NOTES on the LEVINE-TRISTRAM SIGNATURE FUNCTION These
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Slicing Bing Doubles
Algebraic & Geometric Topology 6 (2006) 3001–999 3001 Slicing Bing doubles DAVID CIMASONI Bing doubling is an operation which produces a 2–component boundary link B.K/ from a knot K. If K is slice, then B.K/ is easily seen to be boundary slice. In this paper, we investigate whether the converse holds. Our main result is that if B.K/ is boundary slice, then K is algebraically slice. We also show that the Rasmussen invariant can tell that certain Bing doubles are not smoothly slice. 57M25; 57M27 Introduction Bing doubling [2] is a standard construction which, given a knot K in S 3 , produces a 2–component oriented link B.K/ as illustrated below. (See Section 1 for a precise definition.) K B.K/ Figure 1: The figure eight knot and its Bing double It is easy to check that if the knot K is slice, then the link B.K/ is slice. Does the converse hold ? An affirmative answer to this question seems out of reach. However, a result obtained independently by S Harvey [9] and P Teichner [22] provides a first step in this direction. 1 Recall that the Levine–Tristram signature of a knot K is the function K S ޚ 1 W ! defined as follows: for ! S , K .!/ is given by the signature of the Hermitian 2 matrix .1 !/A .1 !/A , where A is a Seifert matrix for K and A denotes the C transposed matrix. Published: December 2006 DOI: 10.2140/agt.2006.6.3001 3002 David Cimasoni Theorem (Harvey [9], Teichner [22]) If B.K/ is slice, then the integral over S 1 of the Levine–Tristram signature of K is zero. -
Arxiv:Math/0307077V4
Table of Contents for the Handbook of Knot Theory William W. Menasco and Morwen B. Thistlethwaite, Editors (1) Colin Adams, Hyperbolic Knots (2) Joan S. Birman and Tara Brendle, Braids: A Survey (3) John Etnyre Legendrian and Transversal Knots (4) Greg Friedman, Knot Spinning (5) Jim Hoste, The Enumeration and Classification of Knots and Links (6) Louis Kauffman, Knot Diagramitics (7) Charles Livingston, A Survey of Classical Knot Concordance (8) Lee Rudolph, Knot Theory of Complex Plane Curves (9) Marty Scharlemann, Thin Position in the Theory of Classical Knots (10) Jeff Weeks, Computation of Hyperbolic Structures in Knot Theory arXiv:math/0307077v4 [math.GT] 26 Nov 2004 A SURVEY OF CLASSICAL KNOT CONCORDANCE CHARLES LIVINGSTON In 1926 Artin [3] described the construction of certain knotted 2–spheres in R4. The intersection of each of these knots with the standard R3 ⊂ R4 is a nontrivial knot in R3. Thus a natural problem is to identify which knots can occur as such slices of knotted 2–spheres. Initially it seemed possible that every knot is such a slice knot and it wasn’t until the early 1960s that Murasugi [86] and Fox and Milnor [24, 25] succeeded at proving that some knots are not slice. Slice knots can be used to define an equivalence relation on the set of knots in S3: knots K and J are equivalent if K# − J is slice. With this equivalence the set of knots becomes a group, the concordance group of knots. Much progress has been made in studying slice knots and the concordance group, yet some of the most easily asked questions remain untouched. -
Ribbon Concordances and Doubly Slice Knots
Ribbon concordances and doubly slice knots Ruppik, Benjamin Matthias Advisors: Arunima Ray & Peter Teichner The knot concordance group Glossary Definition 1. A knot K ⊂ S3 is called (topologically/smoothly) slice if it arises as the equatorial slice of a (locally flat/smooth) embedding of a 2-sphere in S4. – Abelian invariants: Algebraic invari- Proposition. Under the equivalence relation “K ∼ J iff K#(−J) is slice”, the commutative monoid ants extracted from the Alexander module Z 3 −1 A (K) = H1( \ K; [t, t ]) (i.e. from the n isotopy classes of o connected sum S Z K := 1 3 , # := oriented knots S ,→S of knots homology of the universal abelian cover of the becomes a group C := K/ ∼, the knot concordance group. knot complement). The neutral element is given by the (equivalence class) of the unknot, and the inverse of [K] is [rK], i.e. the – Blanchfield linking form: Sesquilin- mirror image of K with opposite orientation. ear form on the Alexander module ( ) sm top Bl: AZ(K) × AZ(K) → Q Z , the definition Remark. We should be careful and distinguish the smooth C and topologically locally flat C version, Z[Z] because there is a huge difference between those: Ker(Csm → Ctop) is infinitely generated! uses that AZ(K) is a Z[Z]-torsion module. – Levine-Tristram-signature: For ω ∈ S1, Some classical structure results: take the signature of the Hermitian matrix sm top ∼ ∞ ∞ ∞ T – There are surjective homomorphisms C → C → AC, where AC = Z ⊕ Z2 ⊕ Z4 is Levine’s algebraic (1 − ω)V + (1 − ω)V , where V is a Seifert concordance group. -
Fibered Knots and Potential Counterexamples to the Property 2R and Slice-Ribbon Conjectures
Fibered knots and potential counterexamples to the Property 2R and Slice-Ribbon Conjectures with Bob Gompf and Abby Thompson June 2011 Berkeley FreedmanFest Theorem (Gabai 1987) If surgery on a knot K ⊂ S3 gives S1 × S2, then K is the unknot. Question: If surgery on a link L of n components gives 1 2 #n(S × S ), what is L? Homology argument shows that each pair of components in L is algebraically unlinked and the surgery framing on each component of L is the 0-framing. Conjecture (Naive) 1 2 If surgery on a link L of n components gives #n(S × S ), then L is the unlink. Why naive? The result of surgery is unchanged when one component of L is replaced by a band-sum to another. So here's a counterexample: The 4-dimensional view of the band-sum operation: Integral surgery on L ⊂ S3 $ 2-handle addition to @B4. Band-sum operation corresponds to a 2-handle slide U' V' U V Effect on dual handles: U slid over V $ V 0 slid over U0. The fallback: Conjecture (Generalized Property R) 3 1 2 If surgery on an n component link L ⊂ S gives #n(S × S ), then, perhaps after some handle-slides, L becomes the unlink. Conjecture is unknown even for n = 2. Questions: If it's not true, what's the simplest counterexample? What's the simplest knot that could be part of a counterexample? A potential counterexample must be slice in some homotopy 4-ball: 3 S L 3-handles L 2-handles Slice complement is built from link complement by: attaching copies of (D2 − f0g) × D2 to (D2 − f0g) × S1, i. -
Berge–Gabai Knots and L–Space Satellite Operations
BERGE-GABAI KNOTS AND L-SPACE SATELLITE OPERATIONS JENNIFER HOM, TYE LIDMAN, AND FARAMARZ VAFAEE Abstract. Let P (K) be a satellite knot where the pattern, P , is a Berge-Gabai knot (i.e., a knot in the solid torus with a non-trivial solid torus Dehn surgery), and the companion, K, is a non- trivial knot in S3. We prove that P (K) is an L-space knot if and only if K is an L-space knot and P is sufficiently positively twisted relative to the genus of K. This generalizes the result for cables due to Hedden [Hed09] and the first author [Hom11]. 1. Introduction In [OS04d], Oszv´ath and Szab´ointroduced Heegaard Floer theory, which produces a set of invariants of three- and four-dimensional manifolds. One example of such invariants is HF (Y ), which associates a graded abelian group to a closed 3-manifold Y . When Y is a rational homologyd three-sphere, rk HF (Y ) ≥ |H1(Y ; Z)| [OS04c]. If equality is achieved, then Y is called an L-space. Examples included lens spaces, and more generally, all connected sums of manifolds with elliptic geometry [OS05]. L-spaces are of interest for various reasons. For instance, such manifolds do not admit co-orientable taut foliations [OS04a, Theorem 1.4]. A knot K ⊂ S3 is called an L-space knot if it admits a positive L-space surgery. Any knot with a positive lens space surgery is then an L-space knot. In [Ber], Berge gave a conjecturally complete list of knots that admit lens space surgeries, which includes all torus knots [Mos71]. -
RASMUSSEN INVARIANTS of SOME 4-STRAND PRETZEL KNOTS Se
Honam Mathematical J. 37 (2015), No. 2, pp. 235{244 http://dx.doi.org/10.5831/HMJ.2015.37.2.235 RASMUSSEN INVARIANTS OF SOME 4-STRAND PRETZEL KNOTS Se-Goo Kim and Mi Jeong Yeon Abstract. It is known that there is an infinite family of general pretzel knots, each of which has Rasmussen s-invariant equal to the negative value of its signature invariant. For an instance, homo- logically σ-thin knots have this property. In contrast, we find an infinite family of 4-strand pretzel knots whose Rasmussen invariants are not equal to the negative values of signature invariants. 1. Introduction Khovanov [7] introduced a graded homology theory for oriented knots and links, categorifying Jones polynomials. Lee [10] defined a variant of Khovanov homology and showed the existence of a spectral sequence of rational Khovanov homology converging to her rational homology. Lee also proved that her rational homology of a knot is of dimension two. Rasmussen [13] used Lee homology to define a knot invariant s that is invariant under knot concordance and additive with respect to connected sum. He showed that s(K) = σ(K) if K is an alternating knot, where σ(K) denotes the signature of−K. Suzuki [14] computed Rasmussen invariants of most of 3-strand pret- zel knots. Manion [11] computed rational Khovanov homologies of all non quasi-alternating 3-strand pretzel knots and links and found the Rasmussen invariants of all 3-strand pretzel knots and links. For general pretzel knots and links, Jabuka [5] found formulas for their signatures. Since Khovanov homologically σ-thin knots have s equal to σ, Jabuka's result gives formulas for s invariant of any quasi- alternating− pretzel knot. -
Knots and Links in Lens Spaces
Alma Mater Studiorum Università di Bologna Dottorato di Ricerca in MATEMATICA Ciclo XXVI Settore Concorsuale di afferenza: 01/A2 Settore Scientifico disciplinare: MAT/03 Knots and links in lens spaces Tesi di Dottorato presentata da: Enrico Manfredi Coordinatore Dottorato: Relatore: Prof.ssa Prof. Giovanna Citti Michele Mulazzani Esame Finale anno 2014 Contents Introduction 1 1 Representation of lens spaces 9 1.1 Basic definitions . 10 1.2 A lens model for lens spaces . 11 1.3 Quotient of S3 model . 12 1.4 Genus one Heegaard splitting model . 14 1.5 Dehn surgery model . 15 1.6 Results about lens spaces . 17 2 Links in lens spaces 19 2.1 General definitions . 19 2.2 Mixed link diagrams . 22 2.3 Band diagrams . 23 2.4 Grid diagrams . 25 3 Disk diagram and Reidemeister-type moves 29 3.1 Disk diagram . 30 3.2 Generalized Reidemeister moves . 32 3.3 Standard form of the disk diagram . 36 3.4 Connection with band diagram . 38 3.5 Connection with grid diagram . 42 4 Group of links in lens spaces via Wirtinger presentation 47 4.1 Group of the link . 48 i ii CONTENTS 4.2 First homology group . 52 4.3 Relevant examples . 54 5 Twisted Alexander polynomials for links in lens spaces 57 5.1 The computation of the twisted Alexander polynomials . 57 5.2 Properties of the twisted Alexander polynomials . 59 5.3 Connection with Reidemeister torsion . 61 6 Lifting links from lens spaces to the 3-sphere 65 6.1 Diagram for the lift via disk diagrams . 66 6.2 Diagram for the lift via band and grid diagrams . -
Order 2 Algebraically Slice Knots 1 Introduction
ISSN 1464-8997 (on line) 1464-8989 (printed) 335 Geometry & Topology Monographs Volume 2: Proceedings of the Kirbyfest Pages 335–342 Order 2 Algebraically Slice Knots Charles Livingston Abstract The concordance group of algebraically slice knots is the sub- group of the classical knot concordance group formed by algebraically slice knots. Results of Casson and Gordon and of Jiang showed that this group contains in infinitely generated free (abelian) subgroup. Here it is shown that the concordance group of algebraically slice knots also contain elements of finite order; in fact it contains an infinite subgroup generated by elements of order 2. AMS Classification 57M25; 57N70, 57Q20 Keywords Concordance, concordance group, slice, algebraically slice 1 Introduction The classical knot concordance group, C , was defined by Fox [5] in 1962. The work of Fox and Milnor [6], along with that of Murasugi [18] and Levine [14, 15], revealed fundamental aspects of the structure of C . Since then there has been tremendous progress in 3– and 4–dimensional geometric topology, yet nothing more is now known about the underlying group structure of C than was known in 1969. In this paper we will describe new and unexpected classes of order 2 in C . What is known about C is quickly summarized. It is a countable abelian group. ∞ ∞ ∞ According to [15] there is a surjective homomorphism of φ: C → Z ⊕Z2 ⊕Z4 . The results of [6] quickly yield an infinite set of elements of order 2 in C , all of which are mapped to elements of order 2 by φ. The results just stated, and their algebraic consequences, present all that is known concerning the purely algebraic structure of C in either the smooth or topological locally flat category. -
Arxiv:1809.04186V2 [Math.GT] 3 Jan 2021
SATELLITES OF INFINITE RANK IN THE SMOOTH CONCORDANCE GROUP MATTHEW HEDDEN AND JUANITA PINZÓN-CAICEDO Abstract. We conjecture that satellite operations are either constant or have infinite rank in the concordance group. We reduce this to the difficult case of winding number zero satellites, and use SO(3) gauge theory to provide a general criterion sufficient for the image of a satellite operation to generate an infinite rank subgroup of the smooth concordance group C. Our criterion applies widely; notably to many unknotted patterns for which the corresponding operators on the topological concordance group are zero. We raise some questions and conjectures regarding satellite operators and their interaction with concordance. 1. Introduction Oriented knots are said to be concordant if they cobound a properly embedded cylinder in [0; 1] × S3. One can vary the regularity of the embeddings, and typically one considers either smooth or locally flat continuous embeddings. Either choice defines an equivalence relation under which the set of knots becomes an abelian group using the connected sum operation. These concordance groups of knots are intensely studied, with strong motivation provided by the profound distinction between the groups one defines in the topologically locally flat and smooth categories, respectively. Indeed, many questions pertaining to 4– manifolds with small topology (like the 4–sphere) can be recast or addressed in terms of concordance. Despite the efforts of many mathematicians, the concordance groups are still rather poorly understood. In both categories, for instance, the basic question of whether the groups possess elements of any finite order other than two remains open. -
Alexander Polynomial, Finite Type Invariants and Volume of Hyperbolic
ISSN 1472-2739 (on-line) 1472-2747 (printed) 1111 Algebraic & Geometric Topology Volume 4 (2004) 1111–1123 ATG Published: 25 November 2004 Alexander polynomial, finite type invariants and volume of hyperbolic knots Efstratia Kalfagianni Abstract We show that given n > 0, there exists a hyperbolic knot K with trivial Alexander polynomial, trivial finite type invariants of order ≤ n, and such that the volume of the complement of K is larger than n. This contrasts with the known statement that the volume of the comple- ment of a hyperbolic alternating knot is bounded above by a linear function of the coefficients of the Alexander polynomial of the knot. As a corollary to our main result we obtain that, for every m> 0, there exists a sequence of hyperbolic knots with trivial finite type invariants of order ≤ m but ar- bitrarily large volume. We discuss how our results fit within the framework of relations between the finite type invariants and the volume of hyperbolic knots, predicted by Kashaev’s hyperbolic volume conjecture. AMS Classification 57M25; 57M27, 57N16 Keywords Alexander polynomial, finite type invariants, hyperbolic knot, hyperbolic Dehn filling, volume. 1 Introduction k i Let c(K) denote the crossing number and let ∆K(t) := Pi=0 cit denote the Alexander polynomial of a knot K . If K is hyperbolic, let vol(S3 \ K) denote the volume of its complement. The determinant of K is the quantity det(K) := |∆K(−1)|. Thus, in general, we have k det(K) ≤ ||∆K (t)|| := X |ci|. (1) i=0 It is well know that the degree of the Alexander polynomial of an alternating knot equals twice the genus of the knot. -
On Signatures of Knots
1 ON SIGNATURES OF KNOTS Andrew Ranicki (Edinburgh) http://www.maths.ed.ac.uk/eaar For Cherry Kearton Durham, 20 June 2010 2 MR: Publications results for "Author/Related=(kearton, C*)" http://www.ams.org/mathscinet/search/publications.html?arg3=&co4... Matches: 48 Publications results for "Author/Related=(kearton, C*)" MR2443242 (2009f:57033) Kearton, Cherry; Kurlin, Vitaliy All 2-dimensional links in 4-space live inside a universal 3-dimensional polyhedron. Algebr. Geom. Topol. 8 (2008), no. 3, 1223--1247. (Reviewer: J. P. E. Hodgson) 57Q37 (57Q35 57Q45) MR2402510 (2009k:57039) Kearton, C.; Wilson, S. M. J. New invariants of simple knots. J. Knot Theory Ramifications 17 (2008), no. 3, 337--350. 57Q45 (57M25 57M27) MR2088740 (2005e:57022) Kearton, C. $S$-equivalence of knots. J. Knot Theory Ramifications 13 (2004), no. 6, 709--717. (Reviewer: Swatee Naik) 57M25 MR2008881 (2004j:57017)( Kearton, C.; Wilson, S. M. J. Sharp bounds on some classical knot invariants. J. Knot Theory Ramifications 12 (2003), no. 6, 805--817. (Reviewer: Simon A. King) 57M27 (11E39 57M25) MR1967242 (2004e:57029) Kearton, C.; Wilson, S. M. J. Simple non-finite knots are not prime in higher dimensions. J. Knot Theory Ramifications 12 (2003), no. 2, 225--241. 57Q45 MR1933359 (2003g:57008) Kearton, C.; Wilson, S. M. J. Knot modules and the Nakanishi index. Proc. Amer. Math. Soc. 131 (2003), no. 2, 655--663 (electronic). (Reviewer: Jonathan A. Hillman) 57M25 MR1803365 (2002a:57033) Kearton, C. Quadratic forms in knot theory.t Quadratic forms and their applications (Dublin, 1999), 135--154, Contemp. Math., 272, Amer. Math. Soc., Providence, RI, 2000. -
Alternating Knots
ALTERNATING KNOTS WILLIAM W. MENASCO Abstract. This is a short expository article on alternating knots and is to appear in the Concise Encyclopedia of Knot Theory. Introduction Figure 1. P.G. Tait's first knot table where he lists all knot types up to 7 crossings. (From reference [6], courtesy of J. Hoste, M. Thistlethwaite and J. Weeks.) 3 ∼ A knot K ⊂ S is alternating if it has a regular planar diagram DK ⊂ P(= S2) ⊂ S3 such that, when traveling around K , the crossings alternate, over-under- over-under, all the way along K in DK . Figure1 show the first 15 knot types in P. G. Tait's earliest table and each diagram exhibits this alternating pattern. This simple arXiv:1901.00582v1 [math.GT] 3 Jan 2019 definition is very unsatisfying. A knot is alternating if we can draw it as an alternating diagram? There is no mention of any geometric structure. Dissatisfied with this characterization of an alternating knot, Ralph Fox (1913-1973) asked: "What is an alternating knot?" black white white black Figure 2. Going from a black to white region near a crossing. 1 2 WILLIAM W. MENASCO Let's make an initial attempt to address this dissatisfaction by giving a different characterization of an alternating diagram that is immediate from the over-under- over-under characterization. As with all regular planar diagrams of knots in S3, the regions of an alternating diagram can be colored in a checkerboard fashion. Thus, at each crossing (see figure2) we will have \two" white regions and \two" black regions coming together with similarly colored regions being kitty-corner to each other.