The 250 Knots with up to 10 Crossings
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The 250 Knots with up to 10 Crossings
Andrey Boris Khesin
University of Toronto
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The list of knots with up to 10 crossings is commonly referred to as the Rolfsen Table. This paper presents a way to generate the Rolfsen table in a simple, clear, and reproducible manner. The methods we use are similar to those used by J. Hoste, M. Thistlethwaite, and J. Weeks in [1]. The difference between our methods comes from the fact that [1] uses a more complicated algorithm to be able to find all the knots with up to 17 crossings, while our approach demonstrates a simpler way to find the knots up to 10 crossings. We do this by generating all planar knot diagrams with up to 10 crossings and applying several simplifications to group the knot diagrams into equivalence classes. From these classes, we generate the full list of candidate knots and reduce it with several sets of moves. Lastly, we use invariants to show that each of the 250 diagrams generated is distinct, proving that there are exactly 250 knots with 10 crossings or fewer. Though the algorithms used could be made more efficient, readability was chosen over speed for simplicity and reproducibility.
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I Introduction
The Rolfsen table is the list of the 250 knots with 10 crossings or fewer. Here we attempt to generate it and prove its completeness by using a computer algorithm. This has been accomplished several times in the past. A notable example is [1], where J. Hoste, M. Thistlethwaite, and J. Weeks found all of the knots with up to 17 crossings. The methods we use are far less advanced, which allows us to effect a less intensive computation, finding the knots with up to 10 crossings, but use a simpler algorithm to do accomplish this.
Although it is possible to compute the Rolfsen table by hand, it is a rather tedious task. Our calculation is made possible by using a computer. To demonstrate a method of generating the Rolfsen table, we create a simple algorithm for finding all 250 knots with up to 10 crossings, partially sacrificing efficiency in the process.
We begin our reconstruction of the Rolfsen table by considering which knot diagrams could potentially be included in the table. There are only a finite number of ways to draw a knot diagram with a given number of crossings. Additionally, many of these knot diagrams are reducible, which means that they are equivalent to other knot diagrams with fewer crossings.
There are far more than 250 knot diagrams with up to 10 crossings, even after only irreducible knot diagrams are considered. The reason for this is that there are several moves that can transform one knot diagram into an equivalent one. Two knot diagrams are equivalent if and only if there exists a series of such moves that transforms one of the diagrams into the other.
Reidemeister Moves
First Second Third
Crossing NumberPreserving Moves
Flype 2–Pass
Crossing NumberReducing Moves
(2, 1)–Pass (3, 2)–Pass
Right Left
The first manner in which we simplify the list of knot diagrams is by
eliminating knot diagrams that are mirror images of each other.
For example, the righthanded and lefthanded trefoils are not equivalent as it
is impossible to turn one into the other (see Fig. 2).
We only include one of the two in the Rolfsen table.
The notation we use to represent a knot diagram does not encode the handedness
of the knot so this is not an issue.
For any two knot diagrams and , we cut at some point to create ends and and we cut at some point to create ends and . Joining to and to results in one larger knot, . We say that and are knot factors of . The commutative operation of joining and to create is called knot composition. Knots that cannot be decomposed into two knot factors other than themselves and the unknot are called prime. If they can be decomposed this way, they are called composite (see Fig. 3). We only include prime knots in our tabulation.
Lastly, we group knots into equivalence classes based on whether or not there exists a series of moves that transform one knot diagram into another (see Fig. 1). Out of each of these equivalence classes, we select one knot to include in our tabulation. Having done this, all that remains is proving that our list contains no remaining equivalent knot diagrams.
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II MD Codes
The first thing we need to do is to establish is a way to efficiently represent a knot diagram with some sort of notation. This notation must be relatively easy for both humans and computers to work with.
In [1], a notation is used to represent an crossing knot diagram with integers. This notation is called Dowker notation. Its density and simplicity make it convenient for our purposes.
For an crossing knot diagram, its representation in Dowker notation is constructed as follows. We start by picking an arbitrary point on one of the knot diagram’s edges as well as an arbitrary direction along that edge. We then move along the knot diagram, moving along each edge, until we have traveled along all edges and have returned to our starting point. Note that we will pass each crossing twice, once under and once over. Each time we pass a crossing, we consider the number of crossings that we have encountered so far and write that number down at the crossing that we are passing. In other words, when we encounter our first crossing, we write down the number 1 at that point. It is important to distinguish between writing the number on the upper or the lower strand of a crossing. If we passed the first crossing while traveling along the upper strand, we write down the number 1 on the upper strand and vice versa. Continuing, we would write down the number 2 at the next crossing we encounter. We would end up writing each number from 1 to exactly once. Furthermore, these numbers would be grouped into pairs, as there would be two numbers written at each of the crossings.
Note that since any two closed curves intersect in an even number of places, it follows that the pair of numbers written at each crossing will contain one odd number and one even number. If this were not the case then we would be able to leave a crossing, travel in a closed loop, and come back to that crossing having encountered an odd number of crossings along the way, which is not possible.
The pairs of numbers have no order, so sorting them in ascending order by
comparing the odd value in each pair does not sacrifice any information.
It then follows that the list of even values, sorted by their corresponding odd
value, is sufficient to fully reconstruct the original list of pairs.
As an example, we show how we would find the Dowker notation for the trefoil. Note that the handedness of the trefoil is irrelevant. After labeling the trefoil, the pairs are (1, 4), (2, 5) and (3, 6) (see Fig. 4). We reorder the values in some of the pairs, in this case in (2, 5), to place the odd value first. Then the pairs can be ordered by their odd value to get (1, 4), (3, 6), and (5, 2). The original pairs can be reconstructed with the sequence (4, 6, 2) as there is a unique way of reestablishing the odd counterparts to each of the even numbers. Thus, (4, 6, 2) is the Dowker notation for the trefoil. Since this sequence contains only even numbers, storing half of each value works just as well and makes some computations easier. Therefore, we represent the trefoil by (2, 3, 1). We call the notation that stores half of each integer an MD code (M is for modified). The matrix of pairs is called an ED code (E is for extended). The ED code for the trefoil is .
We will later refer to examining permutations.
Since a MD code is a permutation of the numbers from 1 to , we can examine
each such permutation to see if it encodes a viable knot diagram.
Note the distinction between a permutation, one of the many ways of ordering the
numbers from 1 to , and an MD code, a permutation of the number from 1 to
that encodes a particular knot diagram.
Crossings
Righthanded Lefthanded
As described so far, this notation only tells us which strands cross which. What it does not tell us is the handedness of each crossing (see Fig. 5). In other words, the shape of the knot diagram can be reconstructed, but every crossing will effectively be blurred out, as it will not be clear which of the two strands in the crossing is the upper strand and which is the lower strand. To account for this, we declare that a crossing is positive if out of the two values that make up a crossing, the odd one corresponds to the upper strand of the crossing. If a crossing is not positive, it is negative and we indicate this by negating the even value in each negative crossing. For example, if a crossing is marked (17, 34) and the strand labeled 17 passes above the strand labeled 34, we leave the crossing as is. On the other hand, if the upper strand is marked 34, we denote the crossing by the pair (17, 34).
If we were to flip over a knot diagram and look at it from the back, all of the values in the MD code would change sign. To account for this, when necessary we negate all of the values in the MD code to make the leading term positive. As a result, every knot diagram with crossings can be represented by a signed permutation of the numbers from 1 to .
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III Alternating Knots
A subset of the knots we are trying to tabulate are called alternating knots. By determining which alternating knots should be included in our tabulation, we can simplify the task of determining the remainder of the list. For this reason, we start by determining which alternating knots should be included in our reconstruction of the Rolfsen table.
When we move along a knot diagram, labeling its edges to determine its MD code, we go over some strands and under others. If we always alternate between going over and under the strands we cross, we say that the knot diagram is alternating. We note that any minimal knot diagram that is equivalent to an alternating knot diagram will be alternating (see [2]). Thus, it makes sense to refer to alternating knots as this property is independent of our choice of knot diagram, as long as it is minimal. Any knot that is not an alternating knot is a nonalternating knot. We note that the MD code of an alternating knot will consist entirely of positive entries.
To generate all of the knot diagrams that might be included in our tabulation, we do not need to generate every possible knot diagram that there is. It suffices to first determine the list of alternating knots in our reconstruction of the Rolfsen table. Afterwards, we will construct the nonalternating knots from our finalized list of alternating knots.
We know that not all permutations of 10 values result in valid knots. Thus, some of these permutations must be eliminated from consideration. There are several criteria which we can use to determine which alternating knots should be included in our list. We will first define these criteria, then explain how to implement a test that verifies that they are satisfied. The alternating knot corresponding to a given permutation is included in our tabulation if and only if it meets all of the following criteria.

A knot diagram can produce different permutations depending on where one starts numbering and in which direction they proceed. There are ways to choose both a starting point and a direction. A permutation is minimal if it is lexicographically smaller than or equal to all of the other possible permutations of the corresponding knot diagram. To satisfy this criterion, a permutation must be minimal.

The resulting knot diagram must be prime. Since a composite knot diagram can be split into two knot factors, we know that as we label the knot, we will have to go through all of the crossings of one of the knot factors before we move on to the other. This means that the values from 1 to will be split into two consecutive subsequences since the values in each subsequence will be the labels of the crossings of one of the knot factors. In a permutation, this would be expressed as a set of pairs, all of whose values form a consecutive subsequence. Thus, such a set must not exist in the ED code for the knot diagram to be prime (see Fig. 3). This also handily eliminates knot diagrams that contain a kink and could be simplified with the first Reidemeister move. The third Reidemeister move and the simplifying direction of the second Reidemeister move cannot occur in alternating knots (see Fig. 1).

The permutation must encode a diagram which is realizable. This means that there must be a way to draw the knot diagram in the plane without adding any intersections beyond the ones encoded in the permutation. The simplest permutation that fails this test is (2, 4, 1, 5, 3). It is physically impossible to draw a knot diagram on a plane that would have a nonrealizable permutation as its MD code.

The knot diagram must be minimal with respect to flyping. This means that the knot diagram’s minimal permutation must be lexicographically minimal over all of the permutations of knot diagrams that can be obtained from our original diagram by applying a sequence of flypes (see Fig. 1).
The first two conditions can be used to avoid testing all possible alternating MD codes. If we arranged the permutations lexicographically and went along checking each one, it will frequently be possible to skip checking up to permutations at a time, where .
Skipping these permutations is made possible as the first two criteria can be checked directly from the permutation. If a permutation that fails one of the first two criteria contains a string of values that make the permutation fail this criterion, then all permutations that contain the same string of values will also fail this criterion and do not need to be considered. Thus, as soon as we find such a permutation, we increment the last digit of the offending subsequence, thereby skipping permutations ahead, where is the number of digits left in the permutation after the subsequence. In other words, given a leading subsequence that fails a criterion, we do not try to continue it with terms that we know will fail the same test.
For the first criterion, a permutation is not minimal if we can find a pair of values in our ED code which are numerically closer together than the leading term and its oddvalued pair, the number 1. So if there is an even value in the ED code which is closer to its paired odd value than the first number in the ED code is to 1, then all permutations with in the same position will not be minimal. This is because starting the enumeration of the knot diagram’s crossings at the one previously labeled would result in a smaller first element in the MD code, which is not allowed as the knot diagrams in the table must be minimal.
Similarly, if a knot diagram is composite, this is represented by several consecutive terms in the permutation, so all permutations obtained by rearranging the values that come after this sequence would also fail this test. Checking if a knot is prime was described above, we need to find a subsequence of the values from 1 to such that the all of the values’ pairs are just a reordering of the same subsequence. For example, if an MD code starts with (2, 3, 1, …) it will not be prime. This is because the subsequence (1, 2, 3, 4, 5, 6) has pairs (4, 5, 6, 1, 2, 3). Since the second list is just a rearrangement of the first, any knot that starts with this sequence will contain a knot factor, a trefoil in this case, and will not be prime.
In other words, if a knot is composite, its knot factors will contain consecutive strand labels. Since two knot factors can never cross, the crossings of a knot factor contain two elements of the subsequence that our permutation starts with. Thus, if the pairs of the values in a subsequence do not contain any values outside of that subsequence, the knot diagram is not prime.
The third condition is checked with the help of a modified graph planarity algorithm. If a 4valent graph is constructed out of a knot diagram by replacing each crossing with a vertex and each edge of the knot with an edge in the graph, then typical planarity tests would frequently give false positives. There are 4 edges emanating from a crossing, but there are only 2 ways of arranging them in a valid manner in a knot diagram, but there are 6 ways of arranging 4 edges around a vertex. The reason for this is that a strand is not allowed to exit a crossing via an edge that is adjacent to its incoming edge. Strands must go directly across a crossing which means that the incoming and outgoing edges of a strand must be aligned opposite from each other.
We have not yet imposed any restrictions that would tell a graph planarity algorithm that such cases should not be considered. Permutations that fail this test do not form a planar knot diagram, but the graph that is created by making the same connections between vertices is planar. We can check that the graph formed by the permutation (2, 4, 1, 5, 3) is planar, yet such a knot diagram is impossible to draw, and is thus not realizable.
To solve this problem, it is sufficient to replace each vertex with four vertices in a square to construct the modified graph of the knot diagram (see Fig. 6). This preserves the planarity of the two allowable configurations but bars the other four, as the square would be transformed into a nonplanar bowtie shape. Thus, it suffices to use a regular graph planarity algorithm to check whether the modified graph of the knot diagram is planar. If it is not, the permutation fails the third criterion.
Finally, the fourth condition is checked by using a graph searching algorithm to find all knot diagrams that can be obtained from a given knot diagram with a sequence of flypes (see Fig. 1). From these, we keep only the lexicographically minimal knot diagram. A flype is represented in a permutation as a pair and two disjoint subsequences of 1 to . The two subsequences are the strands that are the part of the knot that gets flipped and the pair is the crossing that gets moved to the other side of the knot during the flype. Note that these subsequences must satisfy several conditions. The first is that all of the numbers in these subsequences must be pairs of other elements of the subsequences. This is much like testing a knot for primality. The reason for this condition is that the part of the knot that is flyped must be like a two strand knot factor, in the sense that it must not cross any part of the knot outside of itself. Additionally, these two subsequences, depending on which way the strands run, must either start or end with the values adjacent to those of the earlier pair. Since that pair contains one odd value and one even value, we can save time by ignoring the cases where this would be violated.
Without the flyping condition, we have generated a list of all candidate knot diagrams. This is a list of all diagrams that encode alternating knots and all appear distinct at first glance. We will use this list later when we will want to examine all valid knot diagrams as opposed to those that are necessarily distinct.
At this point, it is reasonable to doubt that the four conditions have completely narrowed down the list of alternating knots, leaving no equivalent knot diagrams. The reason for why this is sufficient is because any two minimal equivalent alternating knot diagrams are related by a sequence of flypes (see [3]). This means that our list of alternating knot diagrams contains no duplicates and is complete. There are 197 alternating knots with 10 crossings or fewer.
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IV NonAlternating Knots
After generating all of the alternating knots, we have a smaller set of knot diagrams to test to see if they should be included in our tabulation. There are signed permutations with a positive leading term. Of these, we only need to consider those that have the shape of alternating knots in our list. What this means is that we only have to consider the knot diagrams obtained for each alternating knot in our list by flipping the signs of the elements of the alternating knot’s MD code in every possible way. There would be ways to do this but the leading term must stay positive, leaving us with ways.
For the case where , we have 123 alternating knots. This means that we will generate 62976 nonalternating knots. Although this may seem like a large number of knots, most of these can be examined and discarded immediately.
Almost all of these knot diagrams are discarded as they can be reduced with the second Reidemeister move. Many of those that remain can be reduced with a (2, 1)–pass or a (3, 2)–pass (see Fig. 1). We do not consider the (1, 0)–pass as it is the first Reidemeister move. These pass moves can be found in most reducible knot diagrams.
By considering all knot diagrams that cannot be simplified with either the second Reidemeister move or a pass move, there are very few reducible knot diagrams that have not yet been eliminated. The reason for this is that a reducibility test checking only for these moves will occasionally give false negatives. This will be dealt with at a later stage. We will call knot diagrams that can be reduced with the second Reidemeister move or a pass move as immediately reducible. Note that not all reducible knots are immediately reducible. At this point, we have 1176 nonalternating knot diagrams that are not immediately reducible left to consider.
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V Finding Equivalent Diagrams
Canonically, alternating knots precede nonalternating knots in the Rolfsen table. We maintain the same pattern, ordering the knots within each of the two sets lexicographically. Additionally, knots with a lower crossing number always precede those with a higher crossing number.
We need to determine which knot diagrams are equivalent and find the lexicographically smallest permutation for each knot. We do this by examining all knot diagrams which cannot be transformed into lexicographically smaller ones by applying a sequence of crossing numberpreserving moves.
For 10 crossings and fewer, the third Reidemeister move, the 2–pass, and the flype (see Fig. 1) are sufficient to eliminate all but 54 of the nonalternating knot diagrams that are not immediately reducible. Applying the third Reidemeister move is preferable to applying either of the first two Reidemeister moves. This is due to the fact that there are many ways of adding crossings to a knot diagram but there are only a few ways to apply a move that preserves the knot diagram’s crossing number.
To find equivalent knot diagrams, we implement a graph searching algorithm. We first need to build our graph recursively by adding on subsequent layers of knot diagrams. We start with a graph consisting of the set of vertices and edges . We define as the set of those 1176 knot diagrams that are not immediately reducible. For every natural number , we define as the union of and the set of knot diagrams that can be obtained by applying one crossing numberpreserving move to a knot diagram in . We do not need to define our edges recursively. For any nonnegative integer , we define . For any two knot diagrams and in we include the undirected edge (, ) in if we can apply a crossing numberpreserving move to and obtain (see Fig. 1). Lastly, is simply the set of vertices and set of edges .
Since there are finitely many knot diagrams with a given number of crossings, there must exist an integer such that is equivalent to , at which point the graph will cease to change. We then take to be our graph. Each connected component of the graph consists of a set of equivalent diagrams, all representing the same knot.
At this point we return to the earlier concern that this graph might contain some reducible knot diagrams. Any reducible knot diagram that has not yet been removed is not immediately reducible, which means that it cannot be reduced with a pass move or the second Reidemeister move. However, all such diagrams are equivalent to other diagrams which are immediately reducible. Thus, we check to see if any of the knot diagrams in a connected component are immediately reducible. If at least one is, we need to remove the entire component from the graph. To do this, we create a graph which is a subgraph of and contains only the edges and vertices of the components which do not contain any immediately reducible knot diagrams. After this, does not contain any reducible knot diagrams.
We now must generate our list of knots from the graph . To do this, we take the lexicographically smallest knot diagram from each connected component of . As previously mentioned, we get 54 such knots. Combined with the 197 alternating knots, this gives us 251 total knots. However, just because we have applied a variety of moves to construct edges in our graph does not mean that we are done. It is possible that there are equivalent knot diagrams in the graph between which we were unable to find a sequence of moves out of our set. Thus, all we know is that there are no more than 251 knots with 10 crossings or fewer. Our lower bound is currently 200, as we know that our alternating knots are distinct and that we have at least one nonalternating knot with each of 8, 9, and 10 crossings.
The reason that we may have more knot diagrams than we should is because we are restricting ourselves to using flypes, 2–passes, and the third Reidemeister move to find equivalent knot diagrams. Reidemeister’s original theorem has the consequence that if two minimal knot diagrams are equivalent and it is impossible to transform one into the other by repeatedly applying the third Reidemeister move, the only option left available to us is to first add crossings using one of the first two Reidemeister moves, and proceed from there. We are in a similar position because to show that two of our knot diagrams are equivalent, we would have to turn them into more complicated equivalent knot diagrams. However, though there are relatively few ways to apply the third Reidemeister move to a knot diagram, there are many ways of adding a kink to one.
Our next step is to figure out which pairs of knot diagrams in our list might be equivalent. Since there are so many ways of adding kinks, checking all of our knot diagrams for equivalence this way would take a long time. Thus, we would like some way to establish with certainty that some of our knot diagrams cannot be equivalent to any others. We do this by using invariants.
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VI Invariants
All invariants are functions from the space of knot diagrams to an arbitrary target space. The property that an invariant must satisfy is that the images of two equivalent knot diagrams must be equal under an invariant. This allows us to show that two knot diagrams on which an invariant produces a different value are knot diagrams of two different knots.
The invariant condition is easy to satisfy as we could choose the image of the invariant to have unit magnitude. For example, we could state that for any knot diagram, our carefully crafted invariant produces a value of 0. However, such an invariant is useless as we want to be able to show that some knot diagrams are distinct. Thus, we need invariants that produce the same value for nonequivalent knot diagrams as rarely as possible. The degree to which an invariant accomplishes this it is typically called its strength, where weak invariants often produce the same values for different knot diagrams and vice versa. Often, stronger invariants require more time to compute, which is why it is useful to have several invariants. We use them in increasing order of strength so that the most difficult computations only have to be done for a few knot diagrams, those between which the weaker invariants were unable to distinguish.
The weakest invariant that we have available to us is crossing number. We know that all of our knots are nonreducible and we also know that all of our alternating knots are distinct. This immediately reduces our task to simply calculating invariants on nonalternating knots that all have the same crossing number.
After this initial step, we use two different invariants to complete the task. Our initial simplifications would typically be considered too crude to be deemed invariants except in the most technical of circumstances. Our first invariant, the Jones polynomial, is fast and fairly strong and the second, the number of colourings, is slow but even stronger.
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VII Planar Diagram Notation
To find the Jones polynomial of a given knot diagram, the knot diagram must be written in planar diagram notation as opposed to as an MD code. To find this notation, it is necessary to determine the handedness of each of the knot diagram’s crossings (see Fig. 5). All we know about a knot diagram’s crossings from an MD code is which strand passes above or below. We do not know the handedness of each crossing. As there are 2 types of crossings, there are possible ways to set the handedness of a knot diagram’s crossings. Since the only knot diagrams being considered are realizable, it is known that at least one of these crossing orientations will make the knot diagram planar.
Since we are trying to compute polynomials of knot diagrams where , we have that , which is, computationally speaking, a small number. For this reason, we can exhaustively iterate through the crossing orientations until we find one that creates a planar knot diagram.
To test if the knot diagram with given crossing orientations is planar, we apply the knot diagram planarity replacement from before, but replace each outer edge with a ribbon, a pair of parallel edges, to only allow 1 of the 6 edge configurations (see Fig. 7).
Earlier, the square replacement remained planar for either of the two ways of arranging the edges of the crossing so that the strands enter and exit the crossing through opposite edges (see Fig. 6). Now, we wish to exclude one of these two configurations. We do this by arranging the strands into the configuration we desire and changing the incoming edges into pairs of edges. Now, whenever the strands do not exit and enter through opposite edges, the graph will not be planar, just as before and for the same reasons. More importantly, when the handedness of the crossing changes, a twist will be added to two of the ribbons, making the graph nonplanar. Thus, all we need to do is search through all possible sets of crossing orientations until we find one for which this modified graph is planar.
Every crossing is represented in planar diagram notation as (see Fig. 8). Here, is the index given to the lower incoming edge and then , , and proceed counterclockwise. The knot diagram is then written as the product of its crossings in planar diagram notation. For example, the lefthanded trefoil (see Fig. 4) is written as .
Once we can transform knot diagrams into planar diagram notation, we can compute their Jones polynomials.
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VIII Jones Polynomial
The Jones polynomial of a knot diagram is computed from the product of the knot
diagram’s crossings.
Smoothings for a RightHanded Crossing
0smoothing 1smoothing
Every crossing can be smoothed in two distinct ways (see Fig. 9). By smoothing a crossing in a particular manner, the polynomial of that smoothing is multiplied by a coefficient of either or for the 0 and 1smoothings, respectively. Since each smoothing is actually a coefficient multiplied by the two nonintersecting strands of the smoothing, a strand stitching operation is applied to turn a product of smoothings into an unlink of several components.
A strand stitching operation satisfies the property that the product of two strands that share an endpoint, such as the strand from to , (, ), and the strand (, ), will be equal to one strand running between their noncommon endpoints, (, ) in this case.
The final result will always be the product of several strands that are closed loops of the form (, ). Each of these components of the link is given a coefficient of and thus the result is a polynomial in , , and . What we have defined so far is called the Kauffman bracket of a knot diagram , and it is denoted . We note that and ø, where and ø represent the unknot and the empty knot, respectively. Using this notation, a formula for the smoothings of a crossing can be written.
A given smoothing is a 0smoothing if the incoming end of the lower strand is connected to the next end going counterclockwise around the crossing, in other words, the nearest end on its right. If it is connected to the end on its left, the resulting smoothing is a 1smoothing.
Thus, , the Kaufmann bracket of the righthanded trefoil can be evaluated. Note that this trefoil is righthanded so we will only need (1). There are two ways to smooth each crossing so there are eight ways to smoooth the three crossings altogether. Two of these ways are applying three 0smoothings and three 1smoothings. The other six cases are not all distinct, since there are three identical ways of applying either one or two 0smoothings. Thus, each of the cases in these sets have the same bracket value, which is how the bracket of the trefoil is expanded.
Unsurprisingly, (3) looks a lot like an application of the binomial theorem. However, that is only because the trefoil is rotationally symmetric. In the general case, the bracket will not have as many like terms.
By counting the number of components in each unlink, the remaining brackets are evaluated with the corresponding power of .
To make the Kaufmann bracket invariant over the second Reidemeister move, we need to set and . We find that these relations make the Kaufmann bracket invariant over the third move as well. This means that to show that this is actually an invariant, it suffices to show that the Kaufamnn bracket is invariant over the first Reidemeister move. We find that in its current form, this is not the case.
To make the Kaufmann bracket invariant over addition and removal of kinks, the whole polynomial must be multiplied by a coefficient of where is the writhe of the knot diagram, which is the difference between the number of righthanded and lefthanded crossings in the knot diagram.
The resulting polynomial will have a factor of in every component as every unlink that we can get by smoothing the knot diagram has at least one component. Thus, the polynomial is normalized by dividing it by . Lastly, what we have obtained will always be a polynomial in so the rule is applied to make the result a Laurent polynomial in (see [2]).
For the trefoil, these substitutions allow us to transform our equation into a simpler form. We get that the writhe, , is equal to 3. This means that the Jones polynomial for the righthanded trefoil needs to be multiplied by . Applying and , we get the Jones polynomial of the trefoil.
Since the Jones polynomial of the mirror image of a knot diagram is the Jones polynomial of the original knot diagram with replaced by , the minimal of these two polynomials is taken as the value of the invariant for that knot diagram.
Applying the substitution will yield the final version of the Jones polynomial for the righthanded trefoil. However, the lefthanded trefoil has a smaller Jones polynomial by degree so we state that the Jones polynomial for the trefoil is the Jones polynomial for the lefthanded trefoil.
We find that the Jones polynomial shows that every knot diagram out of our 251 with 9 crossings or fewer is distinct. This is because all of the nonalternating knots with fewer than 10 crossings have distinct values for their Jones polynomial. Among the knots with 10 crossings, we find two pairs of knot diagrams with the same Jones polynomial. As we have dramatically reduced the list of diagrams we are unsure about, we can now apply our more powerful invariant at little cost.
Note that this raises our lower bound to 249. This is because there can be at most two extra knots in our list as the Jones polynomial only found two pairs of knots whose Jones polynomial was not distinct.
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IX Knot Colourings
We have two pairs of knots in our list that could be equivalent. We need to determine if the knot diagrams in either pair are distinct. As we have very few knot diagrams to analyze, we can spend some additional time computing a more complicated invariant, in exchange for it being able to distinguish between our knot diagrams. This invariant is the number of colourings of the knot diagram with elements of the permutation group , for some . Such a colouring is an assignment of permutations of elements to edges of the knot diagram such that these permutations satisfy a particular set of conditions. The number of such colourings is invariant over the three Reidemeister moves, making it invariant over all equivalent knot diagrams.
If two knot diagrams are equivalent, the number of colourings using elements of will be the same for all natural numbers . To show that two knot diagrams are not equivalent, it is sufficient to find a value of such that the the invariant produces a different value for the two knot diagrams. Thus, the number of ways to colour both knot diagrams using elements of must be different.
It would be incorrect to simply count the number of ways that various values of can be assigned to all edges of the knot diagram. To be an actual invariant, the assignments must satisfy two conditions. The reason for that is that the values assigned to edges along an arc must be the same. Thus, if we have a crossing , we label the values in that we assign to each edge as , , , and starting from the incoming lower edge and proceeding counterclockwise. From this, the two relations that these four values have to satisfy are constructed.
We know that the permutations must be equal along any arc. Thus, the two edges of the top strand have the same permutations.
The second criterion that our permutations must satisfy is as follows. The signed product of the permutations assigned to the four edges around a crossing must be the identity permutation. To clarify, we start by picking an arbitrary sign convention, which in our case is that inward pointing edges are given a positive sign. Then, we move around a crossing in an arbitrary direction from an arbitrary starting point, which in our case are counterclockwise from the edge labeled . Inverting the permutations for the negative, and thus outward pointing, edges, we construct an equation that positive crossings must satisfy. Note that in a positive crossing, edges and point outwards.
For a negative crossing, we switch the signs of and .
By putting together (7) and (8), we get an equation for each positive crossing.
So we can find by finding the permutation conjugation of and . We also get an equation for negative crossings.
Thus, for negative crossings, is the permutation conjugation of and .
We note that since we are taking the permutation conjugation of with , then and will have the same cycle lengths. As any two edges across a crossing have the same cycle lengths, and since we can follow the path of the knot by going through each crossing, one by one, never changing cycle lengths, then all of the values for the edges must have the same cycle lengths. This gives us a lot more information.
Whereas before we would have had to map edges to and count the total number of colourings, now they can be mapped to a subset of . If all the elements of this subset have the same cycle lengths, then the number of colourings for each such subset can be counted independently. Thus, instead of ending up with a single number as our invariant, we end up with different values, where is the partition function. This is due to the fact that elements of have different possible cycle lengths. Thus, to show that the knot diagrams are different, it suffices for any one of these values to differ.
As previously stated, we cannot simply find the number of ways to map edges to elements of . For simplicity, we will assume that from now on we are dealing with a positive crossing. To do this for a negative crossing, it suffices to invert before computing its permutation conjugation with .
We need to find as many equations that relate the edges as possible using (7), (8), and (9). For knot diagrams with crossings we have to find equations relating the edges. Finding such equations is easy with (7) as every crossing has an upper arc whose two edges must have equal values in . Similarly, every crossing also gives us an equation from (10) or (11), so we have a total of equations.
We know that we cannot choose the permutations for all edges independently as there are equations relating them that will may not be satisfied if we were to do so. We also know choosing a permutation for just one edge will not be sufficient to generate the remaining edges. Thus, there is some number of edges whose values can be used to generate the rest of the edges using (7), (10), and (11). We call such edges generators and we need to find such a set of edges. Note that this set will not be unique, but we want to minimize its size while still guaranteeing that we can generate all of the permutations.
For some perspective, when , there are between 3 and 5 generators which can determine the rest of the 20 permutations. It is immediately clear that edges can be derived from the other by using (7). Thus, we are only interested in finding which of the other can generate all of the permutations. What we are effectively doing is writing out the indices from 1 to and striking out all those indices which can be determined from those that remain. For each crossing, we examine the edges that make up the upper strand and remove the one with the larger index from our list. After we have done this, we have remaining indices. We will call the set of these indices .
We create a graph with vertices , where is the power set function. Note that , which for is not too large. For each crossing, (10) tells us that knowing as well as either or , is sufficient to determine the other one, either or , respectively. We represent this in the graph with a directed edge. From every vertex with set where contains both and , we draw a directed edge to the vertex with set . Similarly, we draw an edge from each vertex whose set contains both and to the vertex with set . An edge from vertex to vertex represents the fact that by knowing the permutations for all of the edges with indices in the set , we can determine the permutations for all of the edges with indices in the set by applying (10) or (11) once.
We consider the vertices from which there is a path to , the vertex containing all of the indices. If there is a path from a vertex to the vertex , then we know that being given the permutations for the edges whose indices are in is sufficient to determine all of the permutations of the knot diagram. Thus, to find our set of generators, we choose the vertex from which there is a path from to such that is as small as possible. To find the sequence of edges whose permutations can be determined, we examine any path from to and choose that as our order.
Once we have found the generators, we need to start testing colourings. We first break up into disjoint subsets by cycle lengths. For each of these subsets , we try assigning permutations in to each of the generators in in every possible way. There are ways of doing so. This exponential is the reason for why we put so much effort into minimizing our set of generators.
Once we set the generator permutations, we generate the permutations for the rest of the edges, and then check that (10) or (11) is satisfied for each crossing. If it is, then the colouring is valid, otherwise, it is not.
We count the total number of valid colourings and our invariant becomes a list of size containing the number of valid colourings of the knot diagram using elements of . Each element of the list corresponds to a different subset of , where all of the elements in each subset have the same cycle lengths.
After we had applied the Jones polynomial, we found two pairs of knot diagrams that could be equivalent. After setting to 5 and calculating the number of colourings for each of the four knot diagrams in those two pairs, we found that the two knot diagrams in our of the pairs produced different values, showing that they represent distinct knots. The two knots in the other pair produced the same list for the number of ways in which they could be coloured using elements of . Thus, we have at least 250 distinct knot diagrams and potentially as many as 251.
We now try to see if the knot diagrams which have produced the same result for each of our invariants are equivalent. To show that the two knot diagrams in the pair are equivalent, we try adding a positive kink into the knot diagrams in each of the 10 possible ways. To add a kink, we insert a into the position in the MD code and add 1 to all of the other values in the MD code that are greater than or equal to .
Our two new 11crossing knot diagrams are found to be equivalent under repeated application of the third Reidemeister move (see Fig. 1).
Thus, the two knot diagrams that were producing the same values for each of our invariants are equivalent. This proves conclusively that we there are no fewer and no more than 250 knots with up to 10 crossings.
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X Knot Graphs
In our calculation of the Rolfsen table, we mainly used three moves, the 2–pass, the third Reidemeister move, and the flype (see Fig. 1). We generated a graph of connections to find equivalent knot diagrams. Now, we run our algorithms with a different set of knot diagrams. We replace distinct prime alternating knot diagrams with all prime alternating knot diagrams. The difference between the sets is that the latter has diagrams that are equivalent with respect to flyping.
From these knot diagrams, all of their nonalternating knot diagrams are generated, each knot diagram is mapped to a vertex, these vertices are connected with edges representing 2–passes, third Reidemeister moves, and flypes (see Fig. 1), and lastly all connected components that were found to be reducible are removed.
The result is the full graph of irreducible knot diagrams and their connections. This graph can be used for testing knot invariants. Each invariant must produce the same result for each vertex in every connected component. Below is this graph, but with no labels. The 2–passes, third Reidemeister moves, and flypes are represented by red, green, and blue edges, respectively.
This graph is also available online at http://tiny.cc/RolfsenTableGraph.
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XI Utility Functions
Here we include all the functions that are not mathematically interesting, but merely serve as helper functions for those that are. They are included here for completeness and in alphabetical order for ease of access.
All of this code is also available online at http://tiny.cc/RolfsenTableCode.
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XII The Result
This list can be found online at http://tiny.cc/RolfsenTable.
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XIII Acknowledgements
The author is grateful to Prof. Dror BarNatan for his neverending support and assistance with this project. Additionally, Prof. BarNatan originally suggested the topic of this project.
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XIV References
References
References
 Hoste, Jim, Morwen Thistlethwaite, and Jeff Weeks. “The First 1,701,936 Knots.” The Mathematical Intelligencer 20.4 (1998): 3348. Web.
 Kauffman, Louis H. “New Invariants in the Theory of Knots.” The American Mathematical Monthly 95.3 (1988): 195. Web.
 Menasco, William W., and Morwen B. Thistlethwaite. “The Tait Flyping Conjecture.” Bulletin of the American Mathematical Society 25.2 (1991): 40313. Web.