Knot Group Epimorphisms DANIEL S
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The Subgroups of a Free Product of Two Groups with an Amalgamated Subgroup!1)
transactions of the american mathematical society Volume 150, July, 1970 THE SUBGROUPS OF A FREE PRODUCT OF TWO GROUPS WITH AN AMALGAMATED SUBGROUP!1) BY A. KARRASS AND D. SOLITAR Abstract. We prove that all subgroups H of a free product G of two groups A, B with an amalgamated subgroup V are obtained by two constructions from the inter- section of H and certain conjugates of A, B, and U. The constructions are those of a tree product, a special kind of generalized free product, and of a Higman-Neumann- Neumann group. The particular conjugates of A, B, and U involved are given by double coset representatives in a compatible regular extended Schreier system for G modulo H. The structure of subgroups indecomposable with respect to amalgamated product, and of subgroups satisfying a nontrivial law is specified. Let A and B have the property P and U have the property Q. Then it is proved that G has the property P in the following cases: P means every f.g. (finitely generated) subgroup is finitely presented, and Q means every subgroup is f.g.; P means the intersection of two f.g. subgroups is f.g., and Q means finite; P means locally indicable, and Q means cyclic. It is also proved that if A' is a f.g. normal subgroup of G not contained in U, then NU has finite index in G. 1. Introduction. In the case of a free product G = A * B, the structure of a subgroup H may be described as follows (see [9, 4.3]): there exist double coset representative systems {Da}, {De} for G mod (H, A) and G mod (H, B) respectively, and there exists a set of elements t\, t2,.. -
The Free Product of Groups with Amalgamated Subgroup Malnorrnal in a Single Factor
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF PURE AND APPLIED ALGEBRA Journal of Pure and Applied Algebra 127 (1998) 119-136 The free product of groups with amalgamated subgroup malnorrnal in a single factor Steven A. Bleiler*, Amelia C. Jones Portland State University, Portland, OR 97207, USA University of California, Davis, Davis, CA 95616, USA Communicated by C.A. Weibel; received 10 May 1994; received in revised form 22 August 1995 Abstract We discuss groups that are free products with amalgamation where the amalgamating subgroup is of rank at least two and malnormal in at least one of the factor groups. In 1971, Karrass and Solitar showed that when the amalgamating subgroup is malnormal in both factors, the global group cannot be two-generator. When the amalgamating subgroup is malnormal in a single factor, the global group may indeed be two-generator. If so, we show that either the non-malnormal factor contains a torsion element or, if not, then there is a generating pair of one of four specific types. For each type, we establish a set of relations which must hold in the factor B and give restrictions on the rank and generators of each factor. @ 1998 Published by Elsevier Science B.V. All rights reserved. 0. Introduction Baumslag introduced the term malnormal in [l] to describe a subgroup that intersects each of its conjugates trivially. Here we discuss groups that are free products with amalgamation where the amalgamating subgroup is of rank at least two and malnormal in at least one of the factor groups. -
Some Remarks on Cabling, Contact Structures, and Complex Curves
Proceedings of 14th G¨okova Geometry-Topology Conference pp. 49 – 59 Some remarks on cabling, contact structures, and complex curves Matthew Hedden Abstract. We determine the relationship between the contact structure induced by a fibered knot, K ⊂ S3, and the contact structures induced by its various cables. Understanding this relationship allows us to classify fibered cable knots which bound a properly embedded complex curve in the four-ball satisfying a genus constraint. This generalizes the well-known classification of links of plane curve singularities. 1. Introduction A well-known construction of Thurston and Winkelnkemper [ThuWin] associates a contact structure to an open book decomposition of a three-manifold. This allows us to talk about the contact structure associated to a fibered knot. Here, a fibered knot is a pair, (F, K) ⊂ Y , such that Y − K admits the structure of a fiber bundle over the circle with fibers isotopic to F and ∂F = K. We denote the contact structure associate to a fibered knot by ξF,K or, when the fiber surface is unambiguous, by ξK . Thus any operation on knots (or Seifert surfaces) which preserves the property of fiberedness induces an operation on contact structures. For instance, one can consider the Murasugi sum operation on surfaces-with-boundary (see [Gab] for definition). In this case, a result of Stallings [Sta] indicates that the Murasugi sum of two fiber surfaces is also fibered (a converse to this was proved by Gabai [Gab]). The effect on contact structures is given by a result of Torisu: Theorem 1.1. (Theorem 1.3 of [Tor].) Let (F1,∂F1) ⊂ Y1 (F2,∂F2) ⊂ Y2 be two fiber surfaces, and let (F1 ∗ F2,∂(F1 ∗ F2)) ⊂ Y1#Y2 denote any Murasugi sum. -
Arxiv:Hep-Th/9404101V3 21 Nov 1995
hep-th/9404101 April 1994 Chern-Simons Gauge Theory on Orbifolds: Open Strings from Three Dimensions ⋆ Petr Horavaˇ ∗ Enrico Fermi Institute University of Chicago 5640 South Ellis Avenue Chicago IL 60637, USA ABSTRACT Chern-Simons gauge theory is formulated on three dimensional Z2 orbifolds. The locus of singular points on a given orbifold is equivalent to a link of Wilson lines. This allows one to reduce any correlation function on orbifolds to a sum of more complicated correlation functions in the simpler theory on manifolds. Chern-Simons theory on manifolds is known arXiv:hep-th/9404101v3 21 Nov 1995 to be related to 2D CFT on closed string surfaces; here I show that the theory on orbifolds is related to 2D CFT of unoriented closed and open string models, i.e. to worldsheet orb- ifold models. In particular, the boundary components of the worldsheet correspond to the components of the singular locus in the 3D orbifold. This correspondence leads to a simple identification of the open string spectra, including their Chan-Paton degeneration, in terms of fusing Wilson lines in the corresponding Chern-Simons theory. The correspondence is studied in detail, and some exactly solvable examples are presented. Some of these examples indicate that it is natural to think of the orbifold group Z2 as a part of the gauge group of the Chern-Simons theory, thus generalizing the standard definition of gauge theories. E-mail address: [email protected] ⋆∗ Address after September 1, 1994: Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544. 1. Introduction Since the first appearance of the notion of “orbifolds” in Thurston’s 1977 lectures on three dimensional topology [1], orbifolds have become very appealing objects for physicists. -
An Introduction to Knot Theory and the Knot Group
AN INTRODUCTION TO KNOT THEORY AND THE KNOT GROUP LARSEN LINOV Abstract. This paper for the University of Chicago Math REU is an expos- itory introduction to knot theory. In the first section, definitions are given for knots and for fundamental concepts and examples in knot theory, and motivation is given for the second section. The second section applies the fun- damental group from algebraic topology to knots as a means to approach the basic problem of knot theory, and several important examples are given as well as a general method of computation for knot diagrams. This paper assumes knowledge in basic algebraic and general topology as well as group theory. Contents 1. Knots and Links 1 1.1. Examples of Knots 2 1.2. Links 3 1.3. Knot Invariants 4 2. Knot Groups and the Wirtinger Presentation 5 2.1. Preliminary Examples 5 2.2. The Wirtinger Presentation 6 2.3. Knot Groups for Torus Knots 9 Acknowledgements 10 References 10 1. Knots and Links We open with a definition: Definition 1.1. A knot is an embedding of the circle S1 in R3. The intuitive meaning behind a knot can be directly discerned from its name, as can the motivation for the concept. A mathematical knot is just like a knot of string in the real world, except that it has no thickness, is fixed in space, and most importantly forms a closed loop, without any loose ends. For mathematical con- venience, R3 in the definition is often replaced with its one-point compactification S3. Of course, knots in the real world are not fixed in space, and there is no interesting difference between, say, two knots that differ only by a translation. -
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. -
Fibered Ribbon Disks
FIBERED RIBBON DISKS KYLE LARSON AND JEFFREY MEIER Abstract. We study the relationship between fibered ribbon 1{knots and fibered ribbon 2{knots by studying fibered slice disks with handlebody fibers. We give a characterization of fibered homotopy-ribbon disks and give analogues of the Stallings twist for fibered disks and 2{knots. As an application, we produce infinite families of distinct homotopy-ribbon disks with homotopy equivalent exteriors, with potential relevance to the Slice-Ribbon Conjecture. We show that any fibered ribbon 2{ knot can be obtained by doubling infinitely many different slice disks (sometimes in different contractible 4{manifolds). Finally, we illustrate these ideas for the examples arising from spinning fibered 1{knots. 1. Introduction A knot K is fibered if its complement fibers over the circle (with the fibration well-behaved near K). Fibered knots have a long and rich history of study (for both classical knots and higher-dimensional knots). In the classical case, a theorem of Stallings ([Sta62], see also [Neu63]) states that a knot is fibered if and only if its group has a finitely generated commutator subgroup. Stallings [Sta78] also gave a method to produce new fibered knots from old ones by twisting along a fiber, and Harer [Har82] showed that this twisting operation and a type of plumbing is sufficient to generate all fibered knots in S3. Another special class of knots are slice knots. A knot K in S3 is slice if it bounds a smoothly embedded disk in B4 (and more generally an n{knot in Sn+2 is slice if it bounds a disk in Bn+3). -
Categorified Invariants and the Braid Group
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 143, Number 7, July 2015, Pages 2801–2814 S 0002-9939(2015)12482-3 Article electronically published on February 26, 2015 CATEGORIFIED INVARIANTS AND THE BRAID GROUP JOHN A. BALDWIN AND J. ELISENDA GRIGSBY (Communicated by Daniel Ruberman) Abstract. We investigate two “categorified” braid conjugacy class invariants, one coming from Khovanov homology and the other from Heegaard Floer ho- mology. We prove that each yields a solution to the word problem but not the conjugacy problem in the braid group. In particular, our proof in the Khovanov case is completely combinatorial. 1. Introduction Recall that the n-strand braid group Bn admits the presentation σiσj = σj σi if |i − j|≥2, Bn = σ1,...,σn−1 , σiσj σi = σjσiσj if |i − j| =1 where σi corresponds to a positive half twist between the ith and (i + 1)st strands. Given a word w in the generators σ1,...,σn−1 and their inverses, we will denote by σ(w) the corresponding braid in Bn. Also, we will write σ ∼ σ if σ and σ are conjugate elements of Bn. As with any group described in terms of generators and relations, it is natural to look for combinatorial solutions to the word and conjugacy problems for the braid group: (1) Word problem: Given words w, w as above, is σ(w)=σ(w)? (2) Conjugacy problem: Given words w, w as above, is σ(w) ∼ σ(w)? The fastest known algorithms for solving Problems (1) and (2) exploit the Gar- side structure(s) of the braid group (cf. -
Combinatorial Group Theory
Combinatorial Group Theory Charles F. Miller III March 5, 2002 Abstract These notes were prepared for use by the participants in the Workshop on Algebra, Geometry and Topology held at the Australian National University, 22 January to 9 February, 1996. They have subsequently been updated for use by students in the subject 620-421 Combinatorial Group Theory at the University of Melbourne. Copyright 1996-2002 by C. F. Miller. Contents 1 Free groups and presentations 3 1.1 Free groups . 3 1.2 Presentations by generators and relations . 7 1.3 Dehn’s fundamental problems . 9 1.4 Homomorphisms . 10 1.5 Presentations and fundamental groups . 12 1.6 Tietze transformations . 14 1.7 Extraction principles . 15 2 Construction of new groups 17 2.1 Direct products . 17 2.2 Free products . 19 2.3 Free products with amalgamation . 21 2.4 HNN extensions . 24 3 Properties, embeddings and examples 27 3.1 Countable groups embed in 2-generator groups . 27 3.2 Non-finite presentability of subgroups . 29 3.3 Hopfian and residually finite groups . 31 4 Subgroup Theory 35 4.1 Subgroups of Free Groups . 35 4.1.1 The general case . 35 4.1.2 Finitely generated subgroups of free groups . 35 4.2 Subgroups of presented groups . 41 4.3 Subgroups of free products . 43 4.4 Groups acting on trees . 44 5 Decision Problems 45 5.1 The word and conjugacy problems . 45 5.2 Higman’s embedding theorem . 51 1 5.3 The isomorphism problem and recognizing properties . 52 2 Chapter 1 Free groups and presentations In introductory courses on abstract algebra one is likely to encounter the dihedral group D3 consisting of the rigid motions of an equilateral triangle onto itself. -
An Introduction to Orbifolds
An introduction to orbifolds Joan Porti UAB Subdivide and Tile: Triangulating spaces for understanding the world Lorentz Center November 2009 An introduction to orbifolds – p.1/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. An introduction to orbifolds – p.2/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. ··· (there are other notions of orbifold in algebraic geometry, string theory or using grupoids) An introduction to orbifolds – p.2/20 Examples: tessellations of Euclidean plane Γ= h(x, y) → (x + 1, y), (x, y) → (x, y + 1)i =∼ Z2 Γ\R2 =∼ T 2 = S1 × S1 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 2 2 2 2 2 2 2 2 2 2 An introduction to orbifolds – p.3/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) An introduction to orbifolds – p.4/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) 2 4 2 6 An introduction to orbifolds – p.4/20 Definition Informal Definition • An orbifold O is a metrizable topological space equipped with an atlas modelled on Rn/Γ, Γ < O(n) finite, with some compatibility condition. -
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]. -
23. Mon, Mar. 10 the Free Product Has a Universal Property, Which Should Remind You of the Property of the Disjoint Union of Spaces X Y
23. Mon, Mar. 10 The free product has a universal property, which should remind you of the property of the disjoint union of spaces X Y . First, for any groups H and K, there are inclusion homomorphisms H H K and K Hq K. ! ⇤ ! ⇤ Proposition 23.1. Suppose that G is any group with homomorphisms ' : H G and H ! 'K : K G. Then there is a (unique) homomorphism Φ:H K G which restricts to the given! homomorphisms from H and K. ⇤ ! Our result from last time can be restated as follows: Proposition 23.2. Suppose that X = U V , where U and V are path-connected open subsets and both contain the basepoint x .IfU V is[ also path-connected, then the natural homomorphism 0 \ Φ:⇡ (U) ⇡ (V ) ⇡ (X) 1 ⇤ 1 ! 1 is surjective. Now that we have a surjective homomorphism to ⇡1(X), the next step is to understand the kernel N. Indeed, then the First Isomorphism Theorem will tell us that ⇡1(X) ⇠= ⇡1(U) ⇡1(V )/N . Here is one way to produce an element of the kernel. Consider a loop ↵ in U V . We can⇤ then consider \ its image ↵U ⇡1(U) and ↵V ⇡1(V ). Certainly these map to the same element of ⇡1(X), so 1 2 2 ↵U ↵V− is in the kernel. Proposition 23.3. With the same assumptions as above, the kernel K of ⇡1(U) ⇡1(V ) ⇡1(X) 1 ⇤ ! is the normal subgroup N generated by elements of the form ↵U ↵V− . 1 Recall that the normal subgroup generated by the elements ↵U ↵V− can be characterized either 1 as (1) the intersection of all normal subgroups containing the ↵U ↵V− or (2) the subgroup generated 1 1 by all conjugates g↵U ↵V− g− .