2-knots with the same knot group but different knot quandles

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  • Journal of the Mathematical Society of Japan
  • arXiv (Cornell University)

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Summary

This paper presents a significant advancement in the understanding of 2-knots by providing the first explicit examples of 2-knots that share the same knot group but possess distinct knot quandles. This addresses a long-standing open problem in knot theory, where such distinctions were known for 1-knots (e.g., the square knot and granny knot) but had no known analogues in higher dimensions.

The core innovation lies in leveraging and extending the concept of the “quandle type” as a powerful invariant. Knot quandles are algebraic structures that capture more detailed topological information about a knot than its knot group (the fundamental group of the knot’s complement). While an isomorphism between knot quandles implies an isomorphism between their associated knot groups, the converse is not generally true. This paper meticulously demonstrates this for 2-knots.

The key innovations and their integration are as follows:

  1. Introduction of the Quandle “Type”: The authors introduce a specific algebraic invariant for any quandle, called its “type.” Defined as the minimum positive integer \(n\) (if it exists) such that for any two elements \(x, y\) in the quandle, iterating a specific binary operation \(n\) times (\(x *^n y\)) returns \(x\). If no such integer exists, the type is infinite. This “type” serves as a quantitative measure to distinguish quandles.

  2. Calculation of Quandle Type for Generalized Alexander Quandles: A crucial technical result (Proposition 2.1) establishes that for a generalized Alexander quandle GAlex(\(G, f\)) (defined by a group \(G\) and its automorphism \(f\)), its type is precisely the order of the automorphism \(f\). This connects the abstract quandle invariant to a fundamental group-theoretic property.

  3. Determining Monodromy Order for Twist Spins: The paper then focuses on a specific class of 2-knots called n-twist spins, denoted \(\tau^n(k)\), which are constructed from 1-knots \(k\) by Zeeman’s twist-spinning process. A critical step (Proposition 3.2, with proof in Appendix A) proves that the order of the monodromy automorphism \(\phi\) associated with the complement of \(\tau^n(k)\) is exactly the twist number \(n\).

  4. Connecting Twist Number to Quandle Type: By combining the above, the paper proves a central theorem (Theorem 3.3): the type of the knot quandle of an n-twist spun knot \(\tau^n(k)\) is precisely \(n\). This directly links a topological construction parameter (\(n\)) to an algebraic invariant of the knot quandle, making the twist number a direct discriminator of quandles.

  5. Construction of Counterexamples: Using the derived property, the authors construct infinitely many triples of 2-knots that fulfill the desired conditions. They consider twist spins of torus knots. It is a known prior result (from Gordon’s work) that for coprime integers \(p, q, r\), the knot groups of \(\tau^p(t_{q,r})\), \(\tau^q(t_{r,p})\), and \(\tau^r(t_{p,q})\) are mutually isomorphic (due to homeomorphic properties of their underlying branched covering spaces). However, by Theorem 3.3, their knot quandles have types \(p, q,\) and \(r\) respectively. Since \(p, q, r\) are coprime, their quandles must be non-isomorphic, thus providing the desired examples.

As a significant byproduct, the paper also provides a comprehensive classification of twist spins whose knot quandles are finite, both for oriented and unoriented 2-knots (Theorems 4.1 and 4.5). This classification unifies and extends previous partial results in the literature, demonstrating the utility of the quandle “type” as a robust invariant for distinguishing these complex 2-knot structures.

Main Prior Ingredients Needed:

  • Quandle Theory and Knot Quandles: The fundamental definitions and properties of quandles, their associated groups, and their role as knot invariants (pioneered by Joyce, Matveev).
  • Generalized Alexander Quandles: The specific construction and properties of GAlex(\(G, f\)) and its connection to knot quandles of fibered knots (as established by Inoue).
  • Zeeman’s Twist-Spinning Construction: The method for obtaining 2-knots from 1-knots by spinning a knot complement.
  • Properties of Branched Covering Spaces: Knowledge about the fundamental groups and homeomorphic relationships of branched covering spaces, particularly for torus knots, which allows for the identification of 2-knots with isomorphic knot groups.
  • Monodromy of Fibered Knots: Understanding how the monodromy map acts on the fundamental group of the fiber in a fibered knot complement.
  • Classification Results for 1-Knots: Previous work on the distinguishability of 1-knots by group vs. quandle, and classifications of 1-knots with finite quandles or specific group structures.
We give a first example of 2-knots with the same knot group but different knot quandles by analyzing the knot quandles of twist spins. As a byproduct of the analysis, … We give a first example of 2-knots with the same knot group but different knot quandles by analyzing the knot quandles of twist spins. As a byproduct of the analysis, we also give a classification of all twist spins with finite knot quandles.
We consider a locally flat <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-sphere in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> … We consider a locally flat <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-sphere in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> representing a primitive homology class <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="xi"> <mml:semantics> <mml:mi>ξ<!-- ξ --></mml:mi> <mml:annotation encoding="application/x-tex">\xi</mml:annotation> </mml:semantics> </mml:math> </inline-formula>, which is referred to as a <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-knot in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> representing <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="xi"> <mml:semantics> <mml:mi>ξ<!-- ξ --></mml:mi> <mml:annotation encoding="application/x-tex">\xi</mml:annotation> </mml:semantics> </mml:math> </inline-formula>. Then for any given primitive class <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="xi"> <mml:semantics> <mml:mi>ξ<!-- ξ --></mml:mi> <mml:annotation encoding="application/x-tex">\xi</mml:annotation> </mml:semantics> </mml:math> </inline-formula>, there exists a <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-knot in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> representing <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="xi"> <mml:semantics> <mml:mi>ξ<!-- ξ --></mml:mi> <mml:annotation encoding="application/x-tex">\xi</mml:annotation> </mml:semantics> </mml:math> </inline-formula> with simply-connected complement. In this paper, we consider the classification of <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-knots in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> whose complements have a fixed fundamental group. We show that if the complement of a <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-knot <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S"> <mml:semantics> <mml:mi>S</mml:mi> <mml:annotation encoding="application/x-tex">S</mml:annotation> </mml:semantics> </mml:math> </inline-formula> in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> is simply connected, then the ambient isotopy type of <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S"> <mml:semantics> <mml:mi>S</mml:mi> <mml:annotation encoding="application/x-tex">S</mml:annotation> </mml:semantics> </mml:math> </inline-formula> is determined. In the case of nontrivial <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="pi 1"> <mml:semantics> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msub> <mml:mi>π<!-- π --></mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:mrow> <mml:annotation encoding="application/x-tex">{\pi _1}</mml:annotation> </mml:semantics> </mml:math> </inline-formula>, however, we show that the ambient isotopy type of a <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="2"> <mml:semantics> <mml:mn>2</mml:mn> <mml:annotation encoding="application/x-tex">2</mml:annotation> </mml:semantics> </mml:math> </inline-formula>-knot in <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="upper S squared times upper S squared"> <mml:semantics> <mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> <mml:mo>×<!-- × --></mml:mo> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:mrow> <mml:annotation encoding="application/x-tex">{S^2} \times {S^2}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> with nontrivial <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="pi 1"> <mml:semantics> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msub> <mml:mi>π<!-- π --></mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:mrow> <mml:annotation encoding="application/x-tex">{\pi _1}</mml:annotation> </mml:semantics> </mml:math> </inline-formula> is not always determined by <inline-formula content-type="math/mathml"> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" alttext="pi 1"> <mml:semantics> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:msub> <mml:mi>π<!-- π --></mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:mrow> <mml:annotation encoding="application/x-tex">{\pi _1}</mml:annotation> </mml:semantics> </mml:math> </inline-formula>.
We have a knot quandle and a fundamental class as invariants for a surface-knot. These invariants can be defined for a classical knot in a similar way, and it is … We have a knot quandle and a fundamental class as invariants for a surface-knot. These invariants can be defined for a classical knot in a similar way, and it is known that the pair of them is a complete invariant for classical knots. In this paper, we compare a situation in surface-knot theory with that in classical knot theory, and prove the following: There exist arbitrarily many inequivalent surface-knots of genus $g$ with the same knot quandle, and there exist two inequivalent surface-knots of genus $g$ with the same knot quandle and with the same fundamental class.
1. Knots and Related Manifolds 2. The Knot Group 3. Localization and Asphericity 4. The Rank 1 Case 5. The Rank 2 Case 6. Ascending Series and the Large Rank … 1. Knots and Related Manifolds 2. The Knot Group 3. Localization and Asphericity 4. The Rank 1 Case 5. The Rank 2 Case 6. Ascending Series and the Large Rank Cases 7. The Homotopy Type of M(K) 8. Applying Surgery to Determine the Knot.
A n-knot group is the fundamental group of the complement of an n-sphere smoothly embedded in Sn+2. Artin gave in 1925 ([A]) an algebraic characterization of 1-knot groups. M. Kervaire … A n-knot group is the fundamental group of the complement of an n-sphere smoothly embedded in Sn+2. Artin gave in 1925 ([A]) an algebraic characterization of 1-knot groups. M. Kervaire gave in 1965 ([K]) an algebraic characterization of n-knot groups for n = 3. The problem of characterizing algebraically 2-knot groups has been posed several times (see for example [Su, Problem 4.7]). Ribbon 2-knot groups have been characterized algebraically by Yajima [Y]. We will give here a characterization of 2-knot groups in terms of presentations. It has the flavor of Artin's characterization of 1-knot groups. S. Kamada has independently obtained another characterization of 2-knot groups ([Ka]).
We show that fibered 2-knots with closed fiber the Hantzsche–Wendt flat 3-manifold are not reflexive, while every fibered 2-knot with closed fiber a Nil-manifold with base orbifold S(3, 3, 3) … We show that fibered 2-knots with closed fiber the Hantzsche–Wendt flat 3-manifold are not reflexive, while every fibered 2-knot with closed fiber a Nil-manifold with base orbifold S(3, 3, 3) is reflexive. We also determine when the knots are amphicheiral or invertible, and give explicit representatives for the possible meridians (up to automorphisms of the knot group which induce the identity on abelianization) for the groups of all knots in either class. This completes the TOP classification of 2-knots with torsion-free, elementary amenable knot group. In the final section, we show that the only non-trivial doubly null-concordant knots with such groups are those with the group of the 2-twist spin of the knot 9 46 .
We study smooth, proper embeddings of noncompact surfaces in 4-manifolds, focusing on exotic planes and annuli, i.e., embeddings pairwise homeomorphic to the standard embeddings of R^2 and R^2-int D^2 in … We study smooth, proper embeddings of noncompact surfaces in 4-manifolds, focusing on exotic planes and annuli, i.e., embeddings pairwise homeomorphic to the standard embeddings of R^2 and R^2-int D^2 in R^4. We encounter two uncountable classes of exotic planes, with radically different properties. One class is simple enough that we exhibit explicit level diagrams of them without 2-handles. Diagrams from the other class seem intractable to draw, and require infinitely many 2-handles. We show that every compact surface embedded rel nonempty boundary in the 4-ball has interior pairwise homeomorphic to infinitely many smooth, proper embeddings in R^4. We also see that the almost-smooth, compact, embedded surfaces produced in 4-manifolds by Freedman theory must have singularities requiring infinitely many local minima in their radial functions. We construct exotic planes with uncountable group actions injecting into the pairwise mapping class group. This work raises many questions, some of which we list.
We study smooth, proper embeddings of noncompact surfaces in 4-manifolds, focusing on exotic planes and annuli, i.e., embeddings pairwise homeomorphic to the standard embeddings of R^2 and R^2-int D^2 in … We study smooth, proper embeddings of noncompact surfaces in 4-manifolds, focusing on exotic planes and annuli, i.e., embeddings pairwise homeomorphic to the standard embeddings of R^2 and R^2-int D^2 in R^4. We encounter two uncountable classes of exotic planes, with radically different properties. One class is simple enough that we exhibit explicit level diagrams of them without 2-handles. Diagrams from the other class seem intractable to draw, and require infinitely many 2-handles. Every compact surface embedded rel nonempty boundary in the 4-ball has interior pairwise homeomorphic to infinitely many smooth, proper embeddings in R^4. The almost-smooth, compact, embedded surfaces produced in 4-manifolds by Freedman theory have singularities requiring infinitely many local minima in their radial functions. There are exotic planes with uncountable groups acting isotopically essentially. This work raises many questions, some of which we list.
A link L is universal if every closed orientable 3-manifold M is a finite branched covering of S3 with the branch set equal to L. Known examples of universal links … A link L is universal if every closed orientable 3-manifold M is a finite branched covering of S3 with the branch set equal to L. Known examples of universal links are the figure eight knot and the Borromean rings. It is also known that the trefoil knot is not universal. The notion of universality can be refined by allowing only certain types of branching. A branched covering p:M→N over a link L is of type {1,2} if the branching (ramification) index of each component of p−1(K) is either 1 or 2. A link L is 2-universal if every closed orientable 3-manifold M is a finite branched cover of S3 over L, of type {1,2}. The existence of 2-universal links has been known, but not of 2-universal knots. The authors use the existence of 2-universal links to prove that 2-universal knots exist. Their main theorem implies that for any 2-universal link L there exists a branched covering p:S3→S3 over a knot K, such that L is a sublink of the pseudo-branch cover, i.e., such that L is contained in the union of those components of p−1(K) which have branching indices 1. The link L is 2-universal; therefore for any given closed orientable 3-manifold M there exists a branched covering q:M→S3 over L, of type {1,2}. Furthermore, since L is a sublink of the pseudo-branch cover, the branched covering p∘q:M→S3 is also of type {1,2}, implying that K is 2-universal. Part of the reason for studying 2-universal knots is the following. There exists a discrete universal group of hyperbolic isometries U (a discrete group of hyperbolic isometries G is universal if any closed orientable 3-manifold M is homeomorphic to the orbit space H3/H where H is a subgroup of G of finite index). The group U is generated by three 90∘ rotations. Since there are 3-manifolds which are not hyperbolic, any universal group has to contain rotations. The existence of a 2-universal hyperbolic knot would imply the existence of a discrete universal group of hyperbolic isometries that would only contain rotations by 180∘.
We construct a map from knots to (abstract) 2-knots which can be extended to higher dimensions; this map is the natural "knot" counterpart for "braid" theory of groups $G_{n}^{k}$. We construct a map from knots to (abstract) 2-knots which can be extended to higher dimensions; this map is the natural "knot" counterpart for "braid" theory of groups $G_{n}^{k}$.
We construct a map from knots to (abstract) 2-knots which can be extended to higher dimensions; this map is the natural knot counterpart for braid theory of groups $G_{n}^{k}$. We construct a map from knots to (abstract) 2-knots which can be extended to higher dimensions; this map is the natural knot counterpart for braid theory of groups $G_{n}^{k}$.
We show that every $\mathbb{Z}$-torsion free knot module is realized by a ribbon 2-knot with group of geometric dimension at most 2, and give some partial results on the characterization … We show that every $\mathbb{Z}$-torsion free knot module is realized by a ribbon 2-knot with group of geometric dimension at most 2, and give some partial results on the characterization of the knot modules of fibred ribbon 2-knots.
During the period from the end of the 1960s through to the beginning of the 1970s, Conway pursued the objective of forming a complete table of knots. As we have … During the period from the end of the 1960s through to the beginning of the 1970s, Conway pursued the objective of forming a complete table of knots. As we have seen in our discussions thus far, the knot invariants that had been discovered up to that point in time were not sufficient to accomplish this aim. Therefore, Conway pulled another jewel from his bag of cornucopia and introduced the concept of a tangle. Using this variation on a knot, a new class of knots could be defined: algebraic knots. By studying this class of knots, various Local problems were able to be solved, which led to a further jump in the level of understanding of knot theory. However, since there are knots that are not algebraic, the complete classification of knots could not be realized. Nevertheless, the introduction of this new research approach has had a significant impact on knot theory. In this chapter we shall investigate 2-bridge knots (or links), which are a special kind of algebraic knot obtained from trivial tangles.
The sheet number of a 2-knot is an analogous quantity to the crossing number of a 1-knot. We prove that (i) a 2-knot is trivial if and only if the … The sheet number of a 2-knot is an analogous quantity to the crossing number of a 1-knot. We prove that (i) a 2-knot is trivial if and only if the sheet number is equal to one, and (ii) there is no 2-knot with the sheet number two.
As a generalization of quandles, biquandles have given many invariants of classical/surface/virtual links. In this paper, we show that the fundamental quandle [Formula: see text] of any classical/surface link [Formula: … As a generalization of quandles, biquandles have given many invariants of classical/surface/virtual links. In this paper, we show that the fundamental quandle [Formula: see text] of any classical/surface link [Formula: see text] detects the fundamental biquandle [Formula: see text]; more precisely, there exists a functor [Formula: see text] from the category of quandles to that of biquandles such that [Formula: see text]. Then, we can expect invariants from biquandles to be reduced to those from quandles. In fact, we introduce a right-adjoint functor [Formula: see text] of [Formula: see text], which implies that the coloring number of a biquandle [Formula: see text] is equal to that of the quandle [Formula: see text].
The 2-twist spun trefoil is an example of a sphere that is knotted in 4-dimensional space. A proof is given in this paper that this sphere is distinct from the … The 2-twist spun trefoil is an example of a sphere that is knotted in 4-dimensional space. A proof is given in this paper that this sphere is distinct from the same sphere with its orientation reversed. Our proof is based on a state-sum invariant for knotted surfaces developed via a cohomology theory of racks and quandles (also known as distributive groupoids). A quandle is a set with a binary operation — the axioms of which model the Reidemeister moves in classical knot theory. Colorings of diagrams of knotted curves and surfaces by quandle elements, together with cocycles of quandles, are used to define state-sum invariants for knotted circles in $3$-space and knotted surfaces in $4$-space. Cohomology groups of various quandles are computed herein and applied to the study of the state-sum invariants. Non-triviality of the invariants is proved for a variety of knots and links, and conversely, knot invariants are used to prove non-triviality of cohomology for a variety of quandles.
Litherland has shown that if a knot is (+)-amphicheiral then its m-twist-spin is reversible. We show that, for classical knots, in many cases the converse holds. Litherland has shown that if a knot is (+)-amphicheiral then its m-twist-spin is reversible. We show that, for classical knots, in many cases the converse holds.
Given a tangle diagram of a classical knot K, we construct a surface diagram of any twist-spun 2-knot of K. From the crossings of the tangle diagram, we can get … Given a tangle diagram of a classical knot K, we construct a surface diagram of any twist-spun 2-knot of K. From the crossings of the tangle diagram, we can get information of the corresponding triple points of the surface diagram, which are used to compute cocycle invariants of twist-spun 2-knots.
Journal Article SOME HIGHER-DIMENSIONAL KNOTS WITH THE SAME HOMOTOPY GROUPS Get access C. McA. GORDON C. McA. GORDON Florida State UniversityTallahassee, Florida 32306 Search for other works by this author … Journal Article SOME HIGHER-DIMENSIONAL KNOTS WITH THE SAME HOMOTOPY GROUPS Get access C. McA. GORDON C. McA. GORDON Florida State UniversityTallahassee, Florida 32306 Search for other works by this author on: Oxford Academic Google Scholar The Quarterly Journal of Mathematics, Volume 24, Issue 1, 1973, Pages 411–422, https://doi.org/10.1093/qmath/24.1.411 Published: 01 January 1973 Article history Received: 04 July 1972 Published: 01 January 1973
structures on 2-dimensional orbifolds . . . . . . . .421 §3.The basic theory of Seifert fibre spaces 428 §4. structures on 2-dimensional orbifolds . . . . . . . .421 §3.The basic theory of Seifert fibre spaces 428 §4.
A rack, which is the algebraic distillation of two of the Reidemeister moves, is a set with a binary operation such that right multiplication is an automorphism. Any codimension two … A rack, which is the algebraic distillation of two of the Reidemeister moves, is a set with a binary operation such that right multiplication is an automorphism. Any codimension two link has a fundamental rack which contains more information than the fundamental group. Racks provide an elegant and complete algebraic framework in which to study links and knots in 3–manifolds, and also for the 3–manifolds themselves. Racks have been studied by several previous authors and have been called a variety of names. In this first paper of a series we consolidate the algebra of racks and show that the fundamental rack is a complete invariant for irreducible framed links in a 3–manifold and for the 3–manifold itself. We give some examples of computable link invariants derived from the fundamental rack and explain the connection of the theory of racks with that of braids.
The present paper contains a 'roof of Dehn's lemma and an analogous result that we call the sphere theorem, from which other theorems follow.' DEHN'S LEMMA. Let M be a … The present paper contains a 'roof of Dehn's lemma and an analogous result that we call the sphere theorem, from which other theorems follow.' DEHN'S LEMMA. Let M be a 3-manifold, compact or not, with boundary which may be empty, and in M let D be a 2-cell with self-intersections (singularities), having as boundary the simple closed polygonal curve C and such that there exists a closed neighborhood of C in D which is an annulus (i.e. no point of C is singular). Then there exists a 2-cell Do with boundary C, semi-linearly imbedded in M. SPHERE THEOREM. Let M be an orientable 3-manifold, compact or not, with boundary which may be empty, such that 7r2(M) # 0, and which can be semi-linearly2 imbedded in a 3-manifold N, having the following property: the commutator quotient group of any non-trivial (but not necessarily proper) finitely generated subgroup of 7r,(N) has an element of infinite order (n.b. in particular this holds if 7r,(N) = 1). Then there exists a 2-sphere S semi-linearly imbedded in M, such that3 S X 0 in M. Dehn's lemma was included in a 1910 paper of M. Dehn [4] p. 147, but in 1928 H. Kneser [13] p. 260, observed that Dehn's proof contained a serious gap. In 1935 and 1938 appeared two papers by I. Johansson [11], [12], on Dehn's lemma. In the second one, p. 659, he proves that, if Dehn's lemma holds for all orientable 3-manifolds, it then holds for all non-orientable ones. We now prove in this paper that Dehn's lemma holds for all orientable 3-manifolds. Our proof makes use also of I. Johansson's first paper. As far as the sphere theorem is concerned we have to remark that, to the best knowledge of this author, the first one to attempt a theorem of this kind was H. Kneser in 1928, [13] p. 257; however his proof does not seem to be conclusive. In 1937 S. Eilenberg [5] p. 242, Remark 1, observed a relation between the nonvanishing of the second homotopy group and the existence of a non-contractible 2-sphere. Finally in 1939 J. H. C. Whitehead [25] p. 161, posed a problem which stimulated the author to prove the sphere theorem, stated above. We emphasize that, if 7r,(N) is a free group4 then the hypotheses of the sphere theorem are fulfilled, according to the following NIELSEN-SCHREIER THEOREM. Every subgroup of a free group is itself a free group.5
We give a classification of 2-twist-spun spherical Montesinos knots. We give a classification of 2-twist-spun spherical Montesinos knots.
This paper contains some remarks about spinning which show, in particular, that the spun reef knot is equivalent to the spun granny. This paper contains some remarks about spinning which show, in particular, that the spun reef knot is equivalent to the spun granny.
Zeeman has shown that the complement of a twist-spun knot fibres over the circle. He also proves that the group of the 5-twist-spun trefoil is just the direct product of … Zeeman has shown that the complement of a twist-spun knot fibres over the circle. He also proves that the group of the 5-twist-spun trefoil is just the direct product of the fundamental group of the fibre with the integers. We generalise this by showing that, for torus knots, the group of the twist-spun knot is such a direct product whenever the fibre is a homology sphere. This then suggests the question (asked by Zeeman for the case of the 5-twist-spun trefoil) as to whether there is a corresponding product structure in the geometry. We answer in the negative.