Ribbon n-knots with isomorphic quandles
Blake Karl Winter

TL;DR
This paper proves that for ribbon knottings of n-spheres with 1-handles in higher-dimensional spheres, isomorphic quandles imply stable equivalence after finitely many trivial connected sums.
Contribution
It establishes a link between quandle isomorphisms and stable equivalence of ribbon knottings in higher dimensions, extending previous understanding.
Findings
Isomorphic knot quandles imply stable equivalence after trivial sums.
The result applies to ribbon knottings of n-spheres with 1-handles.
Provides a new criterion for knot equivalence in higher dimensions.
Abstract
Let be ribbon knottings of -spheres with -handles in , . We show that if the knot quandles of these knots are isomorphic, then the ribbon knottings are stably equivalent, in the sense of Nakanishi and Nakagawa, after taking a finite number of connected sums with trivially embedded copies of .
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Taxonomy
TopicsGeometric and Algebraic Topology · Homotopy and Cohomology in Algebraic Topology · Mathematical Dynamics and Fractals
Ribbon -knots with isomorphic quandles
Blake K. Winter
Abstract.
Let be ribbon knottings of -spheres with -handles in , . We show that if the knot quandles of these knots are isomorphic, then the ribbon knottings are stably equivalent, in the sense of Nakanishi and Nakagawa, after taking a finite number of connected sums with trivially embedded copies of .
The author wishes to acknowledge Adam Sikora, William Menasco, Jason Manning, and Sam Nelson, for their recommendations on the writing of this paper.
1. Introduction
The fundamental quandle of a knot or link is a powerful invariant for classical links in , [3, 6]. It is also an invariant for links in any dimension. In this paper, we will consider ribbon -links, , in , under an equivalence relation wherein two links are considered to be equivalent if they are isotopic after taking the connected sum with a finite number of trivially embedded copies of . We will show that the quandle is a complete invariant for this equivalence relation: two ribbon links are equivalent iff they have isomorphic quandles. Furthermore, we will show that the isotopy takes on the special form of a stable equivalence, as defined in [7, 8].
2. Ribbon Links
Here we will review the definition of ribbon links. See [2, 7, 8] for further discussion of ribbon links in arbitrary dimensions.
Remark 1**.**
Throughout, we will use the notation to represent a closed -disk.
Intuitively, a ribbon presentation is a collection of embedded -disks, joined together by -handles that are attached to the boundaries of the disks, and which are allowed to pass through the interiors of the disks transversely. We will make this precise:
Let be an -manifold. Let be a set of disjoint oriented -disks . Let be a set of oriented -handles , with the following conditions:
- (1)
must be embedded in , with compatible orientations. 2. (2)
For all , the components of are a finite embedded collection of -disks embedded in , such that each component separates from .
This implies that is contained in the interior of the image of . Such intersections between a handle and a base are called ribbon intersections or ribbon singularities. A handle can intersect any number of bases in ribbon intersections, and it can intersect the same base multiple times (or zero). We will in general identify the maps and with their images.
Definition 2**.**
The disks in are called bases, while the elements of are called (fusion) handles or bands.
Definition 3**.**
Given a set of bases and handles, the union of all the bases and handles together forms an immersed manifold, which is called a ribbon solid.
Any immersed -manifold which can be expressed in this form will also be called a ribbon solid. Note that a given ribbon solid might be able to be broken up into bases and handles in many different ways.
Definition 4**.**
Let be collections of bases and handles. Let be the link defined as . Then is called a ribbon link, and the pair are a ribbon presentation for .
In other words, is the closure of the boundary of the ribbon solid defined by the union of the bases and handles in the pair . We identify two ribbon presentations, and , of if there is a path between them in the space of ribbon presentations of This is equivalent to requiring that , , and that there exists an ambient isotopy of , , such that is the identity, and for all , , and .
Observe that since we require that the handles be glued to the bases in an orientation-preserving manner, will be orientable. Note also that for ribbon -links, the components of a ribbon link may not be ribbon knots themselves. However, for -links with , each component of a ribbon link will automatically be a ribbon knot.
Given a ribbon link , there are in general multiple ribbon presentations for . There are some distinct notions of equivalence for ribbon presentations. We will, for the moment, restrict our attention to knots; the generalization to links is straightforward.
Definition 5**.**
Let be a ribbon knot with ribbon presentations and . These presentations are called simply equivalent if , , and there exists an isotopy , , of , such that is the identity, and for all , , and .
That is, the isotopy maps handles to handles, and maps the boundaries of bases to the boundaries of bases. It need not map the interiors of the bases to one another, however. Thus, simple equivalence may create new intersections of handles with the interiors of bases, as illustrated in Fig. 1.
Lemma 6**.**
*For a ribbon presentation in a simply-connected manifold is determined uniquely up to simple equivalence by specifying the following ribbon data:
(a) the cardinality of and,
(b) for each , a specification of the base to which is attached, a specification of the base to which is attached, and a sequence of bases, through which the handle passes through, up to reversal of that sequence.*
Proof.
Clearly there is a ribbon presentation fulfilling every possible ribbon data as above. We need to show that such ribbon presentation is unique, up to simple equivalence. Note that for for each , the sequence determines the homotopy class of the handle in uniquely. Since and the core of the handle is -dimensional, the homotopy class of the handle determines its isotopy class as well. ∎
In this is of course not the case, since the homotopy class of the handle does not determine its isotopy class in . In addition, one must specify a cyclic ordering of handles glued to a base for .
There is a notion of equivalence between ribbon presentations called stable equivalence, defined by Nakanishi, [7].
Definition 7**.**
Two ribbon presentations are stably equivalent if they are related by simple equivalence, together with the following three changes, which are illustrated in Fig. 2:
- (1)
Add a new base with a handle starting on and terminating on any other base, without passing through any bases. 2. (2)
Handle pass*: Isotope through , leaving fixed.* 3. (3)
Handle slide*: If connects with , and has an end on , we may slide that end along over to .*
Observe that for a knotted -sphere, by Euler characteristic arguments. It is easy to check that for , a ribbon -knot will have the homeomorphism type of an -sphere with -handles attached.
Given a ribbon -knot , it is an open question whether any two ribbon presentations for are related by stable equivalence for . For the case , Nakanishi and Nakagawa provide a family of knots, each of which admits multiple ribbon presentations which are not stably equivalent, [8, 7].
3. Quandles
Definition 8**.**
A quandle, [3], (also called a distributive groupoid in [6]) consists of a set and a binary operation on such that for all , the following equalities hold.
- (1)
. 2. (2)
There is a unique such that . 3. (3)
.
When the operation is implied, we may denote the quandle by , suppressing the operation.
In general, it is common to denote the operation in any quandle by using the conjugation notation. For any quandle we may define . Analogously, we will denote the element stipulated by property (2) by , i.e. . By convention, we interpret .
Quandles as knot invariants were introduced in [3, 6]. Here we recall the definition of a quandle associated to a knot, as given by Joyce for classical knots in [3]. The geometric definition holds for any codimension- knot, however.
Let be a link in , with and assumed to be orientable, and let be an open tubular neighborhood of . Then is a manifold with boundary containing . The fundamental group of this space is called the link group. We will follow the convention that the product of two homotopy classes of paths goes from right to left, i.e. is the homotopy class of a path which follows and then . This will make it somewhat easier to discuss the action of the link group on the link quandle.
A meridian of is the boundary of the disk fibre of the tubular neighborhood of considered as a disk bundle over . Note that the orientations of and of determine an orientation of . A meridian is defined uniquely up to conjugation.
We define the quandle associated to the pair and a chosen base point as follows. The elements of are homotopy classes of paths in that start at and end in , where homotopies are required to preserve these two conditions. The quandle operation, , between two elements is defined as the homotopy class of , where the overbar indicates that the path is followed in reverse and is the meridian of passing through the endpoint of , cf. 3. It is a straightforward exercise to show that this binary operation is well-defined and it satisfies the definition of a quandle operation. We call the link quandle of (or the knot quandle if is a knot).
Note that there is a right action of on : is the equivalence class including the homotopy class of the path .
The following theorem was proved for classical knots in [3]. The arguments in [3] are easily generalized to any knots, as is done in [9]. As we will not be making use of this result, we will skip the proof here, referring interested readers to those two sources.
Theorem 9**.**
For knots, is determined by with its peripheral structure.
4. Ribbon -Knots with Isomorphic Quandles
Let us say that in a ribbon presentation a handle is a trivial handle if both ends are attached to the same base and can be isotoped so it does not meet any bases except at its ends. In other words, does not pass through any bases.
Definition 10**.**
Let be -knots in , and let . Let indicate the connected sum of copies of that are trivially embedded, that is, which bound embedded copies of . We will say that and are weakly equivalent if is isotopic to .
Note that in [5], weak equivalence is called “stable equivalence,” as gluing on copies of may be thought of as a stabilization of the knot. Because this term is also used to refer stable equivalence of ribbon presentations, we are adopting the term “weak equivalence” instead to avoid any confusion.
Definition 11**.**
Let be ribbon presentations for -links, . We will say that they are -weakly stably equivalent if they are stably equivalent after attaching trivial handles, and that they are weakly stably equivalent if they are -weakly stably equivalent for some finite .
Given a ribbon presentation , the bases in are a collection of embedded disks. We will say that a path in passes through a base if it intersects the interior of transversely. Note that in general position, a path can pass through a base positively or negatively, depending on whether it passes through it in the same direction as the normal vector or in the opposite direction.
Remark 12**.**
To specify a handle , it suffices to specify the starting base to which is glued, the signed intersections of the handle in the order it passes through bases, and the terminal base to which is glued. Any two handles meeting these conditions are smoothly isotopic and thus equivalent.
Theorem 13**.**
Let be a ribbon knot in , , of arbitrary genus. Suppose that admits a base and handle presentation with bases, and . Then is -weakly stably equivalent to an unknotted ribbon knot.
Proof.
Let be new trivial handles glued to , with all their ends connected to base . Perform handle slides so that starts on and terminates on , twisting them at the end so that they pass through bases equally many times positively as negatively. Let be a curve which travels to without passing through any bases, then follows the handle to (traveling through the same bases in the same order) and returns to the basepoint for the fundamental group without passing through any additional bases. Since , and since by construction is homologically trivial, bounds a disk in . Note in particular that this disk does not pass through the handles . This disk may be taken to be smooth and immersed by various approximation theorems, [4, Theorem 10.16, Theorem 10.21] and [1, Theorem 2.5]. By general position, this disk meets itself at most in isolated points. Sliding along this disk we may, by handle passes only, make into a handle connecting to without passing through any bases. Now all handles in may be moved by handle passes so they only pass through base , after which all other bases may be deleted after appropriate handle slides. But a ribbon presentation with a single base is always stably equivalent to the unknotted ribbon presentation. ∎
For a ribbon -knot with and ribbon presentation , there is a natural presentation for the knot quandle . This presentation is generated by the bases in and has one relation for each handle . The relation has the following form: let and be the starting and ending bases for , and let follow the word (here is a word in the bases in , where each base can appear positively or negatively, depending on whether the handle passes through it in a direction that agrees with the normal vector or opposite to it) as it moves from to . Then the relation is given by the equation . Geometrically, the generator corresponding to a base is given by an equivalence class of paths containing a path that goes from the basepoint to the base without passing through any other bases.
Theorem 14**.**
A ribbon -knot, , with ribbon presentation , has a knot quandle whose presentation is as described in the previous paragraph.
Proof.
This is proved by repeated application of the Van Kampen theorem. Alternately, it is not difficult to write down the double point curves in a projection of a ribbon knot where each base and handle is embedded under the projection. Then the double point curves correspond to handles passing through bases, and the relations may be worked out using the computations as shown in e.g. [2] (which are themselves based on the Van Kampen theorem). ∎
Remark 15**.**
Let be the quandle of a ribbon knot with presentation . To specify an element of , it suffices to specify a path by assuming that starts at the basepoint for the quandle, then specifying the ordered signed intersections of the path with the bases, and finally specifying on which base the path terminates.
This follows from general position arguments.
Remark 16**.**
We will denote the generator of a quandle corresponding to a base by using the same symbol; whether we are referring to the base or the quandle element will be clear from context.
Throughout the following, we will make extensive use of the following fact, which forms part of the geometric definition of the quandle of a knot complement. Let be a knot in , and let be the basepoint for the quandle . Let be the closure of a tubular neighborhood of . Recall that elements of the quandle are equivalence classes of paths which start on and terminate on . Two paths are equivalent as quandle elements iff they are homotopic through paths starting on and terminating on . Therefore, there exists a disk whose boundary consists of the union of with some path on . By various approximation theorems, [4, Theorem 10.16, Theorem 10.21] and [1, Theorem 2.5], we may assume this disk is smooth and immersed, and therefore by general position we may assume that is immersed and embedded except at a finite number of points, provided that . In fact for , general position arguments show that the disk can be taken to be embedded. Thus, the homotopy may be taken to be a homotopy through embedded paths, that is, a smooth isotopy of the path which traces out the disk .
We will repeatedly make use of the existence of such isotopies. All our applications are essentially uses of the following construction. Let be a ribbon presentation for . Let be handles such that and are ribbon presentations. Recall that a handle is an embedding of into such that is embedded in elements of . We will refer to as the core of . Observe that once the core of is specified, the handle itself is specified up to isotopy. Now suppose that have the property that . Let . Now determine quandle elements for .
Lemma 17**.**
Let , , be as described in the previous paragraph, and suppose that as elements of . Then there is a stable equivalence between and which involves only performing handle slides and passes isotoping to agree with .
Proof.
Let be the homotopy disk giving the equivalence of as elements of . This is a disk in the complement of . This disk may be perturbed so that its interior does not meets or , by general position arguments. Now intersects itself only in isolated points. Therefore, we may slide along this disk until it agrees with . During this process we will be sliding the end of the core of around on so we may perform some handle slides, as well as passes. ∎
Remark 18**.**
This argument cannot be extended to an argument for an analogous result for handles and that are already part of the ribbon presentation for . This is because in that case, the disk might pass through the interior of the handle or themselves. This cannot happen in the above case because are homotopic using a homotopy in the complement of , and, therefore, the homotopy cannot move the path through the interior of or since they are not handles for the presentation of .
Lemma 19**.**
Let be a ribbon -knot, , with ribbon presentation . Suppose that the quandle is generated by . Then, by adding a trivial handle to , we can merge and some into a single base through stable equivalence.
Proof.
Let be the new trivial handle, with both ends on . We may isotope so that the midpoint of the core of passes through the basepoint for the quandle while it remains a trivial handle. Now the path that goes from the basepoint to is equivalent in the quandle to a path from the basepoint to some other base which does not pass through the base , since generates the quandle. There is a quandle homotopy disk connecting these two paths which does not intersect (since all the relations in the quandle are geometrically given by the handles in ). We may slide the portion of between its midpoint and terminal point along this disk so that it joins and and follows the path , using the method described in Lemma 17. Since does not pass through , we can now perform handle passes through so that any handles passing through are moved to instead pass through . Once no longer contains any ribbon intersections, we may collapse one of the attaching handles to join it to an adjacent base. ∎
Theorem 20**.**
Let be ribbon -knots, , with ribbon presentations , respectively, of the same genus, such that the identity map on induces a quandle isomorphism between and . Then they are -weakly stably equivalent.
Proof.
Let connect . Attach a trivial handle to with both ends on . Let be isotoped so that the midpoint of its core passes through the basepoint for the quandle. The path from to following the core of and the path from to following are homotopic in the quandle ; thus we may slide ’s latter half along the homotopy disk, as described in Lemma 17. After this is done, will pass through exactly the same bases as . Repeat this for each handle in . Then perform the same operation using the trivial handles we have added to , modifying them so that all the handles originally in are now in as well. We now have all the handles in in as well, and all the handles in have been added to . Thus we have modified the two ribbon presentations so they have identical sets of bases and handles. ∎
Theorem 21**.**
Let be ribbon -knots, , with ribbon presentations of the same genus , respectively. Let be a function which extends to a quandle isomorphism . Then are -weakly stably equivalent with bases given by and respectively.
Proof.
For each , we obtain a quandle element . The are paths from the basepoint to some base . Create a trivial base connected by a handle to by a handle that does not pass through any bases. Then we may slide so that it terminates on . Clearly does not pass through . Therefore, we can pull back along , contracting the quandle element, until we have so isotoped such that is now a path from the basepoint to which does not pass through any bases.
Now the collection of s generates the quandle . By Lemma 19, is -weakly stably equivalent to a knot whose bases consist of exactly the s. Add an equal number of handles to . Then by Theorem 20 the result follows. ∎
Theorem 22**.**
Let be ribbon -knots (of the same genus) with ribbon presentations , respectively. Suppose the knot quandles and are isomorphic. Then and are -weakly stably equivalent.
Proof.
Let be the isomorphism. Then defines a map from to defined by sending (where we send the base to the quandle element which its standard generator is sent to by . Now apply Theorem 21. ∎
Corollary 23**.**
Let be as in the previous theorem, but with possibly different genus. Then they are weakly stably equivalent.
Corollary 24**.**
Let be two ribbon presentations for a single -knot , . Then they are -weakly stably equivalent.
This is related to the question posed in [7], where it is asked whether two ribbon presentations for the same -knot with are necessarily stably equivalent. In [8] an infinite family of examples are constructed showing that two ribbon presentations for the same -knot do not need to be stably equivalent. In fact examples are constructed of -knots with stably inequivalent ribbon presentations for any .
Remark 25**.**
These results all hold in their natural generalizations to ribbon links with multiple components.
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