Twist spun knots of twist spun knots of classical knots
Abstract.
A -twist spun knot is an -dimensional knot in the -dimensional sphere which is obtained from an -dimensional knot in the -dimensional sphere by applying an operation called a -twist-spinning. This construction was introduced by Zeeman in 1965. In this paper, we show that the -twist-spinning of the -twist-spinning of a classical knot is a trivial -knot in if . We also give a sufficient condition for the -twist-spinning of the -twist-spinning of a classical knot to be non-trivial.
1. Introduction
To study fibered links in higher dimensional spheres geometrically, one idea is to relate them to lower dimensional fibered links. In singularity theory, a cyclic suspension, or more generally the Thom-Sebastiani construction, is quite common. It enables us to study the Milnor fibration of the singularity of a polynomial map at the origin in the form , , by using the Milnor fiberation of the lower dimensional singularity . A topological construction of the cyclic suspension is studied by Kauffman in [13]. His construction can be applied for simple fibered links in the odd dimensional spheres. The fibered knot in obtained by a cyclic suspension is a cyclic branched cover of along the lower dimensional fibered knot and the fiber surface is obtained correspondingly. The monodromy matrix is obtained from the monodromy matrix of the lower one by taking a certain tensor product.
In the study on higher dimensional knots, in 1965, Zeeman introduced a way of constructing an -dimensional knot in from an -dimensional knot in for [19]. This construction is called a -twist-spinning. The knot in obtained from a knot in by the -twist-spinning is called a -twist spun knot of . If , then a -twist spun knot is a fibered knot and the fiber surface is the -fold cyclic branched cover of along with removing one open ball. Moreover, the monodromy is periodic, shifting the sheets of the cyclic branched cover by . Properties of fibered knots obtained by a cyclic suspension and a -twist-spinning are similar, though no relations between them are known yet.
Recently, the authors studied a more general class of -twist spun knots in called a branched twist spin, and proved that, in most cases, branched twist spins are equivalent if and only if the corresponding -dimensional knots in are equivalent [8]. Here two knots and are said to be equivalent if there exists a diffeomorphism from the sphere containing to the sphere containing satisfying . The key observation in that paper is that the quotient group of the fundamental group of the complement of a branched twist spin of a -dimensional knot in by its center is isomorphic to the fundamental group of the -orbifold of cyclic type with underlying space and ramification locus of order in most cases.
In this paper, we study a twist spun knot of a twist spun knot. Let and be positive integers and be the -twist spun knot of the -twist spun knot of a knot in , which is a -knot in .
Theorem 1.1.
If either is trivial or , then is trivial.
It is shown in [8, Proposition 3.2] that if is non-trivial and , then is a non-trivial -knot in . Theorem 1.1 means that even if is non-trivial, becomes trivial if . We do not know if the same observation works for higher dimensional cases, see Remark 3.3.
The converse of the assertion in Theorem 1.1 holds under a certain condition.
Theorem 1.2.
Set . If is non-trivial, , and the center of is trivial, then is non-trivial.
Note that if is a non-trivial and non-torus knot and the -fold cyclic branched cover of along is aspherical, then the center of is trivial. See the first half of the proof of [8, Lemma 3.1]. For example, if is a hyperbolic knot with or a prime satellite knot with , then the center of is trivial. We will prove in Theorem 4.1 that if is a -torus knot and does not divide then the center of is non-trivial.
The authors would like to thank Makoto Sakuma for helpful suggestions. The second author would like to thank the organizers of the International Conference ”Singularities and Algebraic Geometry” Tuy Hoa 2024 for their kind hospitality and the organization of the excellent conference. The second author is supported by JSPS KAKENHI Grant Numbers JP23K03098 and JP23H00081, and JSPS-VAST Joint Research Program, Grant number JPJSBP120219602.
2. -twist-spinning and branched twist spin
In this section, we introduce the -twist-spinning of an -dimensional knot in and a branched twist spin in . An -dimensional knot (or -knot for short) is the image of an embedding of into . Throughout this paper, denotes the interior of a topological space , denotes the boundary of , and denotes a compact tubular neighborhood of a topological space embedded in .
2.1. -twist-spinning
Let be an -knot. Choose a point in and a coordinate neighborhood such that and . Let be the unit ball in and set and . The pair is an unknotted -ball in the -ball. Let be the closure of and be the closure of . If is not trivial, then is a knotted -ball relatively embedded in the -ball . Gluing and by the identity map from to , we recover the -knot in . See Figure 1.

Now set and , where is the unit disk in . Let denote the coordinate of and denote the angular coordinate of . Hence is equipped with the coordinates , where we think that the angle is not defined if . Then we glue and by the diffeomorphism defined by
(2.1) |
where , and . The union is the pair of the boundaries of and , which is the pair of and an -knot in . This -knot is called the -twist spun knot of . We denote it as . Note that the above definition of works even if is negative. In this paper, we always assume that by reversing the orientation of if necessary.
For a -knot , a presentation of can be obtained easily, see for example [16, 19]. Applying the same argument in these references to , we obtain the following presentation.
Lemma 2.1.
Let be a presentation of with generators and relators . Then
where is a meridian of in . In particular, and .
Proof.
The complement is the union of and . Since is unknotted, is homotopic to . Note that this homotopy is given by the deformation retract from to the equator of the -sphere shown on the left in Figure 2. Hence is homotopic to a manifold obtained from by attaching . In particular, we have
where .

The gluing map of to is defined by (2.1). Setting the coordinates on as , we have
Let be a loop given by , which coincides with the loop . This loop commutes any elements in and . Therefore, it commutes any elements in . This loop is parametrized by in .
Let denote a loop in given by the parameter . This loop is a meridian of in , which can be seen from the figure on the left in Figure 2. Since is parametrized by , its image in rotates times along and once along . Since is null-homotopic in , we have . Thus the presentation of in the assertion is obtained.
If then the meridian is in the center of . We can choose the generators of to be conjugate to (cf. [12]). Since is isomorphic to , is the infinite cyclic group generated by .
The assertion in the case is obtained from the presentation of immediately. ∎
Theorem 2.2 (Zeeman [19]).
If then there exists a locally trivial fibration
The fiber is diffeomorphic to the -fold cyclic branched cover of along with removing an open ball and the monodromy is periodic, shifting the sheets of the cyclic branched cover by .
Remark 2.3.
If , then the fiber is diffeomorphic to the -dimensional unit ball. Therefore, is a trivial -knot in .
2.2. Branched twist spin
Circle actions on homotopy -spheres are classified by Montgomery and Yang [14] and Fintushel [3], and later, Pao proved in [15] that such homotopy -spheres are the standard -sphere . A -sphere embedded in that is invariant under a circle action is called a branched twist spin (cf. [10, §16.3]). A branched twist spin is obtained from a knot in by “twisting”, like a -twist-spinning, but the “twisting” for a branched twist spin is defined by two integers and , where is either a pair of coprime integers in or . We may assume that by reversing the orientation of if necessary. In this paper, since we study branched twist spins without fixing the orientation of , we always assume that . If then it is nothing but the -twist spun knot of .
In [15], Pao constructed a fibered -knot by setting the -fold cyclic branched cover of along with removing an open ball to be a fiber and the monodromy to be periodic, shifting the sheets of the cyclic branched cover by , and then prove that the total space is the complement of a -knot in . His results are summarized as follows:
Theorem 2.4 (Pao [15]).
Let be the branched twist spin of defined by a pair of coprime positive integers and , where is a knot in . Then, there exists a locally trivial fibration
The fiber is diffeomorphic to the -fold cyclic branched cover of along with removing an open ball and the monodromy is periodic, shifting the sheets of the cyclic branched cover by .
3. Proofs of the theorems
We first prove Theorem 1.1.
Proof of Theorem 1.1.
We prove that if either is a trivial knot or then is a trivial -knot in . It is known that if in is trivial then in is also trivial for any [19, Corollary 3]. Therefore, if is trivial then is also.
Assume that . The fiber of is the -fold cyclic branched cover of along with removing one open -ball. We will prove that this is diffeomorphic to the unit -ball.
As mentioned in Theorem 2.2, there exists a locally trivial fibration
whose fiber is the -fold cyclic branched cover of along with removing one open -ball and its monodromy is the -shift of the sheets of the cyclic branched cover. The manifold is obtained from the exterior by cutting it by a fiber , making copies, gluing them in order, and filling the boundary by canonically. The manifold before the final filling is the manifold whose fiber is and monodromy is the -shift of the sheets of the cyclic branched cover. This is the exterior of a branched twist spin. Remark that the -branched twist spin is defined for positive integers and satisfying or . Hence the assumption is needed. By filling the boundary of the manifold by , we obtain the manifold . There are two way of filling . The difference is the so-called Gluck twist ([9], cf. [6]). In either case, this is nothing but the construction of a branched twist spin. In particular, by [15, Theorem 4], is diffeomorphic to . Since the fiber of is obtained from by removing one open ball, it is diffeomorphic to the unit -ball. Thus the -knot , which is the boundary of the -ball, is a trivial -knot in . ∎
Next, we show some lemmas for proving Theorem 1.2. Let be a knot in and be a presentation of with generators and relators . We may set the generators to be meridians.
Lemma 3.1.
Let be the -twist spun knot of the -twist spun knot of a knot in . Then
(3.1) |
where and are the meridians of and , respectively, and we can set them as .
Proof.
By Lemma 2.1,
Then, the presentation in the assertion is obtained by applying Lemma 2.1 to this presentation again.
The decomposition of used to define the -twist-spinning is as in Figure 3. We now describe the decomposition of to read off the meridian of . The first factor of the second piece of the decomposition of is obtained from by removing the interior of a -dimensional ball intersecting trivially. We set this to be the product of the upper hemisphere of and the second factor of . Set to be the intersection of with . Note that , where is the north pole of the sphere on the left in Figure 3. The first piece of the decomposition of is , where we used the notation instead of since it is different from in Figure 3. The meridian of is a loop on that goes around once and does not go around . Hence it is a loop on that goes around once. This is nothing but the loop in Figure 3. As explained in the proof of Lemma 2.1, is a meridian of . Hence we have . ∎

For a presentation of of a knot in , the fundamental group of the orbifold with underlying space and remification locus is presented as
(3.2) |
where is a meridian of . Using a Wirtinger presentation of , we may set . See for instance [18, 2, 17, 1] for basics of such orbifolds.
Lemma 3.2.
Suppose that and the center of is trivial. Then, the center of is isomorphic to , generated by , and the quotient group of by its center is isomorphic to .
Proof.
Take a Wirtinger presentation of . Set and eliminate and from the presentation (3.1) by using the relations and as
This group is the quotient group of by its normal subgroup generated by and for . Let denote for simplicity. Then the above isomorphism is denoted as . Since is contained in the normal closure of the group generated by , we have
Here the last isomorphism follows from the fact that is central and hence normal in .
Let be the projection and let denote the center of . Since is a group epimorphism, is contained in the center of . Then, the assumption of the triviality of the center of implies that is trivial. Thus we have . ∎
Proof of Theorem 1.2.
Suppose that is non-trivial, , and the center of is trivial. By Lemma 3.2, the quotient group of by its center is isomorphic to . Since the abelianization of is isomorphic to , if then is non-trivial. On the other hand, for a trivial -knot , is isomorphic to and hence the quotient group of by its center is trivial. Therefore, is non-trivial. ∎
Remark 3.3.
From a knot in and a sequence of positive integers , we can obtain an knot in by applying -twist-spinning for to inductively. Let denote this -knot in . A presentation of can be obtained by the same way as in Lemma 3.1. Similar to Lemma 3.2, we can prove that if and the center of is trivial, then the quotient group of by its center is isomorphic to . Hence Theorem 1.2 holds in the higher dimensional cases also. On the other hand, it is not clear if a theorem similar to Theorem 1.1 holds or not since we used the fact, proved by Pao, that a cyclic branched cover of along a twist spun knot is and its brancherd locus is a branched twist spin [15], but a similar statement is not known in the higher dimensional cases.
4. On the center of for a torus knot
Let be a -torus knot, where and . Let and be the elements in corresponding to the preferred meridian-longitude pair of the standard torus on which lies. The meridian of is given as , where and are integers satisfying . By (3.2), the orbifold group is presented as
(4.1) |
Theorem 4.1.
Let be a -torus knot with and . For , if does not divide , then the center of has a non-trivial element.
Hence Lemma 3.2 does not hold for these torus knots.
Proof.
Let be the abelianization map. Since , which is equal to , corresponds to an element in the center of , is an element in the center of . It is suffice to show that is non-trivial in . For , let denote the image of by . Set and , where . Since is a meridian of , . Since , the solution of is given in the form and for . Since , we have . This and imply that . Hence we have and . Since by the assumption, we have . Hence is non-trivial in . ∎
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