3-sphere, then K and K′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$K'$$\end{document} are isotopic. It was an old conjecture of Gordon, proved by Kronheimer, Mrowka, Ozsváth and Szabó, that every slope is characterising for the unknot. In this paper, we show that every knot K has infinitely many characterising slopes, confirming a conjecture of Baker and Motegi. In fact, p / q is characterising for K provided |p| is at most |q| and |q| is sufficiently large.


Introduction
Any closed orientable 3-manifold is obtained by Dehn surgery on a link in the 3sphere [19,32]. This surgery description of the manifold is known to be highly nonunique [15]. Nevertheless, if one restricts to knots, rather than links, and one considers only certain surgery slopes, then uniqueness results are a realistic goal. One way of formalising this is via the notion of a 'characterising slope' which is defined as follows.
For a knot K in S 3 , we let S 3 K ( p/q) denote the 3-manifold obtained by p/q Dehn surgery on K . A slope p/q is a characterising slope for K if whenever there is an orientation-preserving homeomorphism between S 3 K ( p/q) and S 3 K ( p/q) for some knot K in S 3 , then there is an orientation-preserving homeomorphism of S 3 taking K to K . (Recall that slopes on a boundary torus of the exterior of a link in the 3-sphere are parametrised by fractions p/q ∈ Q ∪ {∞}, where 1/0 = ∞ represents the meridian and 0/1 = 0 represents the longitude of the relevant link component. Throughout this paper the integers p and q will be assumed to be coprime.) Communicated  There has been considerable interest in characterising slopes over many years. A conjecture of Gordon [10], proved by Kronheimer, Mrowka, Ozsváth and Szabó [16], was that every slope is a characterising slope for the unknot. Using Heegaard Floer homology, this was extended to the figure-eight knot and the trefoil by Ozsváth and Szabó [24]. Then Ni and Zhang [23] showed that certain slopes are characterising slopes for the torus knot T 5,2 . This was developed by McCoy [20], who showed that every torus knot has characterising slopes; in fact, all but finitely many non-integral slopes are characterising for a torus knot. Ni and Zhang conjectured that, for any hyperbolic knot K , all but finitely many slopes are characterising for K . However, this was disproved by Baker and Motegi [2], who gave examples of hyperbolic knots (8 6 being the simplest) for which no integer slope is characterising. Baker and Motegi conjectured that, nevertheless, every knot has infinitely many characterising slopes. The main result of this paper is a proof of their conjecture. 3 . Then any slope p/q is characterising for K , provided | p| ≤ |q| and |q| is sufficiently large.

Theorem 1.1 Let K be a knot in S
Baker and Motegi also conjectured that for any hyperbolic knot K in S 3 , all but finitely many of its non-integral slopes are characterising. We cannot prove this, but we do achieve the following result.

Theorem 1.2 Let K be a hyperbolic knot in S 3 . Then any slope p/q is characterising for K provided that |q| is sufficiently large.
In the proof of both Theorems 1.1 and 1.2, one must consider not just the knot K but also another knot K . The argument works most efficiently when both K and K are hyperbolic, in which case we have the following stronger version of Theorem 1.2. 3 . Then there is a constant C(K ) with the following property. If there is an orientation-preserving homeomorphism between S 3 K ( p/q) and S 3 K ( p /q ) for some hyperbolic knot K in S 3 and |q | ≥ C(K ), then there is an orientation-preserving homeomorphism of S 3 taking K to K and p/q = p /q .

Theorem 1.3 Let K be a hyperbolic knot in S
A possible approach to Theorem 1.3 is to show that S 3 K ( p/q) 'remembers' the Dehn surgery in the following sense. By Thurston's hyperbolic Dehn surgery theorem [30], S 3 K ( p/q) is hyperbolic provided | p| + |q| is sufficiently large and moreover, the core of the surgery solid torus is the shortest geodesic in S 3 K ( p/q). Suppose the same is true of S 3 K ( p /q ) for some hyperbolic knot K in S 3 . By Mostow rigidity [21], the homeomorphism from S 3 K ( p/q) to S 3 K ( p /q ) is homotopic to an isometry, which must therefore take the shortest geodesic to the shortest geodesic. This therefore restricts to an orientation-preserving homeomorphism from S 3 − int(N (K )) to S 3 − int(N (K )) taking the slope p/q to the slope p /q . Using a theorem of Gordon and Luecke [11] (which is essentially that knots in the 3-sphere are determined by their complements), this homeomorphism takes the meridional slope on ∂ N (K ) to the meridional slope on ∂ N (K ), and hence extends to an orientation-preserving homeomorphism from S 3 to S 3 taking K to K . This sort of argument has been used before, for example by Bleiler, Hodgson and Weeks [5] and by Rieck and Yamashita [28]. They analysed the related concept of cosmetic surgeries, where there is an orientation-preserving homeomorphism between S 3 K ( p/q) and S 3 K ( p /q ) but p/q = p /q (and so the knot type is fixed but the slope can vary).
There is a significant difficulty with the line of argument presented in the previous paragraph. The core of the surgery solid torus is indeed the shortest geodesic in S 3 K ( p/q) when | p|+|q| is greater than some constant, but this constant depends on K .
We are also considering surgery along K and here the relevant constant depends on K . Thus, we cannot immediately deduce that any slope p/q is a characterising slope for K . Indeed, the examples due to Baker and Motegi [2] of hyperbolic knots with infinitely many non-characterising slopes highlight that this argument cannot be made to work in this form. Nevertheless, by delving deeper into the theory of hyperbolic 3-manifolds and Dehn surgery, it is possible to construct a proof of Theorem 1.3. The proof is given in Sect. 3, after the relevant background material on Dehn surgery has been collated in Sect. 2.
To prove Theorem 1.2, we must also consider the possibility that K is not hyperbolic. One would expect that S 3 K ( p /q ) is then non-hyperbolic for 'generic' slopes p /q . On the other hand, S 3 K ( p/q) is known to be hyperbolic for all but at most 10 slopes p/q, by work of the author and Meyerhoff [18]. Somewhat more pertinent to our analysis here is that S 3 K ( p/q) is hyperbolic when |q| ≥ 9, a result also proved in Lackenby and Meyerhoff [18]. However, it is in fact the case that S 3 K ( p /q ) might be hyperbolic for infinitely many slopes p /q , even without bound on |q |. A careful analysis of the JSJ decomposition for S 3 − int(N (K )) is required before Theorem 1.2 can be proved in this case. This is completed in Sect. 5, after a review of JSJ decompositions for knot exteriors is given in Sect. 4.
To prove Theorem 1.1, we must also establish that S 3 K ( p/q) 'remembers' the Dehn surgery when K is not hyperbolic. In the case where the JSJ piece of S 3 − int(N (K )) containing ∂ N (K ) is hyperbolic, the argument is again that this piece remains hyperbolic after Dehn surgery and the core of the attached solid torus is its shortest geodesic. But when the JSJ piece of S 3 − int(N (K )) containing ∂ N (K ) is non-hyperbolic, an alternative argument is required. This piece is Seifert fibred, and we show that the Seifert fibration extends over the attached solid torus. The core curve becomes an exceptional fibre and its singularity order (which is the number of times that the regular fibres wind around it) is the largest in the manifold. It is in this sense that the manifold 'remembers' the Dehn surgery. In order for this argument to work, we require here that | p| ≤ |q| and that |q| is sufficiently large. The proof is given in Sect. 6.
In this paper, all 3-manifolds will be oriented and connected. We use the symbol ∼ = to denote the existence of an orientation-preserving homeomorphism. Knots will not be oriented. We use (M, K ) denote a pair consisting of the oriented 3-manifold M and the unoriented knot K in M. Thus, (M, K ) ∼ = (M , K ) means that there is an orientationpreserving homeomorphism taking M to M and taking K to K , but with no regard to an orientation on K or K . We also use the terminology (M, K ) ∼ =∂ (M, K ) to denote the existence of an orientation-preserving homeomorphism of M that takes K to K and that equals the identity on ∂ M. More generally, if M and M are 3-manifolds and a homeomorphism between their boundaries has already been given, then we write M ∼ =∂ M to denote the existence of a homeomorphism between M and M that restricts to the given homeomorphism between ∂ M and ∂ M .
If σ is a slope on a toral boundary component of M, we let M(σ ) denote the manifold that is obtained by Dehn filling along it. If K is a knot in M and σ is a slope on ∂ N (K ), then the result of performing Dehn surgery along K using the slope σ is denoted M K (σ ).
We say that a compact orientable 3-manifold is hyperbolic if its interior admits a complete, finite-volume hyperbolic structure. We say that a knot K in a compact orientable 3-manifold M is hyperbolic if M − int(N (K )) is hyperbolic.

Background results on Dehn surgery
The following is a version of Thurston's hyperbolic Dehn surgery theorem. The usual version of the hyperbolic Dehn surgery theorem ( [30] or Theorem E.5.1 in [3]) asserts that there is a finite set of slopes on each component of ∂ X so that, as long as these slopes are avoided when Dehn filling is performed, the resulting manifold is hyperbolic. This is proved by perturbing the hyperbolic structure on X to form an incomplete hyperbolic structure, and then taking the metric completion. If the perturbation is chosen correctly, the points that are added in when forming the completion are a union of disjoint simple closed geodesics in the resulting hyperbolic manifold. One can check that for most filling slopes, these geodesics are very short. More precisely, if one chooses a basis for the first homology of each boundary torus so that slopes on the torus can be identified with fractions p/q ∈ Q ∪ {∞}, then the length of the corresponding geodesic is O((| p| 2 +|q| 2 ) −1 ), according to an analysis by Neumann and Zagier [22]. Thus, for all i sufficiently large, X (σ i 1 , . . . , σ i n ) is hyperbolic and the cores of the attached solid tori are all geodesics. Furthermore, these geodesics all have lengths that tend to zero as i → ∞. By the way that the hyperbolic structure on X (σ i 1 , . . . , σ i n ) is constructed, the hyperbolic manifolds X (σ i 1 , . . . , σ i n ) converge to X in the geometric topology (see Proposition E.6.29 in [3]). Hence, by Theorem E.2.4 in [3], provided is small enough, the -thick parts of X and X (σ i 1 , . . . , σ i n ) are homeomorphic for all sufficiently large i. We deduce that the -thin parts of these manifolds have the same number of components. We choose to be smaller than the length of any closed geodesic in X and smaller than the 3-dimensional Margulis constant. Therefore, the number of components of the -thin part of X is its number of cusps. We can easily observe this many components of the -thin part of X (σ i 1 , . . . , σ i n ): its cusps and the solid toral neighbourhoods of the surgery curves. Hence, this is precisely the -thin part of X (σ i 1 , . . . , σ i n ). Therefore, the only closed geodesics in X (σ i 1 , . . . , σ i n ) with length less than are powers of a core curve. Let N be any horoball neighbourhood of the cusps of X . This contains the δ-thin part of X for some is not quite a horoball neighbourhood of the cusps together with solid toral neighbourhoods of the core curves. But a minor adjustment to φ i can be made to achieve this, without modifying its bilipschitz constant too much. Hence, the final conclusion of the theorem can be achieved. See [3,30] for more details.
Jørgensen and Thurston analysed the space of hyperbolic 3-manifolds with a bound on their volume. Using the thick-thin decomposition of these manifolds, they were able to show the following (see [30] or Theorem E.4.8 in [3]).

Theorem 2.2 Let M i be a sequence of pairwise distinct, oriented hyperbolic 3manifolds with volume at most V . Then there is an oriented hyperbolic 3-manifold X with volume at most V and a collection T 1 , . . . , T n of toral boundary components of ∂ X with the following property. For some subsequence of the M i , there is a collection of slopes
In the theory of Dehn surgery, a key quantity that is considered is the distance (σ, σ ) between two slopes σ and σ on a torus. This is defined to be the modulus of the algebraic intersection number between curves representing σ and σ . A major theme is to produce upper bounds on (σ, σ ) when σ and σ are slopes on the same boundary torus of a hyperbolic 3-manifold such that Dehn filling along these slopes results in non-hyperbolic 3-manifolds.
An important geometric quantity associated with any slope on the boundary of a hyperbolic 3-manifold is its 'length' which is defined as follows. Let M be a compact orientable 3-manifold with interior that admits a complete, finite-volume hyperbolic metric and let N be a horoball neighbourhood of its cusps. Then the tori ∂ N inherit a Euclidean metric. The length of a slope σ on ∂ M is the shortest curve on ∂ N with slope σ . Note that the length depends on the choice of horoball neighbourhood N . It is usually advantageous to take N to be as large as possible, and so one often considers a maximal horoball neighbourhood of its cusps, which is by definition an open horoball neighbourhood that is not contained in a larger one. Then ∂ N does not form a union of disjoint embedded tori. Instead, these are immersed tori, but they still inherit a Euclidean metric, and so one can still use N to define the length of any slope on ∂ M.
The relevance of slope length was first made apparent by work of Gromov and Thurston, who proved that if (σ 1 , . . . , σ n ) is a collection of slopes on distinct boundary components of M and there is a horoball neighbourhood of the cusps with respect to which each σ i has length more than 2π , then M(σ 1 , . . . , σ n ) admits a negatively curved Riemannian metric [4]. As a consequence of Perelman's proof of the geometrisation conjecture [25][26][27], such a manifold is now also known to be hyperbolic. The constant 2π was reduced to 6 by the author [17] and Agol [1]. At the time, the conclusion on M(σ 1 , . . . , σ n ) was somewhat weaker, but again as a consequence of geometrisation, M(σ 1 , . . . , σ n ) is now known to be hyperbolic if each σ i has length more than 6.
The following result relates slope length to the distance between slopes.

Theorem 2.3 Let M be a compact orientable non-hyperbolic 3-manifold, and let K be a hyperbolic knot in M. Let N be a maximal horoball neighbourhood in M
where μ is the meridional slope on ∂ N (K ).
This was essentially proved in Corollary 2.4 of [7], but there the constant was ( √ 3/2π) rather than ( √ 3/6). The improvement in the constant is due to the use of the 6-theorem rather than the Gromov-Thurston 2π theorem.
The first inequality in the following theorem was proved by Futer, Kalfagianni and Purcell [8]. A similar result was proved by Cooper and the author [7] but with less explicit estimates. The second inequality is due to Thurston [30]. Theorem 2.4 Let X be a compact orientable hyperbolic 3-manifold with boundary a non-empty collection of tori. Let T 1 , . . . , T n be toral boundary components of ∂ X where n > 0. Let (σ 1 , . . . , σ n ) be a collection of slopes, where σ j lies on T j . Suppose that there is a horoball neighbourhood of the cusps of X on which each σ j has length at least min > 2π . Then X (σ 1 , . . . , σ n ) is a hyperbolic manifold satisfying The version of the above theorem in [7] was a crucial step in the proof of the following result of Cooper and the author (Theorem 4.1 in [7]).

Theorem 2.5
Let M be a compact orientable 3-manifold with boundary a (possibly empty) union of tori. Let > 0. Then there are only finitely many compact orientable hyperbolic 3-manifolds X and slopes σ 1 , . . . , σ n on distinct components of ∂ X such that M ∼ = X (σ 1 , . . . , σ n ) and where the length of each σ i is at least 2π + , when measured using some horoball neighbourhood of the cusps of X .
The following is due to Lackenby and Meyerhoff [18]. Theorem 2.6 Let K be a hyperbolic knot in S 3 . Then S 3 K ( p/q) is also hyperbolic if |q| ≥ 9. Theorem 1.2 in [18] states that if a 1-cusped hyperbolic 3-manifold is Dehn filled in two different ways and the resulting manifolds are not hyperbolic, then the distance between the two surgery slopes is at most 8. Theorem 2.6 follows since S 3 K (∞) = S 3 is not hyperbolic and |q| = ( p/q, ∞).
The following is due to Gordon and Luecke [12].
The following result generalises the above two theorems from the exterior of a knot in the 3-sphere to knot exteriors in certain other 3-manifolds.

Theorem 2.8 Let M be the exterior of the unlink or unknot in S 3 , and let K be a hyperbolic knot in M. Then M K ( p/q) is irreducible and has incompressible boundary
Proof The manifold M K (∞) = M has compressible boundary. By Thurston's geometrisation theorem [31], M K ( p/q) is hyperbolic provided it contains no essential disc, sphere, annulus or torus, since its boundary is a non-empty union of tori. In the case where M K ( p/q) has an essential disc, |q| = ( p/q, ∞) ≤ 1 by a theorem of Wu [33]. When M K ( p/q) has an essential sphere, |q| = ( p/q, ∞) = 0, by a theorem of Scharlemann [29]. If M K ( p/q) has an essential annulus, then |q| = ( p/q, ∞) ≤ 2 by a result of Gordon and Wu [14]. When M K ( p/q) has an essential torus, |q| = ( p/q, ∞) ≤ 2 by Gordon and Luecke [13].
Gordon and Luecke [11] proved that knots in the 3-sphere are determined by their complements. Specifically, any homeomorphism between S 3 − int(N (K )) and S 3 − int(N (K )) for non-trivial knots K and K in S 3 must send meridians to meridians. The following generalises this to knot exteriors in some other 3-manifolds.  N (K )) sends the meridional slope on ∂ N (K ) to some slope σ on ∂ N (K ). We want to show that σ is the meridional slope μ on ∂ N (K ).
When M is the exterior of the unlink with at least two components, the deduction that σ = μ follows from a theorem of Scharlemann [29]. This is because M K (μ) = M has compressible boundary, whereas M K (σ ) ∼ = M has a reducing sphere.
Suppose that M is the exterior of the unknot. Suppose that σ = μ. Then nontrivial surgery on the knot K in the solid torus M yields the solid torus. Note also that M − int(N (K )) is irreducible. Gabai [9] showed that such knots K have to be 1-bridge braids, and in particular must have non-zero winding number in M. Now the homeomorphism M K (σ ) ∼ = M is assumed to be equal to the identity on ∂ M. In particular, the slopes on ∂ M that bound discs in M and M K (σ ) are equal. On the other hand, for simple homological reasons, when non-trivial surgery along a knot in the solid torus M with non-zero winding number is performed, the slopes on ∂ M that are homologically trivial before and after the surgery are distinct. This is a contradiction, and hence σ = μ.

The case where both knots are hyperbolic
In this section, we prove the following generalisation of Theorem 1.3. This not only deals with knots in the 3-sphere, but also knots in the exterior of the unknot or unlink. This extra level of generality will be useful when handling non-hyperbolic knots in later sections.
Suppose first that the manifolds M − int(N (K i )) run over infinitely many distinct homeomorphism types. Then we may pass to a subsequence where they are pairwise distinct. By Theorem 2.3, the length of p i /q i tends to infinity and hence is larger than 4π for sufficiently large i. So by Theorem 2.4, the hyperbolic volume of M − int(N (K i )) is at most (4/3) 3/2 times that of M K i ( p i /q i ). We are assuming that M K i ( p i /q i ) is homeomorphic to M K ( p i /q i ) and hence they have equal volume. Since hyperbolic volume goes down when Dehn filling is performed, the volume of M K ( p i /q i ) is less than that of M − int(N (K )). So, if we set V to be (4/3) 3/2 times the volume of M − int(N (K )), then the volume of M − int(N (K i )) is at most V . By Theorem 2.2, there is an oriented hyperbolic 3-manifold X with volume at most V and a collection T 1 , . . . , T n of toral boundary components of ∂ X with the following property. For some subsequence of the K i , there is a collection of slopes We now consider the possibility that the manifolds M − int(N (K i )) run over only finitely many homeomorphism types. We may then pass to a subsequence where they are a single oriented manifold X . So, in all cases, M K i ( p i /q i ) ∼ = X (σ i 1 , . . . , σ i n , σ i ), for some slope σ i on ∂ X − (T 1 ∪ · · · ∪ T n ), but we allow the possibility that n = 0.
By Theorem 2.1, there is a horoball neighbourhood N of the cusps of X and subsets N i of M − int(N (K i )) consisting of horoball neighbourhoods of the cusps and solid toral neighbourhoods of the surgery curves, so that the inclusion X − N → (M − int(N (K i ))) − N i has bilipschitz constant that tends to 1 as i → ∞. So the length of σ i as measured in X tends to infinity as i → ∞ because the length of p i /q i tends to infinity. We may therefore pass to a subsequence where the slopes σ i represent pairwise distinct slopes on ∂ X . By Theorem 2.1, the core curves in X (σ i 1 , . . . , σ i n , σ i ) are geodesics when i is sufficiently large, with lengths that tend to zero. Similarly, applying Theorem 2.1 again, there is some > 0 such that the only geodesic in M K ( p/q) with length less than is the core curve, provided | p| + |q| is greater than some constant c. There are only finitely many slopes with | p| + |q| ≤ c, and for each of these slopes p/q that give hyperbolic fillings, we can compute the length of the shortest geodesic of the resulting manifold. If set to be less than this length, we deduce that whenever M K ( p i /q i ) is hyperbolic, there is at most one geodesic in M K ( p i /q i ) with length less than and if there is such a geodesic, then it is the core curve. Now, when i sufficiently large, there are n + 1 geodesics in X (σ i 1 , . . . , σ i n , σ i ) with length less than . This is a contradiction unless n = 0. Thus, M − int(N (K i )) is homeomorphic to a fixed oriented hyperbolic manifold X . The homeomorphism

The JSJ decomposition of knot exteriors
In this section, we recall some details about the JSJ decomposition for a knot exterior. A torus properly embedded in a compact orientable irreducible 3-manifold M is essential if it is incompressible and not boundary parallel. A properly embedded torus is a JSJ torus if it is essential and, moreover, any essential torus can be ambient isotoped off it. The JSJ decomposition for M consists of one copy, up to ambient isotopy, of each JSJ torus. The JSJ tori can be made simultaneously disjoint, and so the JSJ decomposition is a union of disjoint essential tori. When M has boundary a (possibly empty) union of tori, the complement of an open regular neighbourhood of the JSJ tori consists of 3-manifolds that are either Seifert fibred or hyperbolic. Each component of this 3-manifold is called a JSJ piece.
When the exterior of a knot K in S 3 has no JSJ tori, it is hyperbolic or Seifert fibred. The latter case arises exactly when K is the unknot or a torus knot. Thus, we focus on the situation where S 3 − int(N (K )) has at least one JSJ torus. This was analysed in detail by Budney [6]. The following summarises some of Theorem 4.18 in [6].

Theorem 4.1 Let K be a knot in S 3 such that S 3 − int(N (K )) has at least one JSJ torus. Then any JSJ piece has one of the following forms:
(1) a Seifert fibre space with base space an annulus and with one exceptional fibre; (2)

a Seifert fibre space with base a planar surface with at least three boundary components and no exceptional fibres; (3) a hyperbolic 3-manifold that is homeomorphic to the exterior of a hyperbolic link L in S 3 such that when one specific component of L is removed, the result is the unlink; (4) the exterior of a torus knot in the 3-sphere.
The Seifert fibre spaces in Case (1) are called cable spaces. One way in which they arise is when a knot K is a cable of a knot K , as follows. Let K be a knot in S 3 , and let N (K ) be a solid torus regular neighbourhood of K . Then K is a cable of K if it lies on ∂ N (K ) and the modulus of its winding number in N (K ) is at least two. More precisely, we say that it is the (r , s)-cable of K if its slope on ∂ N (K ) is r /s. The exterior of K then contains a cable space. For if we isotope K a little into N (K ), then the result of removing a small open regular neighbourhood of K from N (K ) is a cable space. The core curve of N (K ) is the exceptional fibre, with singularity order |s|.
When there is a sequence of knots K = K 1 , . . . , K n = K such that each K i+1 is a cable of K i , we say that K is an iterated cable of K .
It is also worth recording the following extension of Theorem 4.1 when the JSJ piece contains ∂ N (K ). Proof Most of this is contained in Theorem 4.18 of [6]. Case (1) of Theorem 4.1 corresponds to conclusion (1)(b) of Theorem 4.18 in [6]. There, the statement is that K is obtained by 'splicing' a non-trivial knot K with a 'Seifert link' S ( p,q) . This is just the assertion that K is the (q, p) cable of K . (See Definition 4.8 in [6] for the definition of splicing.) Case (2) of Theorem 4.1 corresponds to conclusion 1(c) of Theorem 4.18 in [6]. In this case, K is obtained by splicing some non-trivial knots with a 'key-chain link'. This gives that K is a connected sum of these knots. The complement of the key-chain link is the product of a planar surface P and the circle S 1 . The splicing construction gives that the fibres of the Seifert fibration, which are of the form { * } × S 1 , form meridians on ∂ N (K ). (3) are essentially contained in [6]. When the component of L corresponding to ∂ N (K ) is removed, the result is the unknot or unlink; this is contained in the definition of a 'KGL' in [6]. The assertion about slopes in (3) follows from the definition of 'splicing' in [6], as demonstrated in Example 4.9 in [6]. Note that we parametrise slopes on each boundary component of the JSJ piece of S 3 − int(N (K )) by observing that this torus separates S 3 into a solid torus containing K and the exterior of a non-trivial knot. On the boundary of the non-trivial knot exterior, there is a canonical longitude and meridian, and hence a canonical fraction p/q ∈ Q ∪ {∞} for each slope.

The claims in Case
Note that Case (4) of Theorem 4.1 does not arise because we are assuming that S 3 − int(N (K )) has at least one JSJ torus and hence is not a torus knot exterior.

Hyperbolic fillings on non-hyperbolic knots
It is a major theme in surgery theory that many properties of a 3-manifold with toral boundary are preserved when a boundary component is Dehn filled along a 'generic' slope. So one might expect that if K is a non-hyperbolic knot in S 3 , then S 3 K ( p/q) is also non-hyperbolic if |q| is greater than some universal constant. Slightly surprisingly, this is not true, but we can analyse precisely when this phenomenon arises.

Theorem 5.1 Let K be a non-hyperbolic knot in S 3 . Suppose that S 3 K ( p/q) is hyperbolic for |q| ≥ 2. Then K is an iterated cable of a hyperbolic knot K and S 3
K ( p/q) ∼ = S 3 K ( p /q ) for some slope p /q where |q| < |q | and |q| divides |q |.
The following result goes some way to proving Theorem 5.1.

Proposition 5.2 Let K be a non-hyperbolic knot in S 3 other than the unknot. Suppose that S 3 K ( p/q) does not contain an incompressible torus and that |q| ≥ 2. Then K is a cable of a knot K .
Proof Let X be the JSJ piece of S 3 − int(N (K )) adjacent to ∂ N (K ). If X is all of S 3 − int(N (K )), then K is a torus knot, which is a cable of the unknot. So, we may assume that S 3 − int(N (K )) contains at least one JSJ torus. The possibilities for X are given in Theorem 4.2.
Suppose that X is the exterior of a hyperbolic knot in M, where M is the exterior of the unknot or unlink in S 3 . By Theorem 2.8, X ( p/q) is irreducible and has incompressible boundary, since |q| ≥ 2. Thus, S 3 K ( p/q) contains an incompressible torus, contrary to hypothesis.
Suppose that X is homeomorphic to P × S 1 for a planar surface P with at least three boundary components, and that curves of the form { * } × S 1 on ∂ N (K ) are meridians. So when we Dehn fill ∂ N (K ) along a non-meridional slope, the Seifert fibration on P × S 1 extends over the attached solid torus. Hence, the boundary tori of this filled-in piece are still incompressible, contrary to our hypothesis.
The only remaining possibility is that X is Seifert fibred with base space an annulus and with one exceptional fibre. Then, K is a cable of a knot K .
Then an analysis of surgery along cabled knots gives the following.
is a cable of a knot K . Note that K cannot be the unknot, because then K would be a torus knot and hence S 3 K ( p/q) could not be hyperbolic. By Proposition 5.3 and the assumption that S 3 K ( p/q) is hyperbolic, S 3 K ( p/q) ∼ = S 3 K ( p /q ) for some slope p /q , where |q| < |q | and |q| divides |q |. If K is hyperbolic, the theorem is proved. Therefore, suppose that K is not hyperbolic. By induction, K is an iterated cable of a hyperbolic knot K and S 3 K ( p /q ) ∼ = S 3 K ( p /q ) where |q | < |q | and |q | divides |q |. So, K is an iterated cable of K and S 3 K ( p/q) ∼ = S 3 K ( p /q ) where |q| < |q | and |q| divides |q |.
We are now in a position to prove Theorem 1.2.
Proof of Theorem 1.2. Let K be a hyperbolic knot. Let C(K ) be the constant from Theorem 1.3. We show that any slope p/q is characterising for K , provided that |q| ≥ max{C(K ), 9}.
Let K be a knot in S 3 such that S 3 K ( p/q) ∼ = S 3 K ( p/q). If K is hyperbolic, then by Theorem 1.3, (S 3 , K ) ∼ = (S 3 , K ) and the theorem is proved. So, suppose K is not hyperbolic. By Theorem 2.6, S 3 K ( p/q) is hyperbolic since |q| ≥ 9. By Theorem 5.1, K is an iterated cable of a hyperbolic knot K and and p/q = p /q , using Theorem 1.3. In particular, |q| = |q |, which contradicts our earlier conclusion that |q| < |q |.

Proof of the main theorem
In this section, we complete the proof of Theorem 1.1. Since Theorem 1.2 was proved in the last section, we must focus on the case where K is not hyperbolic. Our first result deals with the relationship between the JSJ decompositions of S 3 − int(N (K )) and S 3 K ( p/q) for suitable slopes p/q. Theorem 6.1 Let K be a knot in S 3 . Suppose that |q| ≥ 9. In the case where K is a torus knot or a cable knot, suppose also that | p| ≤ |q|. Then S 3 K ( p/q) is irreducible and the JSJ tori for S 3 −int(N (K )) form the JSJ tori for S 3 K ( p/q). Moreover, if the JSJ piece of S 3 −int(N (K )) containing ∂ N (K ) is hyperbolic, then so is the corresponding piece in S 3 K ( p/q). If the JSJ piece of S 3 − int(N (K )) containing ∂ N (K ) is Seifert fibred, then so is the corresponding piece in S 3 K ( p/q) and the core of the attached solid torus is an exceptional fibre with singularity order at least |q|.
Proof Let Y be the JSJ piece for S 3 − int(N (K )) that contains ∂ N (K ). We will show that if Y is hyperbolic, then Y ( p/q) is too. We will also show that if Y is Seifert fibred, then this extends to a Seifert fibration for Y ( p/q) in which the core of the surgery solid torus is an exceptional fibre with singularity order at least |q|. In both cases, we deduce that Y ( p/q) has incompressible boundary and is not a copy of T 2 × I . This will prove the theorem. This is because the JSJ tori for S 3 − int(N (K )) form a decomposition of S 3 K ( p/q) into pieces with incompressible boundary, that are either hyperbolic or Seifert fibred and not T 2 × I , and when two Seifert fibred pieces meet along a torus, then their Seifert fibrations are not isotopic on this torus. This is enough to deduce that these tori are the JSJ tori for S 3 K ( p/q) and that S 3 Suppose first that Y is hyperbolic. Then by Theorem 4.2, Y is homeomorphic to the exterior of a hyperbolic link L in S 3 , with the property that when the component of L corresponding to ∂ N (K ) is removed, the result is the unlink, the unknot or the empty set. Furthermore, the homeomorphism Y → S 3 − int(N (L)) takes the slope p/q on ∂ N (K ) to the slope p/q on the relevant component of ∂ N (L). By Theorem 2.6 or 2.8, Y ( p/q) is hyperbolic if |q| ≥ 9.
Suppose now that Y is Seifert fibred. If Y has more than two boundary components, then by Theorem 4.2, it is of the form P × S 1 for a planar surface P and the slope of the fibres on ∂ N (K ) is meridional. Hence, if p/q surgery is performed and q = 0, then the Seifert fibration extends over the solid torus. Moreover, if |q| ≥ 2, then the core of the solid torus becomes an exceptional fibre with order |q|, as required.
Consider now the case when Y is Seifert fibred with two boundary components. Then Y is a cable space and K is an (r , s)-cable of a non-trivial knot. The slope of the regular fibre is rs on ∂ N (K ). The distance between it and p/q is |qrs − p|. Note that where the inequality follows from the fact that |rs| ≥ 2 and | p/q| ≤ 1. We are assuming that |q| ≥ 2. Hence, we deduce that the Seifert fibration of Y extends to Y ( p/q), and the core of the attached solid torus becomes an exceptional fibre with singularity order at least |q|, again as required.
Suppose now that Y is Seifert fibred with a single boundary component. Then Y is the exterior of an (r , s) torus knot. Its Seifert fibration extends over the attached solid torus, as long as the surgery slope is not equal to that of the regular fibre, which is the integer rs. As in the case of the cable space, the distance between p/q and rs is at least |q| and hence again the core of the attached solid torus becomes an exceptional fibre with singularity order at least |q|.
Proof of Theorem 1.1. Let K be a knot in S 3 . If K is the unknot, then Theorem 1.1 follows from the main theorem of [16] by Kronheimer, Mrowka, Ozsváth and Szabó. If K is hyperbolic, then Theorem 1.1 follows from Theorem 1.2, which we proved in the previous section. If K is a torus knot, then it is a theorem of McCoy [20] that every non-integral slope, with at most finitely many exceptions, is characterising for K . So suppose that S 3 − int(N (K )) contains at least one JSJ torus, and let Y be the JSJ piece containing ∂ N (K ). Let K be another knot in S 3 and let Y be the JSJ piece of S 3 − int(N (K )) containing ∂ N (K ).
Suppose that S 3 K ( p/q) ∼ = S 3 K ( p/q) for some slope p/q where | p| ≤ |q| and |q| is larger than some constant that depends on K , and which is to be determined. We will initially assume that |q| ≥ 9 so that Theorem 6.1 applies. So, S 3 K ( p/q) is irreducible and the JSJ tori for S 3 − int(N (K )) form the JSJ tori for S 3 K ( p/q). Theorem 6.1 also applies to K and hence the JSJ tori for S 3 −int(N (K )) form the JSJ tori for S 3 K ( p/q). The homeomorphism S 3 K ( p/q) ∼ = S 3 K ( p/q) takes JSJ tori to JSJ tori, after possibly applying an isotopy. (This isotopy may move the surgery curves in the manifold.) Case 1. Y is Seifert fibred.
If |q| is sufficiently large, then by Theorem 6.1, Y ( p/q) is Seifert fibred and the core of the surgery solid torus in Y ( p/q) is an exceptional fibre with singularity order that is greater than that of any exceptional fibre in any Seifert fibred JSJ piece of S 3 − int(N (K )). Hence, the homeomorphism S 3 K ( p/q) ∼ = S 3 K ( p/q) must take this exceptional fibre to the core of the surgery solid torus in S 3 K ( p/q). Thus, it restricts to S 3 − int(N (K )) ∼ = S 3 − int(N (K )) taking the slope p/q to p/q. It also takes meridians to meridians, by the theorem of Gordon and Luecke [11]. Hence, it extends to (S 3 , K ) ∼ = (S 3 , K ), as required.
Case 2. Y is hyperbolic.
By Theorem 4.2, there is a homeomorphism Y → S 3 − int(N (L )) for some hyperbolic link L . Furthermore, if the component of L corresponding to ∂ N (K ) is removed, the result is the unknot or unlink. The homeomorphism sends the slope p/q on ∂ N (K ) to the slope p/q on the relevant component of ∂ N (L ).
We claim that the homeomorphism S 3 K ( p/q) ∼ = S 3 K ( p/q) takes the JSJ piece in S 3 K ( p/q) containing the surgery curve to the JSJ piece in S 3 K ( p/q) containing the surgery curve, provided that |q| is greater than some constant that depends on K . If not, then Y ( p/q) is homeomorphic to a JSJ piece X for S 3 −int(N (K )) not containing ∂ N (K ). Now, S 3 − int(N (K )) has only finitely many JSJ pieces. By Theorem 2.5, for each such piece X and each > 0, there are only finitely many hyperbolic 3manifolds Y and slopes σ on Y with length at least 2π + such that Y (σ ) ∼ = X . Now the length of p/q on Y is at least ( √ 3/6)|q| > 2π if |q| ≥ 22, by Theorem 2.3. Thus, by choosing p/q to avoid finitely many values and so that |q| ≥ 22, we can arrange that Y ( p/q) X for any JSJ piece X of S 3 − int (N (K )). This proves the claim.
Thus the homeomorphism S 3 K ( p/q) ∼ = S 3 K ( p/q) restricts to a homeomorphism Y ( p/q) ∼ = Y ( p/q). It also restricts to a homeomorphism h : . Let Z and Z denote these manifolds.
Note that each boundary component of Z is a torus in S 3 , which therefore bounds a solid torus on at least one side. The solid torus must contain K , since its boundary torus is incompressible in S 3 − int(N (K )). The same argument gives that, on the other side of the torus, there is the exterior of a non-trivial knot. Thus, each component of Z is homeomorphic to the exterior of a non-trivial knot in S 3 . The same is true of each component of Z . Hence, the homeomorphism h : Z → Z must send meridians to meridians by [11]. It must also send longitudes to longitudes for homological reasons. Since it is orientation-preserving, it must therefore send each slope r /s on each boundary component to the slope r /s on the image boundary component. We say that such a homeomorphism is slope-preserving. This restricts to a homeomorphism h|∂ Z from the boundary of Y ( p/q) to the boundary of Y ( p/q). Now, Y ( p/q) is hyperbolic by Theorem 6.1. Thus, Y ( p/q) is also, and hence so is Y by Theorem 6.1. So by Theorem 4.2, Y is homeomorphic to the exterior of a hyperbolic knot K * in M, where M is the exterior of the unknot or unlink in S 3 . The homeomorphism takes ∂ N (K ) to ∂ N (K * ) and sends each slope r /s on ∂ N (K ) to r /s on ∂ N (K * ). On the remaining components of ∂Y , the homeomorphism sends each slope r /s to the slope s/r on the relevant component of ∂ M. Similarly, Y is homeomorphic to the exterior of a hyperbolic knot K * in M, and the homeomorphism has the same effect on slopes as was the case with Y . We obtain an induced homeomorphism ∂ M → ∂ M as follows. We have a homeomorphism M −int(N (K * )) → Y which restricts to a home-omorphism ∂ M → ∂Y − ∂ N (K ). There is a homeomorphism Y ( p/q) → Y ( p/q) which restricts to a homeomorphism ∂Y − ∂ N (K ) → ∂Y − ∂ N (K ). And then there is a homeomorphism ∂Y −∂ N (K ) → ∂ M. We observe that this is a slope-preserving homeomorphism ∂ M → ∂ M. We can ensure that this is actually equal to the identity on ∂ M by possibly changing the knot K * , as follows. There is a homeomorphism M → M that achieves any given permutation of its boundary components, since one may permute the components of an unlink in any way by an isotopy of the 3-sphere. There is also a homeomorphism M → M which acts as −id on one component of ∂ M and acts as the identity on the remaining components. This is achieved by an isotopy of the 3-sphere, which moves one component of the unlink back to itself but reversing its orientation. By applying such homeomorphisms of M to itself, we take K * to another knot K * , but now the relevant homeomorphism ∂ M → ∂ M is the identity. In other words, M K * ( p/q) ∼ =∂ M K * ( p/q). So, by Theorem 3.1, if |q| is sufficiently large, (M, K * ) ∼ =∂ (M, K * ). This gives a homeomorphism S 3 − int(Z ) → S 3 − int(Z ) taking K to K , and that equals h on its boundary. This extends to a homeomorphism (S 3 , K ) ∼ = (S 3 , K ) using the homeomorphism h : Z → Z .
We note that the same argument gives the somewhat stronger, albeit less catchy, version of Theorem 1.1.

Theorem 6.2 Let K be a knot in S 3 . Then the slope p/q is characterising for K provided that
|q| min |( p/q) − n| : n ∈ Z\{−1, 0, 1} is sufficiently large.
In Theorem 1.1, we required that | p/q| ≤ 1, whereas in Theorem 6.2, we only require that, in some sense, p/q is not too close to any integer in Z\{−1, 0, 1}.
There is only one step in the proof where the hypothesis that | p| ≤ |q| is used. It is in the proof of Theorem 6.1, when the JSJ piece of S 3 − int(N (K )) containing ∂ N (K ) is Seifert fibred. The conclusion there is that this Seifert fibration extends over the surgery solid torus, with the core being a singular fibre with singularity order at least |q|. However, all one really needs is that this singularity order is at least some function f ( p/q) where f is independent of K and that, for certain values of p/q, this function f ( p/q) is large. Examining the proof of Theorem 6.1, we see that the singularity order is |qrs − p| for suitable coprime integers r and s where |rs| ≥ 2. Note that |qrs − p| = |q||rs − ( p/q)| ≥ |q| min |( p/q) − n| : n ∈ Z\{−1, 0, 1} .
Hence if the latter quantity is large, then so is the order of the singular fibre. The proof of Theorem 1.1 can then be readily adapted to establish Theorem 6.2.
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