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Generalized torsion for knots with arbitrarily high genus

Published online by Cambridge University Press:  02 December 2021

Kimihiko Motegi
Affiliation:
Department of Mathematics, Nihon University, 3-25-40 Sakurajosui, Setagaya-ku, Tokyo, 156-8550, Japan e-mail: motegi.kimihiko@nihon-u.ac.jp
Masakazu Teragaito*
Affiliation:
Department of Mathematics and Mathematics Education, Hiroshima University, 1-1-1 Kagamiyama, Higashi-hiroshima, Hiroshima, 739-8524, Japan
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Abstract

Let G be a group, and let g be a nontrivial element in G. If some nonempty finite product of conjugates of g equals the identity, then g is called a generalized torsion element. We say that a knot K has generalized torsion if $G(K) = \pi _1(S^3 - K)$ admits such an element. For a $(2, 2q+1)$-torus knot K, we demonstrate that there are infinitely many unknots $c_n$ in $S^3$ such that p-twisting K about $c_n$ yields a twist family $\{ K_{q, n, p}\}_{p \in \mathbb {Z}}$ in which $K_{q, n, p}$ is a hyperbolic knot with generalized torsion whenever $|p|> 3$. This gives a new infinite class of hyperbolic knots having generalized torsion. In particular, each class contains knots with arbitrarily high genus. We also show that some twisted torus knots, including the $(-2, 3, 7)$-pretzel knot, have generalized torsion. Because generalized torsion is an obstruction for having bi-order, these knots have non-bi-orderable knot groups.

Information

Type
Article
Copyright
© Canadian Mathematical Society, 2021
Figure 0

Figure 1 A braid with an axis $c_n$.

Figure 1

Figure 2 Deform $K_q \cup c_n$.

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Figure 3 Deform $K_q \cup c_n$.

Figure 3

Figure 4 Deform $K_q \cup c_n$.

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Figure 5 The link $K_q \cup c_n$ with unknotting tunnel $\gamma $.

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Figure 6 $K_q \cup c_n$.

Figure 6

Figure 7 Deform N with $\ell $.

Figure 7

Figure 8 Deform N with $\ell $.

Figure 8

Figure 9 Deform N with $\ell $.

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Figure 10 Deform N with $\ell $; $\ell $ is twisted in N as in the right-hand side of Figure 11.

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Figure 11 Absorb q twists.

Figure 11

Figure 12 Two loops $\alpha $ and $\beta $ bound mutually disjoint meridian disks of the outside handlebody H.

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Figure 13 The Heegaard surface $\Sigma $ and the standard generators $a, b, c, d$ of $\pi _1(\Sigma )$.

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Figure 14 $K_0$ and the generators $[G_0]$, $[R_0]$, $[P_0]$ of $\pi _1(\Sigma -K_0)$ (left); the circles $C_1$, $C_2$, $C_3$, and $C_4$ (right).