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Twist spun knots of twist spun knots of classical knots

Mizuki Fukuda Mathematics for Advanced Materials Open Innovation Laboratory, AIST, c/o AIMR, Tohoku University, 2-1-1, Katahira, Aoba-ku, Sendai, Miyagi 980-8577, Japan [email protected]  and  Masaharu Ishikawa Department of Mathematics, Hiyoshi Campus, Keio University, 4-1-1 Hiyoshi, Kohoku, Yokohama 223-8521, Japan [email protected] Dedicated to Professor Tiê´n-So  .n Phạm on the occasion of his 60th birthday.
Abstract.

A kk-twist spun knot is an n+1n+1-dimensional knot in the n+3n+3-dimensional sphere which is obtained from an nn-dimensional knot in the n+2n+2-dimensional sphere by applying an operation called a kk-twist-spinning. This construction was introduced by Zeeman in 1965. In this paper, we show that the m2m_{2}-twist-spinning of the m1m_{1}-twist-spinning of a classical knot is a trivial 33-knot in S5S^{5} if gcd(m1,m2)=1\gcd(m_{1},m_{2})=1. We also give a sufficient condition for the m2m_{2}-twist-spinning of the m1m_{1}-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 (f,0)(f,0) of a polynomial map f:n+1f:\mathbb{C}^{n+1}\to\mathbb{C} at the origin 0 in the form f(𝐳,w)=g(𝐳)+wkf({\bf z},w)=g({\bf z})+w^{k}, (𝐳,w)n×({\bf z},w)\in\mathbb{C}^{n}\times\mathbb{C}, by using the Milnor fiberation of the lower dimensional singularity (g,0)(g,0). 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 S2n+1S^{2n+1} obtained by a cyclic suspension is a cyclic branched cover of S2n1S^{2n-1} 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 nn-dimensional knot in Sn+2S^{n+2} from an n1n-1-dimensional knot in Sn+1S^{n+1} for n2n\geq 2 [19]. This construction is called a kk-twist-spinning. The knot KnK^{n} in Sn+2S^{n+2} obtained from a knot Kn1K^{n-1} in Sn+1S^{n+1} by the kk-twist-spinning is called a kk-twist spun knot of Kn1K^{n-1}. If k1k\geq 1, then a kk-twist spun knot is a fibered knot and the fiber surface is the kk-fold cyclic branched cover of Sn+1S^{n+1} along Kn1K^{n-1} with removing one open ball. Moreover, the monodromy is periodic, shifting the sheets of the cyclic branched cover by 11. Properties of fibered knots obtained by a cyclic suspension and a kk-twist-spinning are similar, though no relations between them are known yet.

Recently, the authors studied a more general class of kk-twist spun knots in S4S^{4} called a branched twist spin, and proved that, in most cases, branched twist spins are equivalent if and only if the corresponding 11-dimensional knots in S3S^{3} are equivalent [8]. Here two knots K1K_{1} and K2K_{2} are said to be equivalent if there exists a diffeomorphism ϕ\phi from the sphere containing K1K_{1} to the sphere containing K2K_{2} satisfying ϕ(K1)=K2\phi(K_{1})=K_{2}. 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 11-dimensional knot KK in S3S^{3} by its center is isomorphic to the fundamental group π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) of the 33-orbifold 𝒪(K,m)\mathcal{O}(K,m) of cyclic type with underlying space S3S^{3} and ramification locus KK of order mm in most cases.

In this paper, we study a twist spun knot of a twist spun knot. Let m1m_{1} and m2m_{2} be positive integers and τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) be the m2m_{2}-twist spun knot of the m1m_{1}-twist spun knot of a knot KK in S3S^{3}, which is a 33-knot in S5S^{5}.

Theorem 1.1.

If either KK is trivial or gcd(m1,m2)=1\gcd(m_{1},m_{2})=1, then τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is trivial.

It is shown in [8, Proposition 3.2] that if KK is non-trivial and m12m_{1}\geq 2, then τm1(K)\tau_{m_{1}}(K) is a non-trivial 22-knot in S4S^{4}. Theorem 1.1 means that even if τm1(K)\tau_{m_{1}}(K) is non-trivial, τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) becomes trivial if gcd(m1,m2)=1\gcd(m_{1},m_{2})=1. 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 m=gcd(m1,m2)m=\gcd(m_{1},m_{2}). If KK is non-trivial, m2m\geq 2, and the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial, then τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is non-trivial.

Note that if KK is a non-trivial and non-torus knot and the mm-fold cyclic branched cover of S3S^{3} along KK is aspherical, then the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial. See the first half of the proof of [8, Lemma 3.1]. For example, if KK is a hyperbolic knot with m3m\geq 3 or a prime satellite knot with m2m\geq 2, then the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial. We will prove in Theorem 4.1 that if KK is a (p,q)(p,q)-torus knot and mm does not divide pqpq then the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) 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. kk-twist-spinning and branched twist spin

In this section, we introduce the kk-twist-spinning of an nn-dimensional knot in Sn+2S^{n+2} and a branched twist spin in S4S^{4}. An nn-dimensional knot (or nn-knot for short) is the image of an embedding of SnS^{n} into Sn+2S^{n+2}. Throughout this paper, Int X\text{\rm Int\,}X denotes the interior of a topological space XX, X\partial X denotes the boundary of XX, and Nbd(Y;X)\text{\rm Nbd}(Y;X) denotes a compact tubular neighborhood of a topological space YY embedded in XX.

2.1. kk-twist-spinning

Let KnK^{n} be an nn-knot. Choose a point pp in KnK^{n} and a coordinate neighborhood g:n+2Sn+2g:\mathbb{R}^{n+2}\to S^{n+2} such that g(0)=pg(0)=p and g1(Kn)=n×{(0,0)}g^{-1}(K^{n})=\mathbb{R}^{n}\times\{(0,0)\}. Let Bn+2B^{n+2} be the unit ball in n+2\mathbb{R}^{n+2} and set Xn+2=g(Bn+2)X^{n+2}=g(B^{n+2}) and Xn=g(Bn+2(n×{(0,0)}))X^{n}=g(B^{n+2}\cap(\mathbb{R}^{n}\times\{(0,0)\})). The pair (Xn+2,Xn)(X^{n+2},X^{n}) is an unknotted nn-ball in the n+2n+2-ball. Let Yn+2Y^{n+2} be the closure of Sn+2XnS^{n+2}-X^{n} and YnY^{n} be the closure of KnXnK^{n}\setminus X^{n}. If KnK^{n} is not trivial, then YnY^{n} is a knotted nn-ball relatively embedded in the n+2n+2-ball Yn+2Y^{n+2}. Gluing (Xn+2,Xn)(X^{n+2},X^{n}) and (Yn+2,Yn)(Y^{n+2},Y^{n}) by the identity map from Xn+2\partial X^{n+2} to Yn+2\partial Y^{n+2}, we recover the nn-knot KnK^{n} in Sn+2S^{n+2}. See Figure 1.

Refer to caption
Figure 1. A decomposition of Sn+2,Kn)S^{n+2},K^{n}) into (Xn+2,Xn)(X^{n+2},X^{n}) and (Yn+2,Yn)(Y^{n+2},Y^{n}), and the coordinates (x,ϕ)(x,\phi) on Xn+2X^{n+2}. The union Xn+2Yn+2X^{n+2}\cup Y^{n+2} is Sn+2S^{n+2} and the union XnYnX^{n}\cup Y^{n} is KnK^{n}.

Now set X=(Xn+2,Xn)×D2X=(\partial X^{n+2},\partial X^{n})\times D^{2} and Y=(Yn+2,Yn)×D2Y=(Y^{n+2},Y^{n})\times\partial D^{2}, where D2D^{2} is the unit disk in 2\mathbb{R}^{2}. Let xx denote the coordinate of g(n×{(0,0)})g(\mathbb{R}^{n}\times\{(0,0)\}) and ϕ\phi denote the angular coordinate of g({0}×(D2{(0,0)}))g(\{0\}\times(D^{2}\setminus\{(0,0)\})). Hence Xn+2X^{n+2} is equipped with the coordinates (x,ϕ)(x,\phi), where we think that the angle ϕ\phi is not defined if (x,ϕ)g(n×{(0,0)})(x,\phi)\in g(\mathbb{R}^{n}\times\{(0,0)\}). Then we glue XX and YY by the diffeomorphism f:XYf:\partial X\to\partial Y defined by

(2.1) ((x,ϕ),θ)((x,ϕ+kθ),θ),((x,\phi),\theta)\mapsto((x,\phi+k\theta),\theta),

where (x,ϕ)Xn+2(x,\phi)\in\partial X^{n+2}, θS1=D2\theta\in S^{1}=\partial D^{2} and k{0}k\in\mathbb{N}\cup\{0\}. The union XYX\cup Y is the pair of the boundaries of Yn+2×D2Y^{n+2}\times D^{2} and Yn×D2Y^{n}\times D^{2}, which is the pair of Sn+3S^{n+3} and an n+1n+1-knot in Sn+3S^{n+3}. This n+1n+1-knot is called the kk-twist spun knot of KnK^{n}. We denote it as τk(Kn)\tau_{k}(K^{n}). Note that the above definition of τk(Kn)\tau_{k}(K^{n}) works even if kk is negative. In this paper, we always assume that k0k\geq 0 by reversing the orientation of S4S^{4} if necessary.

For a 11-knot K1K^{1}, a presentation of π1(S4τk(K1))\pi_{1}(S^{4}\setminus\tau_{k}(K^{1})) can be obtained easily, see for example [16, 19]. Applying the same argument in these references to π1(Sn+3τk(Kn))\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n})), we obtain the following presentation.

Lemma 2.1.

Let x1,,xur1,,rv\langle x_{1},\ldots,x_{u}\mid r_{1},\ldots,r_{v}\rangle be a presentation of π1(Sn+2Kn)\pi_{1}(S^{n+2}\setminus K^{n}) with generators x1,,xux_{1},\ldots,x_{u} and relators r1,,rvr_{1},\ldots,r_{v}. Then

π1(Sn+3τk(Kn))x1,,xu,hr1,,rv,x1hx11h1,,xuhxu1h1,μkh,\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n}))\cong\langle x_{1},\ldots,x_{u},\,h\mid r_{1},\ldots,r_{v},\,x_{1}hx_{1}^{-1}h^{-1},\ldots,x_{u}hx_{u}^{-1}h^{-1},\,\mu^{k}h\rangle,

where μ\mu is a meridian of KnK^{n} in Sn+2S^{n+2}. In particular, π1(Sn+3τ1(Kn))\pi_{1}(S^{n+3}\setminus\tau_{1}(K^{n}))\cong\mathbb{Z} and π1(Sn+3τ0(Kn))π1(Sn+2Kn)\pi_{1}(S^{n+3}\setminus\tau_{0}(K^{n}))\cong\pi_{1}(S^{n+2}\setminus K^{n}).

Proof.

The complement Sn+3τk(Kn)S^{n+3}\setminus\tau_{k}(K^{n}) is the union of M1=(Xn+2Xn)×D2M_{1}=(\partial X^{n+2}\setminus\partial X^{n})\times D^{2} and M2=(Yn+2Yn)×D2M_{2}=(Y^{n+2}\setminus Y^{n})\times\partial D^{2}. Since (Xn+2,Xn)(X^{n+2},X^{n}) is unknotted, Xn+2Xn\partial X^{n+2}\setminus\partial X^{n} is homotopic to S1S^{1}. Note that this homotopy is given by the deformation retract from Xn+2Int Nbd(Xn;Xn+2)\partial X^{n+2}\setminus\text{\rm Int\,Nbd}(\partial X^{n};\partial X^{n+2}) to the equator of the n+1n+1-sphere Xn+2\partial X^{n+2} shown on the left in Figure 2. Hence Sn+3τk(Kn)S^{n+3}\setminus\tau_{k}(K^{n}) is homotopic to a manifold obtained from M2M_{2} by attaching S1×D2S^{1}\times D^{2}. In particular, we have

π1(Sn+3τk(Kn))π1(M2D),\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n}))\cong\pi_{1}(M_{2}\cup D),

where D={}×D2S1×D2D=\{*\}\times D^{2}\subset S^{1}\times D^{2}.

Refer to caption
Figure 2. A decomposition of (Sn+2,Kn)(S^{n+2},K^{n}). The union of Xn+2×D2\partial X^{n+2}\times D^{2} and Yn+2×D2Y^{n+2}\times\partial D^{2} is Sn+3S^{n+3} and the union of Xn×D2\partial X^{n}\times D^{2} and Yn×D2Y^{n}\times\partial D^{2} is τk(Kn)\tau_{k}(K^{n}).

The gluing map f:DM2f:\partial D\to\partial M_{2} of DD to M2M_{2} is defined by (2.1). Setting the coordinates on Y\partial Y as ((x~,ϕ~),θ~)((\tilde{x},\tilde{\phi}),\tilde{\theta}), we have

x~=x,ϕ~=ϕ+kθ,θ~=θ.\tilde{x}=x,\quad\tilde{\phi}=\phi+k\theta,\quad\tilde{\theta}=\theta.

Let hh be a loop given by {}×D2(Xn+2Xn)×D2=M1\{*\}\times\partial D^{2}\subset(\partial X^{n+2}\setminus\partial X^{n})\times D^{2}=M_{1}, which coincides with the loop {}×D2(Yn+2Yn)×D2=M2\{*\}\times\partial D^{2}\subset(Y^{n+2}\setminus Y^{n})\times\partial D^{2}=M_{2}. This loop hh commutes any elements in M1M_{1} and M2M_{2}. Therefore, it commutes any elements in π1(Sn+3τk(Kn))\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n})). This loop is parametrized by θ~S1\tilde{\theta}\in S^{1} in M2\partial M_{2}.

Let μ\mu denote a loop in Xn+2Xn\partial X^{n+2}\setminus\partial X^{n} given by the parameter ϕ\phi. This loop is a meridian of KnK^{n} in Sn+2S^{n+2}, which can be seen from the figure on the left in Figure 2. Since D\partial D is parametrized by θS1\theta\in S^{1}, its image in M2\partial M_{2} rotates kk times along ϕ~S1\tilde{\phi}\in S^{1} and once along θ~S1\tilde{\theta}\in S^{1}. Since D\partial D is null-homotopic in M2DM_{2}\cup D, we have μkh=1\mu^{k}h=1. Thus the presentation of π1(Sn+3τk(Kn))\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n})) in the assertion is obtained.

If k=1k=1 then the meridian μ=h1\mu=h^{-1} is in the center of π1(Sn+3τ1(Kn))\pi_{1}(S^{n+3}\setminus\tau_{1}(K^{n})). We can choose the generators of π1(Sn+3τ1(Kn))\pi_{1}(S^{n+3}\setminus\tau_{1}(K^{n})) to be conjugate to μ\mu (cf. [12]). Since H1(Sn+3τ1(Kn))H_{1}(S^{n+3}\setminus\tau_{1}(K^{n})) is isomorphic to \mathbb{Z}, π1(Sn+3τ1(Kn))\pi_{1}(S^{n+3}\setminus\tau_{1}(K^{n})) is the infinite cyclic group generated by μ\mu.

The assertion in the case k=0k=0 is obtained from the presentation of π1(Sn+3τk(Kn))\pi_{1}(S^{n+3}\setminus\tau_{k}(K^{n})) immediately. ∎

Theorem 2.2 (Zeeman [19]).

If k1k\geq 1 then there exists a locally trivial fibration

f:Sn+3Int Nbd(τk(Kn);Sn+3)S1.f:S^{n+3}\setminus\text{\rm Int\,Nbd}(\tau_{k}(K^{n});S^{n+3})\to S^{1}.

The fiber is diffeomorphic to the kk-fold cyclic branched cover of Sn+2S^{n+2} along KnK^{n} with removing an open ball and the monodromy is periodic, shifting the sheets of the cyclic branched cover by 11.

Remark 2.3.

If k=1k=1, then the fiber is diffeomorphic to the n+1n+1-dimensional unit ball. Therefore, τk(Kn)\tau_{k}(K^{n}) is a trivial n+1n+1-knot in Sn+3S^{n+3}.

2.2. Branched twist spin

Circle actions on homotopy 44-spheres are classified by Montgomery and Yang [14] and Fintushel [3], and later, Pao proved in [15] that such homotopy 44-spheres are the standard 44-sphere S4S^{4}. A 22-sphere embedded in S4S^{4} 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 KK in S3S^{3} by “twisting”, like a kk-twist-spinning, but the “twisting” for a branched twist spin is defined by two integers mm and nn, where (m,n)(m,n) is either a pair of coprime integers in ×\mathbb{Z}\times\mathbb{N} or (0,1)(0,1). We may assume that m0m\geq 0 by reversing the orientation of S4S^{4} if necessary. In this paper, since we study branched twist spins without fixing the orientation of S4S^{4}, we always assume that m0m\geq 0. If (m,n)=(k,1)(m,n)=(k,1) then it is nothing but the kk-twist spun knot of KK.

In [15], Pao constructed a fibered 22-knot by setting the mm-fold cyclic branched cover of S3S^{3} along KK with removing an open ball to be a fiber and the monodromy to be periodic, shifting the sheets of the cyclic branched cover by nn, and then prove that the total space is the complement of a 22-knot in S4S^{4}. His results are summarized as follows:

Theorem 2.4 (Pao [15]).

Let τm,n(K)\tau_{m,n}(K) be the branched twist spin of KK defined by a pair of coprime positive integers mm and nn, where KK is a knot in S3S^{3}. Then, there exists a locally trivial fibration

f:S4Int Nbd(τm,n(K);S4)S1.f:S^{4}\setminus\text{\rm Int\,Nbd}(\tau_{m,n}(K);S^{4})\to S^{1}.

The fiber is diffeomorphic to the mm-fold cyclic branched cover of S3S^{3} along KK with removing an open ball and the monodromy is periodic, shifting the sheets of the cyclic branched cover by nn.

It is natural to ask when two branched twist spins are non-equivalent. This problem is studied by the first author in [4, 5, 7]. See also [8, 11] for more recent results.

3. Proofs of the theorems

We first prove Theorem 1.1.

Proof of Theorem 1.1.

We prove that if either KK is a trivial knot or m=1m=1 then τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is a trivial 33-knot in S5S^{5}. It is known that if KnK^{n} in Sn+2S^{n+2} is trivial then τk(Kn)\tau_{k}(K^{n}) in Sn+3S^{n+3} is also trivial for any k0k\geq 0 [19, Corollary 3]. Therefore, if KK is trivial then τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is also.

Assume that m=1m=1. The fiber of τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is the m2m_{2}-fold cyclic branched cover Mm2(τm1(K))M_{m_{2}}(\tau_{m_{1}}(K)) of S4S^{4} along τm1(K)\tau_{m_{1}}(K) with removing one open 44-ball. We will prove that this is diffeomorphic to the unit 44-ball.

As mentioned in Theorem 2.2, there exists a locally trivial fibration

f:S4Int Nbd(τm1(K);S4)S1f:S^{4}\setminus\text{\rm Int\,Nbd}(\tau_{m_{1}}(K);S^{4})\to S^{1}

whose fiber FF is the m1m_{1}-fold cyclic branched cover Mm1(K)M_{m_{1}}(K) of S3S^{3} along KK with removing one open 33-ball and its monodromy is the 11-shift of the sheets of the cyclic branched cover. The manifold Mm2(τm1(K))M_{m_{2}}(\tau_{m_{1}}(K)) is obtained from the exterior S4Int Nbd(τm1(K);S4)S^{4}\setminus\text{\rm Int\,Nbd}(\tau_{m_{1}}(K);S^{4}) by cutting it by a fiber FF, making m2m_{2} copies, gluing them in order, and filling the boundary by S2×D2S^{2}\times D^{2} canonically. The manifold before the final filling is the manifold whose fiber is FF and monodromy is the m2m_{2}-shift of the sheets of the cyclic branched cover. This is the exterior of a branched twist spin. Remark that the (m1,m2)(m_{1},m_{2})-branched twist spin is defined for positive integers m1m_{1} and m2m_{2} satisfying gcd(m1,m2)=1\gcd(m_{1},m_{2})=1 or (m1,m2)=(0,1)(m_{1},m_{2})=(0,1). Hence the assumption m=gcd(m1,m2)=1m=\gcd(m_{1},m_{2})=1 is needed. By filling the boundary of the manifold by S2×D2S^{2}\times D^{2}, we obtain the manifold Mm2(τm1(K))M_{m_{2}}(\tau_{m_{1}}(K)). There are two way of filling S2×D2S^{2}\times D^{2}. 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], Mm2(τm1(K))M_{m_{2}}(\tau_{m_{1}}(K)) is diffeomorphic to S4S^{4}. Since the fiber of τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is obtained from Mm2(τm1(K))M_{m_{2}}(\tau_{m_{1}}(K)) by removing one open ball, it is diffeomorphic to the unit 44-ball. Thus the 33-knot τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)), which is the boundary of the 44-ball, is a trivial 33-knot in S5S^{5}. ∎

Next, we show some lemmas for proving Theorem 1.2. Let KK be a knot in S3S^{3} and x1,,xur1,,rv\langle x_{1},\ldots,x_{u}\mid r_{1},\ldots,r_{v}\rangle be a presentation of π1(S3K)\pi_{1}(S^{3}\setminus K) with generators x1,,xux_{1},\ldots,x_{u} and relators r1,,rvr_{1},\ldots,r_{v}. We may set the generators to be meridians.

Lemma 3.1.

Let τm2(τm1(K)))\tau_{m_{2}}(\tau_{m_{1}}(K))) be the m2m_{2}-twist spun knot of the m1m_{1}-twist spun knot of a knot KK in S3S^{3}. Then

(3.1) π1(S5τm2(τm1(K)))x1,,xu,h1,h2r1,,rv,x1h1x11h11,,xuh1xu1h11,μ1m1h1,x1h2x11h21,,xuh2xu1h21,h1h2h11h21,μ2m2h2,\begin{split}&\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K)))\\ &\quad\cong\langle x_{1},\ldots,x_{u},\,h_{1},h_{2}\mid r_{1},\ldots,r_{v},\,x_{1}h_{1}x_{1}^{-1}h_{1}^{-1},\ldots,x_{u}h_{1}x_{u}^{-1}h_{1}^{-1},\,\mu_{1}^{m_{1}}h_{1},\\ &\hskip 116.6563pt\;x_{1}h_{2}x_{1}^{-1}h_{2}^{-1},\ldots,x_{u}h_{2}x_{u}^{-1}h_{2}^{-1},\,h_{1}h_{2}h_{1}^{-1}h_{2}^{-1},\,\mu_{2}^{m_{2}}h_{2}\rangle,\end{split}

where μ1\mu_{1} and μ2\mu_{2} are the meridians of KK and τm1(K)\tau_{m_{1}}(K), respectively, and we can set them as μ1=μ2=x1\mu_{1}=\mu_{2}=x_{1}.

Proof.

By Lemma 2.1,

π1(S4τm1(K))x1,,xu,h1r1,,rv,x1h1x11h11,,xuh1xu1h11,μ1m1h1.\begin{split}\pi_{1}(S^{4}\setminus\tau_{m_{1}}(K))\cong\langle x_{1},\ldots,x_{u},\,h_{1}\mid&\;r_{1},\ldots,r_{v},\,x_{1}h_{1}x_{1}^{-1}h_{1}^{-1},\ldots,x_{u}h_{1}x_{u}^{-1}h_{1}^{-1},\,\mu_{1}^{m_{1}}h_{1}\rangle.\end{split}

Then, the presentation in the assertion is obtained by applying Lemma 2.1 to this presentation again.

The decomposition of S4S^{4} used to define the kk-twist-spinning is as in Figure 3. We now describe the decomposition of S5S^{5} to read off the meridian μ2\mu_{2} of τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)). The first factor (Y4,Y2)(Y^{4},Y^{2}) of the second piece of the decomposition of S5S^{5} is obtained from S4S^{4} by removing the interior of a 44-dimensional ball B4B^{4} intersecting τm1(K)\tau_{m_{1}}(K) trivially. We set this B4B^{4} to be the product of the upper hemisphere HH of X3\partial X^{3} and the second factor D2D^{2} of (X3,X1)×D2(\partial X^{3},\partial X^{1})\times D^{2}. Set B2B^{2} to be the intersection of B4B^{4} with τm1(K)\tau_{m_{1}}(K). Note that B2=(HX1)×D2B^{2}=(H\cap\partial X^{1})\times D^{2}, where HX1H\cap\partial X^{1} is the north pole of the sphere on the left in Figure 3. The first piece (X4,X2)×(D2)(\partial X^{4},\partial X^{2})\times(D^{2})^{\prime} of the decomposition of S5S^{5} is (B4,B2)×(D2)(\partial B^{4},\partial B^{2})\times(D^{2})^{\prime}, where we used the notation (D2)(D^{2})^{\prime} instead of D2D^{2} since it is different from D2D^{2} in Figure 3. The meridian μ2\mu_{2} of τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is a loop on (B4B2)×(D2)(\partial B^{4}\setminus\partial B^{2})\times\partial(D^{2})^{\prime} that goes around B2×(D2)\partial B^{2}\times\partial(D^{2})^{\prime} once and does not go around (D2)\partial(D^{2})^{\prime}. Hence it is a loop on HX1H\setminus\partial X^{1} that goes around HX1H\cap\partial X^{1} once. This is nothing but the loop μ1\mu_{1} in Figure 3. As explained in the proof of Lemma 2.1, μ1\mu_{1} is a meridian of KK. Hence we have μ2=μ1=x1\mu_{2}=\mu_{1}=x_{1}. ∎

Refer to caption
Figure 3. A decomposition of (S4,τm1(K))(S^{4},\tau_{m_{1}}(K)).

For a presentation x1,,xur1,,rv\langle x_{1},\ldots,x_{u}\mid r_{1},\ldots,r_{v}\rangle of π1(S3K)\pi_{1}(S^{3}\setminus K) of a knot KK in S3S^{3}, the fundamental group π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) of the orbifold 𝒪(K,m)\mathcal{O}(K,m) with underlying space S3S^{3} and remification locus KK is presented as

(3.2) π1orb(𝒪(K,m))x1,,xur1,,rv,μm\pi_{1}^{orb}(\mathcal{O}(K,m))\cong\langle x_{1},\ldots,x_{u}\mid r_{1},\ldots,r_{v},\,\mu^{m}\rangle

where μ\mu is a meridian of KK. Using a Wirtinger presentation x1,,xur1,,rv\langle x_{1},\ldots,x_{u}\mid r_{1},\ldots,r_{v}\rangle of π1(S3K)\pi_{1}(S^{3}\setminus K), we may set μ=x1\mu=x_{1}. See for instance [18, 2, 17, 1] for basics of such orbifolds.

Lemma 3.2.

Suppose that m=gcd(m1,m2)2m=\gcd(m_{1},m_{2})\geq 2 and the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial. Then, the center of π1(S5τm2(τm1(K)))\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K))) is isomorphic to \mathbb{Z}, generated by x1mx_{1}^{m}, and the quotient group of π1(S5τm2(τm1(K)))\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K))) by its center is isomorphic to π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)).

Proof.

Take a Wirtinger presentation x1,,xur1,,rv\langle x_{1},\ldots,x_{u}\mid\;r_{1},\ldots,r_{v}\rangle of π1(S3K)\pi_{1}(S^{3}\setminus K). Set μ1=μ2=x1\mu_{1}=\mu_{2}=x_{1} and eliminate h1h_{1} and h2h_{2} from the presentation (3.1) by using the relations h1=μ1m1=x1m1h_{1}=\mu_{1}^{-m_{1}}=x_{1}^{-m_{1}} and h2=μ2m2=x1m2h_{2}=\mu_{2}^{-m_{2}}=x_{1}^{-m_{2}} as

π1(S5τm2(τm1(K)))x1,,xur1,,rv,x2x1m1x21x1m1,,xux1m1xu1x1m1,x2x1m2x21x1m2,,xux1m2xu1x1m2.\begin{split}\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K)))\cong\langle x_{1},\ldots,x_{u}\mid\;&r_{1},\ldots,r_{v},\,x_{2}x_{1}^{-m_{1}}x_{2}^{-1}x_{1}^{m_{1}},\ldots,x_{u}x_{1}^{-m_{1}}x_{u}^{-1}x_{1}^{m_{1}},\\ &x_{2}x_{1}^{-m_{2}}x_{2}^{-1}x_{1}^{m_{2}},\ldots,x_{u}x_{1}^{-m_{2}}x_{u}^{-1}x_{1}^{m_{2}}\rangle.\end{split}

This group is the quotient group of π1(S3K)\pi_{1}(S^{3}\setminus K) by its normal subgroup NN generated by xkx1m1xk1x1m1x_{k}x_{1}^{-m_{1}}x_{k}^{-1}x_{1}^{m_{1}} and xkx1m2xk1x1m2x_{k}x_{1}^{-m_{2}}x_{k}^{-1}x_{1}^{m_{2}} for k=2,,uk=2,\ldots,u. Let GG denote π1(S5τm2(τm1(K)))\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K))) for simplicity. Then the above isomorphism is denoted as Gπ1(S3K)/NG\cong\pi_{1}(S^{3}\setminus K)/N. Since NN is contained in the normal closure x1m\langle\langle x_{1}^{m}\rangle\rangle of the group x1m\langle x_{1}^{m}\rangle generated by x1mx_{1}^{m}, we have

π1orb(𝒪(K,m))π1(S3K)/x1m(π1(S3K)/N)/x1mG/x1m.\pi_{1}^{orb}(\mathcal{O}(K,m))\cong\pi_{1}(S^{3}\setminus K)/\langle\langle x_{1}^{m}\rangle\rangle\cong(\pi_{1}(S^{3}\setminus K)/N)/\langle\langle x_{1}^{m}\rangle\rangle\cong G/\langle x_{1}^{m}\rangle.

Here the last isomorphism follows from the fact that x1m\langle x_{1}^{m}\rangle is central and hence normal in GG.

Let p:GG/x1mp:G\to G/\langle x_{1}^{m}\rangle be the projection and let Z(G)Z(G) denote the center of GG. Since pp is a group epimorphism, p(Z(G))p(Z(G)) is contained in the center of G/x1mG/\langle x_{1}^{m}\rangle. Then, the assumption of the triviality of the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) implies that p(Z(G))p(Z(G)) is trivial. Thus we have Z(G)=x1mZ(G)=\langle x_{1}^{m}\rangle. ∎

Proof of Theorem 1.2.

Suppose that KK is non-trivial, m=gcd(m1,m2)2m=\gcd(m_{1},m_{2})\geq 2, and the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial. By Lemma 3.2, the quotient group of π1(S5τm2(τm1(K)))\pi_{1}(S^{5}\setminus\tau_{m_{2}}(\tau_{m_{1}}(K))) by its center is isomorphic to π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)). Since the abelianization of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is isomorphic to /m\mathbb{Z}/m\mathbb{Z}, if m2m\geq 2 then π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is non-trivial. On the other hand, for a trivial 33-knot OO, π1(S5O)\pi_{1}(S^{5}\setminus O) is isomorphic to \mathbb{Z} and hence the quotient group of π1(S5O)\pi_{1}(S^{5}\setminus O) by its center is trivial. Therefore, τm2(τm1(K))\tau_{m_{2}}(\tau_{m_{1}}(K)) is non-trivial. ∎

Remark 3.3.

From a knot KK in S3S^{3} and a sequence of positive integers 𝐦=(m1,m2,,mN){\bf m}=(m_{1},m_{2},\ldots,m_{N}), we can obtain an N+1N+1 knot in SN+3S^{N+3} by applying mim_{i}-twist-spinning for i=1,2,,Ni=1,2,\ldots,N to KK inductively. Let τ𝐦(K)\tau_{\bf m}(K) denote this N+1N+1-knot in SN+3S^{N+3}. A presentation of π1(SN+3τ𝐦(K))\pi_{1}(S^{N+3}\setminus\tau_{\bf m}(K)) can be obtained by the same way as in Lemma 3.1. Similar to Lemma 3.2, we can prove that if m=gcd(m1,m2,,mN)2m=\gcd(m_{1},m_{2},\ldots,m_{N})\geq 2 and the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is trivial, then the quotient group of π1(SN+3τ𝐦(K))\pi_{1}(S^{N+3}\setminus\tau_{\bf m}(K)) by its center is isomorphic to π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)). 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 S4S^{4} along a twist spun knot is S4S^{4} 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 π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) for a torus knot KK

Let KK be a (p,q)(p,q)-torus knot, where p,q2p,q\geq 2 and gcd(p,q)=1\gcd(p,q)=1. Let xx and yy be the elements in π1(S3K)\pi_{1}(S^{3}\setminus K) corresponding to the preferred meridian-longitude pair of the standard torus on which KK lies. The meridian of KK is given as xsyrx^{s}y^{r}, where rr and ss are integers satisfying pr+qs=1pr+qs=1. By (3.2), the orbifold group π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) is presented as

(4.1) π1orb(𝒪(K,m))x,yxpyq,(xsyr)m.\pi_{1}^{orb}(\mathcal{O}(K,m))\cong\langle x,y\mid x^{p}y^{-q},\,(x^{s}y^{r})^{m}\rangle.
Theorem 4.1.

Let KK be a (p,q)(p,q)-torus knot with p,q2p,q\geq 2 and gcd(p,q)=1{\rm gcd}(p,q)=1. For m2m\geq 2, if mm does not divide pqpq, then the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)) has a non-trivial element.

Hence Lemma 3.2 does not hold for these torus knots.

Proof.

Let A:π1orb(𝒪(K,m))/mA:\pi_{1}^{orb}(\mathcal{O}(K,m))\to\mathbb{Z}/m\mathbb{Z} be the abelianization map. Since xpx^{p}, which is equal to yqy^{q}, corresponds to an element in the center of π1(S3K)\pi_{1}(S^{3}\setminus K), xpx^{p} is an element in the center of π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)). It is suffice to show that xpx^{p} is non-trivial in π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)). For nn\in\mathbb{Z}, let n¯/m\bar{n}\in\mathbb{Z}/m\mathbb{Z} denote the image of nn by AA. Set A(x)=a¯A(x)=\bar{a} and A(y)=b¯A(y)=\bar{b}, where a,ba,b\in\mathbb{Z}. Since xsyrx^{s}y^{r} is a meridian of KK, A(xsyr)a¯s+b¯r1modmA(x^{s}y^{r})\equiv\bar{a}s+\bar{b}r\equiv 1\mod m. Since pr+qs=1pr+qs=1, the solution of as+br=1as+br=1 is given in the form a=qtra=q-tr and b=p+tsb=p+ts for tt\in\mathbb{Z}. Since xp=yqx^{p}=y^{q}, we have p(qtr)¯=A(xp)=A(yq)=q(p+ts)¯\overline{p(q-tr)}=A(x^{p})=A(y^{q})=\overline{q(p+ts)}. This and pr+sq=1pr+sq=1 imply that t=0modmt=0\mod m. Hence we have A(x)=q¯A(x)=\bar{q} and A(y)=p¯A(y)=\bar{p}. Since p¯q¯0¯\bar{p}\bar{q}\neq\bar{0} by the assumption, we have A(xp)0¯A(x^{p})\neq\bar{0}. Hence xpx^{p} is non-trivial in π1orb(𝒪(K,m))\pi_{1}^{orb}(\mathcal{O}(K,m)). ∎

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