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The Spiral Index of Knots

Colin Adams William George Rachel Hudson Ralph Morrison Laura Starkston Samuel Taylor  and  Olga Turanova Colin Adams, Department of Mathematics, Bronfman Science Center, Williams College, Williamstown, MA 01267 Colin.C.Adams@williams.edu William George, Department of Mathematics, University of Toronto, Toronto, Ontario, Canada M5S 2E4 wgeorge@math.toronto.edu Rachel Hudson, Department of Mathematics, Bronfman Science Center,Williams College, Williamstown, MA 01267 10rah@williams.edu Ralph Morrison, Department of Mathematics, Bronfman Science Center,Williams College , Williamstown, MA 01267 10rem@williams.edu Laura Starkston, Department of Mathematics, Harvard University, 1 Oxford St., Cambridge, MA 02138 lstarkst@fas.harvard.edu Samuel Taylor, Mathematics Department, College of New Jersey, Ewing, NJ 08628-0718 taylor29@tcnj.edu Olga Turanova, Department of Mathematics, Barnard College, Columbia University, New York, NY 10027-6598 ot2130@barnard.edu
(Date: August 1, 2025)
Abstract.

In this paper, we introduce two new invariants that are closely related to Milnor’s curvature-torsion invariant. The first, the spiral index of a knot, captures the number of maxima in a knot projection that is free of inflection points. This invariant is closely related to both the bridge and braid index of the knot. The second invariant, the projective superbridge index, provides a method of counting the greatest number of maxima that occur in a given knot projection. In addition to investigating the relationships among these invariants, we classify all knots that satisfy (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi.

1. Introduction

A projection of a knot KK is said to be in braid form if as we traverse the knot in its projection plane we wind monotonically about a fixed axis. The braid index of the knot, denoted β[K]\beta[K], is then defined to be the minimum number of times the knot winds about the fixed axis in any of its braid forms. This invariant has shown to be a powerful tool for knot theorists because of its close relationship to other classical invariants like bridge index and newer invariants like the HOMFLYPT polynomial. In this paper we investigate knot projections that are similar to braid form but without the constraint of a fixed axis. Here we require the knot projection to wind in a single direction; that is, we do not allow the planar curvature of the knot projection to change sign. We say that this type of knot projection is in spiral form and call the minimum number of “spirals” necessary for such a projection the spiral index of the knot.

Spiral index, like braid index, is closely related to other properties of the knot. For instance, both impose significant structure on the Seifert circles generated from a diagram of the knot. We also relate the spiral index of a knot to its bridge index, denoted b[K]b[K], by showing that a projection of a knot in spiral form has the same number of maxima in all directions in its plane of projection. To study this more precisely, we introduce the projective superbridge index of a knot, which is related to the superbridge index defined in [5], and which captures the greatest number of maxima of a knot in a projection, minimized over all projections. By relating the spiral index and projective superbridge number to the curvature-torsion invariant defined by Milnor in 1953, we are able to identity all knots for which curvature-torsion is equal to 6π6\pi, a question that was posed by Honma and Saeki [4].

2. Spiral Index

We begin by introducing the notion of spiral form for a knot. Let KK be a knot in 3\mathbb{R}^{3} and, given vS2v\in S^{2}, let Pv(K)P_{v}(K) be the projection of KK onto the plane PP through the origin and orthogonal to vv. When the vector vv is clear from context, we denote the projection P(K)P(K). In a projection, an inflection point is a point at which planar curvature is zero. We further classify inflection points as either ss-inflection points, where planar curvature switches signs, or uu-inflection points, where sign is unchanged.

Definition 1.

A smooth projection of a knot KK is in spiral form if the projection has no ss-inflection points.

Note that this definition is equivalent to the curvature of the projection being non-negative at all points or non-positive at all points. Further, a projection is in spiral form if and only if it has the same number of local maxima with respect to every direction in the plane (see section 4 for a proof of the equivalence).

Definition 2.

The number of maxima in a projection P(K)P(K) that is in spiral form is the spiral number of that projection, sp(P(K))sp(P(K)). The spiral index of a knot KK, denoted by sp[K]sp[K], is the minimum of sp(P(K))sp(P(K)) over all spiral projections of KK.

Spiral form is closely related to the braid index of a knot, denoted β[K]\beta[K]. In fact, because every knot has a projection in braid form [1], every knot also has a projection in spiral form – given a braid projection, we may isotope it to be sufficiently close to a circle centered at the braid axis and thus to have no inflection points. It follows immediately that sp[K]β[K]sp[K]\leq\beta[K]. Further, since the minimum number of maxima over all projections of a knot is no greater than the minimum over all spiral projections, we have b[K]sp[K]b[K]\leq sp[K].

Even though the braid index of a knot may be defined as the minimal number of maxima of a knot projection that winds monotonically around a fixed axis, often the braid index and spiral index of a knot differ. This is because in spiral form, we do not require a fixed axis. For instance, the projection of 616_{1} in Figure 1 has spiral number 3, while the braid index of 616_{1} is 44. Thus, we have sp[61]<β[61]sp[6_{1}]<\beta[6_{1}].

Definition 3.

A knot KK is a curly knot if sp[K]<β[K]sp[K]<\beta[K]. More specifically, we say KK is an nn-curly knot if it is a curly knot with sp[K]=nsp[K]=n.

Refer to caption
Figure 1. The Spiral form of 616_{1} and its Seifert Diagram

Curly knots are relatively common among low crossing knots. Of the 81 nontrivial prime knots up to 9 crossings, there are 26 that we know to be curly knots and only 3 which may or may not be curly. We utilize Theorem 2.6 and its following paragraph to compute that the 33-curly knots up to 99 crossings are 616_{1}, 727_{2}, 767_{6}, 848_{4}, 868_{6}, 888_{8}, 8158_{15}, 949_{4}, 979_{7}, 9119_{11}, 9209_{20}, 9249_{24}, and 9289_{28}. The known 44-curly knots up to 99 crossings are 818_{1}, 838_{3}, 8128_{12}, 929_{2}, 989_{8}, 9129_{12}, 9149_{14}, 9159_{15}, 9199_{19}, 9219_{21}, 9259_{25}, 9399_{39}, and 9419_{41}. It is possible that 959_{5}, 9359_{35}, and 9379_{37} are 44-curly knots but we suspect that their spiral numbers are 55, which would imply they are not curly. In order to further characterize curly knots, we must consider the Seifert circles generated by spiral projections.

Spiral form imposes significant structure on the corresponding diagram of Seifert circles. The minimal spiral form of 616_{1} has five Seifert circles as in Figure 1; four of these circles “bulge out” on all sides, and one circle “bulges in” on all sides. We formalize these notions as follows.

Given a Seifert circle CC, connect its adjacent vertices by line segments (See Figure 2). Call the resulting graph PP. If CC is contained in PP, we call CC an i-circle (the sides of CC “bulge in”). If CC contains PP, we call CC an o-circle (the sides of CC “bulge out”). This characterization is equivalent to saying that for an o-circle all sides curve towards the center, while for i-circles all sides curve away from it.

Refer to caption
Figure 2. i-circles versus o-circles
Lemma 2.1.

For a knot projection in spiral form, any Seifert circle of a Seifert diagram is either an i-circle or an o-circle.

Proof.

Since each edge of the Seifert circle between two vertices has curvature of unchanging sign, we can define each side as curving inward or curving outward. Therefore if there were a Seifert circle which is neither an i-circle nor an o-circle, there would be a vertex at which one edge curving inward met another edge curving outward. Taking into account the orientation of the circle, this implies that the curvatures of these two edges have opposite signs. Since the orientation of the Seifert circle is the same as the orientation of the knot, this contradicts the assumption that the projection is in spiral form. ∎

Lemma 2.2.

The total planar curvature, κ\kappa, of a knot in spiral form with spiral number sp(P(K))sp(P(K)) is 2πsp(P(K))2\pi sp(P(K)).

Proof.

Let μ(K,v)\mu(K,v) denote the number of maxima of the function K(t)vK(t)\cdot v where vS1v\in S^{1}. Milnor proves in [8] that the total absolute curvature of a knot projection equals 2π2\pi times the average of μ(K,v)\mu(K,v) over the unit circle. Since in the spiral projection μ(K,v)=sp(P(K))\mu(K,v)=sp(P(K)) for all vS1v\in S^{1}, it follows that κ=2πsp(P(K))\kappa=2\pi sp(P(K)). ∎

In analogy to the characterization of the braid index as the minimum number of Seifert circles in any projection of the knot(c.f. [10]), we have the following theorem.

Theorem 2.3.

The spiral number of a diagram in spiral form is equal to the number of o-circles minus the number of i-circles.

Proof.

Consider the Seifert circles of an arbitrary projection of our knot KK in spiral form. Let ii be the number of i-circles and oo be the number of o-circles. Each Seifert circle, whether it is an i- or an o-circle, may have vertices of one or both of the two possible forms shown in Figure 3. We will distinguish convex cusps from nonconvex cusps and refer to these as CC cusps and NN cusps respectively. Each crossing of the knot is a vertex of two distinct Seifert circles. One of these vertices must be an CC cusp and the other a NN cusp, as illustrated in Figure 3. Further, there is an angle between the tangents of the two strands of the knot at the ithi^{th} crossing. We call this the exterior angle of the crossing, and denote it by θi\theta^{i}. When we refer to the exterior angle as being associated with an CC cusp, we will denote it θCi\theta_{C}^{i} and similarly, θNi\theta_{N}^{i} for NN cusps.

Refer to caption
Figure 3. Exterior Angles and Cusps

When our Seifert circle is an o-circle, its total curvature is 2π2\pi plus or minus the sum of the exterior angles at each of its cusps. The exterior angles compensate for the angle of rotation between the tangent vectors at the cusp. Thus the total curvature of the o-circle is

(1) κ(O)\displaystyle\kappa(O) =\displaystyle= 2πC cuspsθCi+N cuspsθNj\displaystyle 2\pi-\sum_{\text{C cusps}}\theta_{C}^{i}+\sum_{\text{N cusps}}\theta_{N}^{j}

Now we consider an i-circle which has only three cusps. (Figure 4). The exterior angles are labeled θ1\theta_{1}, θ2\theta_{2}, and θ3\theta_{3}. The total curvature of any curve in 2\mathbb{R}^{2} is the integral of dθd\theta, which (when we have no inflection points) equals the change in the angle between the normals to the smooth curve at each of its ends. Therefore, the curvature of each edge of the i-circle can be measured by calculating the angle between the two line segments which are orthogonal to that edge at the crossings that determine its end points. These angles are labeled ϕ1\phi_{1}, ϕ2\phi_{2}, and ϕ3\phi_{3} in Figure 4.

Refer to caption
Figure 4. Calculation of I-Circle Curvature

Consider the hexagon in Figure 4, whose interior angles sum to 4π4\pi. Summing these angles we obtain the following equation:

4π=6π+iϕijθNj4\pi=6\pi+\sum_{i}\phi_{i}-\sum_{j}\theta_{N}^{j}

Since we know ϕi\sum\phi_{i} equals the curvature of the i-circle, this equals 2π+iθBj-2\pi+\sum_{i}\theta_{B}^{j}.

Note that this formula can generalize to an i-circle with any number of sides as long as all the cusps are NN cusps. If we have such an i-circle with nn sides, we can put in orthogonal line segments as we did in the 33 side case and create a 2n2n-gon. Thus the sum of the angles is (2n2)π(2n-2)\pi. Here, there are nn obtuse angles which sum to 2nπjθNj2n\pi-\sum_{j}\theta_{N}^{j} and nn acute angles which sum to iϕi\sum_{i}\phi_{i}. Therefore,

(2n2)π=2nπjθNj+iϕi(2n-2)\pi=2n\pi-\sum_{j}\theta_{N}^{j}+\sum_{i}\phi_{i}

So the total curvature of any i-circle with only NN cusps is

iϕi=2π+jθNj\sum_{i}\phi_{i}=-2\pi+\sum_{j}\theta_{N}^{j}

Our final case is when i-circles have CC cusps, which occurs in the case of nested i-circles. This is pictured in Figure 5.

Refer to caption
Figure 5. Nested i-circles

In this case, we will replace each CC cusp in the i-circle with a smooth curve that has the same tangent vectors at the end points, as in Figure 6.

Refer to caption
Figure 6. Replacing a C cusp on an i-circle with a smooth curve

The curvature of each replacement curve is the curvature of the CC cusp that it replaced plus the exterior angle θCi\theta_{C}^{i}. We repeat this process for each CC cusp. The smoothed out i-circle has only NN cusps, thus we can calculate its curvature from the above argument. We then subtract all of the θC\theta_{C}’s that we smoothed out to get the total curvature of the original i-circle

(2) κ(I)\displaystyle\kappa(I) =\displaystyle= 2π+N cuspsθNC cuspsθC\displaystyle-2\pi+\sum_{\text{N cusps}}\theta_{N}-\sum_{\text{C cusps}}\theta_{C}

The total curvature of the knot projection equals the sum of the curvatures of all the Seifert circles. Also, in both the formula for the curvature of an o-circle (Equation 1) and in the formula for the curvature of an i-circle (Equation 2) all θC\theta_{C}’s are subtracted and all θN\theta_{N}’s are added. Therefore the total curvature of the knot κ(P(K))\kappa(P(K)) is

κ(P(K))=2πo2πiiθCi+iθNi\kappa(P(K))=2\pi o-2\pi i-\sum_{i}\theta_{C}^{i}+\sum_{i}\theta_{N}^{i}

Since each exterior angle is counted once as an CC cusp angle and once as a NN cusp angle,

iθCi=iθNi\sum_{i}\theta_{C}^{i}=\sum_{i}\theta_{N}^{i}

Therefore

κ(P(K))=2π(oi)\kappa(P(K))=2\pi(o-i)

By the previous lemma, 2πsp(P(K))=κ(K)2\pi sp(P(K))=\kappa(K). So we obtain

sp(P(K))=oisp(P(K))=o-i

Corollary 2.4.

If a knot or link KK is curly, then any spiral projection of KK realizing sp[K]sp[K] must have at least one i-circle in its Seifert diagram.

Proof.

By [10], the minimum number of Seifert circles in any projection of KK equals β[K]\beta[K]. If we have a projection of KK realizing sp[K]sp[K] whose Seifert diagram has only o-circles, then by the previous theorem we have that sp[K]sp[K] is equal to the number of o-circles. As there must be at least β[K]\beta[K] o-circles, we have sp[K]β[K]sp[K]\geq\beta[K] and thus sp[K]=β[K]sp[K]=\beta[K]. ∎

We now use the above results to show that there are no 11- or 22- curly knots or links and to characterize all 3-curly knots and links. First, if sp[K]=1sp[K]=1, then b[K]1b[K]\leq 1 and KK is the trivial knot, which has β[K]=1=sp[K]\beta[K]=1=sp[K] and thus is not curly. In order for a knot or link with sp[K]=2sp[K]=2 to be curly, its minimal spiral projection must have a Seifert diagram with at least one i-circle. Note that this i-circle must have more than 2 sides, as any bigon is an o-circle. Further, since an i-circle with four or more sides would force more than 2 maxima, the i-circle must be a triangle. If the triangle has a strand with two adjacent under/over-crossings, one can slide that strand over the third crossing of the triangle, converting the i-circle to an o-circle without changing the number of spirals, showing that the knot is not curly. Therefore, this triangle must be alternating. To complete this triangle to a nontrivial knot or link, we must add at least two additional local maxima. Thus the spiral index is greater than 2, contradicting the existence of 2-curly knots or links.

Theorem 2.5.

Every 3-curly knot or link has a minimal spiral projection of the form shown in Figure 7.

Refer to caption
Figure 7. Canonical 3-curly: Note to create a knot, two of the boxes contain twists with an even number of crossings and the third contains twists with an odd number of crossings.
Proof.

As with the 2-curly case, we require an alternating triangle in the link. (Given an i-circle with four or more sides, it is impossible to connect the sides to produce a projection with a spiral number of less than 4, so the i-circle must be a triangle). Thus, all links with sp[K]=3<β[K]sp[K]=3<\beta[K] must contain an alternating triangle as shown in Figure 7. No other strands of the link may cross this part of the diagram.

We now consider all possible configurations that include such an alternating i-circle. In order to preserve constantly signed curvature, point aa can only connect to points bb, dd, or ff. Suppose first that aa connects to bb, cc to dd and ee to ff. If aa links directly to bb without winding around the triangle at the center, and the other pairs of points do likewise, we have a trivial knot. Thus, we can assume aa loops once around the triangle and then connect to bb as shown. If cc or ee does likewise, or if the strand from aa to bb loops around twice, the projection will end up with a spiral number number greater than 3, and so cc must link straight to dd and ee to ff. This gives us a 3-curly projection of a knot that is included in the possibilities given by Figure 7.

If aa connects to bb, the only other possibility is that cc connects to ff and ee to dd. This generates a 2-component link. Since the strand connecting ee to dd wraps around the triangle, neither of the other two connecting strands can do so, and we obtain a projection that is included in the possibilities in Figure 7. Up to symmetry of the central triangle, this case covers all the possibilities for a 2-component link.

The only other possibility is if aa connects to dd, bb to ee and cc to ff. In this case, none of the connecting strands can wrap around the triangle or the spiral number will be greater than 3. This results in a 3-component link and it also is included in the possibilities provided by Figure 7.

Refer to caption
Figure 8. i-circle

Note all crossings outside of the middle triangle can be arbitrarily chosen. Furthermore, there are three sections of the knot where strands with the same orientation lie alongside one another, and so arbitrarily many positive or negative twists can be added between them. In the same way we can convert a braid form projection to a spiral projection, we can isotope the knot to prevent these twists from adding inflection points. Thus, the most general form of a 3-curly knot or link is as in Figure 7, where the boxes represent any number of positive or negative two-twists. ∎

Theorem 2.6.

All 3-curly links are alternating and prime.

Refer to caption
Figure 9. Putting 3-curly knots in alternating form.
Refer to caption
Figure 10. Changing to a 3-braid form.
Proof.

We may assume that the link appears as in Figure 7 and that the crossings within a given box alternate. If the crossings in a given box are alternating with respect to the adjacent crossings of the i-circle, then we need not alter that portion of the projection. Suppose now that the crossings in the top box are not alternating with respect to the i-circle crossings. If there is only one crossing in the top box, then the knot is the composition of two 22-braid links, and must have β=3\beta=3. Hence it is not curly.

Assume now there are at least two crossings in the top box. By performing the move shown in Figure 9, we cause that region of the link to become alternating relative to the triangle.

We now consider each of the lower boxes, and assume that they are not already alternating with respect to the center of the knot. If there are no alternating crossings in the box then the knot can be put in 33-braid form, as shown in Figure 10 and thus is not curly. Assuming there are crossings, we can perform a similar move to that shown in Figure 9, causing that region to be alternating relative to the triangle. We can thus obtain an alternating projection. Note that by [7], the link must be in minimal crossing form. Further, as we are in minimal crossing alternating form and the projection of the link is not obviously composite, the link is prime [6]. ∎

In addition to being the minimal spiral form of any 33-curly knot, Figure 7 allows us to generate all 33-curly knots up to a given crossing number. Up to adding arbitrarily many twists, there are 8 possible configurations of this knot (given that there are three locations where crossing can be changed between over and under). It can be shown that each of these configurations can be converted into an alternating knot whose number of crossings increases as crossings are added to any of the boxes. Thus, it is possible to go through every possible combination of varying numbers of positive or negative twists to generate all 33-curly knots up to a given crossing number. We have determined all 33-curly knots up to nine crossings, as listed in the introduction. These knots, along with the 33-braid knots, constitute all knots of spiral index 33.

Proposition 2.7.

All 33-curly knots and links have braid index 44.

Proof.

Consider a link of the form shown in Figure 7. By performing the move shown in Figure 11 on the alternating triangle, we can put the link in a 44-braid form, meaning that the braid of any link of this form has a braid index of at most 44. As 33-curly links must be of this form and by definition have braid index at least 44, we conclude that all 3-curly links have braid index 44. ∎

Refer to caption
Figure 11. Changing a 33-curly knot from 33-spiral form to 44-braid form.

Although a 3-spiral knot can have at most a difference of 11 between β[K]\beta[K] and sp[K]sp[K], this does not hold in general. For instance, Figure 12 shows a curly knot with a nested pair of i-circles, spiral index 4 and braid index 8. Although a general bound on braid index in terms of spiral index has not yet been found, we conjecture that a quadratic bound exists.

In Figure 13, we see a representative of a class of knots, which should yield braid index growing quadratically with spiral index. The knots should be taken to be alternating. The knot shown has spiral number 8 in this projection. It’s 21 i-circles are shaded. Let KnK_{n} be the corresponding generalization to an alternating knot in this class with spiral number at most nn, where n3n\geq 3. Note that the number of i-circles for such a projection is (n1)(n2)2\frac{(n-1)(n-2)}{2}. Utilizing the move from Figure 13 on each i-circle and then sliding strands to put the knot in braid form we can see that β[Kn]n+in2n+2)2\beta[K_{n}]\leq n+i\leq\frac{n^{2}-n+2)}{2}.

In fact, we expect that this is equality, and utilizing the MFW inequality (c.f.[3],[9]) to bound braid index from below, one can see this to be true for n=3,4,5n=3,4,5. It remains to prove the lower bound on braid index for n6n\geq 6.

Refer to caption
Figure 12. A Knot with sp[K]=4sp[K]=4 and β[K]=8\beta[K]=8.
Refer to caption
Figure 13. The knot K8K_{8} in the family {Kn}\{K_{n}\}.

The following proposition provides further evidence demonstrating the abundance of curly knots.

Proposition 2.8.

All twist knots of at least six crossings are curly.

Proof.

We denote a twist knot by TcT_{c}, where cc is the number of crossings in the “twist” portion of the knot (equivalently, TcT_{c} is the (c+2)(c+2)-crossing twist knot.) See Figure 14

We will first prove the result for odd twist knots. The HOMFLYPT polynomial of TnT_{n} for odd n is

PTn(v,z)=v2+vn+1vn+3z2(vn+1+vn1++1)P_{T_{n}}(v,z)=v^{2}+v^{n+1}-v^{n+3}-z^{2}(v^{n+1}+v^{n-1}+...+1)

Recall that the MFW inequality gives us that β[K]12v-breadthPK(v,z)+1\beta[K]\geq\frac{1}{2}\text{v-breadth}P_{K}(v,z)+1. This gives us the bound β[Tn]n+32\beta[T_{n}]\geq\frac{n+3}{2}. As shown in Figure 14, we can put any odd-crossing twist knot with at least 77 crossings in a spiral form with sp(Tn)=n+12sp(T_{n})=\frac{n+1}{2}, giving us the bound sp[Tn]n+12sp[T_{n}]\leq\frac{n+1}{2}. Thus sp[Tn]<β[Tn]sp[T_{n}]<\beta[T_{n}] for odd nn and TnT_{n} is curly. The HOMFLYPT polynomial of TmT_{m} where mm is even is

PTm(v,z)=v2+vmvm2z2(vm2+vm4++1)P_{T_{m}}(v,z)=v^{-2}+v^{m}-v^{m-2}-z^{2}(v^{m-2}+v^{m-4}+...+1)

The MFW inequality gives us that β[K]12v-breadthPK(v,z)+1\beta[K]\geq\frac{1}{2}\text{v-breadth}P_{K}(v,z)+1. Thus, we find that

β[Tm]m+42\beta[T_{m}]\geq\frac{m+4}{2}

We can similarly put any even-crossing twist knot with at least 66 crossings in a spiral form with sp(Tm)=m+22sp(T_{m})=\frac{m+2}{2}. Therefore sp[Tm]m+22sp[T_{m}]\leq\frac{m+2}{2}. Thus we have sp[Tm]m+22<m+42β[Tm]sp[T_{m}]\leq\frac{m+2}{2}<\frac{m+4}{2}\leq\beta[T_{m}], so sp[Tm]<β[Tm]sp[T_{m}]<\beta[T_{m}] for even m and TmT_{m} is curly. We conclude that all twist knots with at least 6 crossings are curly. Note that none of 313_{1}, 414_{1} or 525_{2} can be curly since they all have braid index 22 or 33. ∎

Refer to caption
Figure 14. Putting Odd Twists Knots in Spiral Form
Proposition 2.9.

sp[K1#K2]sp[K1]+sp[K2]1sp[K_{1}\#K_{2}]\leq sp[K_{1}]+sp[K_{2}]-1

Proof.

Take projections of conformations of K1K_{1} and K2K_{2} in minimal spiral form, α1(t)=P1(K1(t))\alpha_{1}(t)=P_{1}(K_{1}(t)) and α2(t)=P2(K2(t))\alpha_{2}(t)=P_{2}(K_{2}(t)).

We define an exterior arc to be an arc of the projection with no crossings except possibly at its end points such that the line that passes through its endpoints divides the plane so that the arc is the only piece of the knot on that side of the line.

We first claim that any knot projection has an exterior arc. Given a projection lying in 2\mathbb{R}^{2}, we can find such an arc by taking a horizontal line above the knot and lowering it until it touches the knot tangentially. Here it will intersect the knot at finitely many points. Take the point whose xx coordinate is the greatest; say this is α(t0)\alpha(t_{0}). Without loss of generality say we have chosen a parameterization with orientation going in the positive xx direction at α(t0)\alpha(t_{0}). Then there exists an ε>0\varepsilon>0 such that the set of tangent lines to points in α((t0,t0+ε))\alpha((t_{0},t_{0}+\varepsilon)) all intersect the knot in exactly one place (the point of tangency). A subset of those tangency points will be an exterior arc.

If α1\alpha_{1} or α2\alpha_{2} has an exterior arc that subtends an angle of π\geq\pi, we do no transformation to that knot projection. If a projection has no such exterior arc, we take an exterior arc that subtends a smaller angle. Since the arc subtends an angle less than π\pi, the tangent lines to the curve at the endpoints of the arc intersect on the exterior side of the plane. Put the plane of projection into 3\mathbb{R}^{3} such that the line through the end-points is along the xx-axis and the line perpendicular to the xx-axis that goes through the intersection point of the tangent lines be the zz-axis. Let (0,0,h)(0,0,h) be the intersection point of the tangent lines. Given this set-up, we perform a linear transformation onto the xyxy-plane given by:

T(x,0,z)=(xhhz,zhz,0)T(x,0,z)=(\frac{xh}{h-z},\frac{z}{h-z},0)

This transformation sends each point pp in the xzxz-plane where z<hz<h to the point where the ray from (0,1,h)(0,-1,h) and through pp intersects the xyxy-plane. Notice that this sends the tangent lines to the arc at its endpoints to parallel lines therefore the projection of the arc subtends an angle of π\pi.

Now we claim that TT preserves minimal spiral form. First of all since αi)\alpha_{i}) has no ss-inflection points, T(αi))T(\alpha_{i})) has no ss-inflection points because if T(αi))T(\alpha_{i})) had some ss-inflection point, p0=T(αi(t0)))p_{0}=T(\alpha_{i}(t_{0}))), then for any ε\varepsilon neighborhood of t0t_{0}, BεB_{\varepsilon}, the tangent line to the curve at p0p_{0} would have pieces of T(αi(Bε)))T(\alpha_{i}(B_{\varepsilon}))) to either side of the line. The plane that passes through the tangent line at p0p_{0} and the tangent line at T1(p0)T^{-1}(p_{0}) divides 3\mathbb{R}^{3} into two halves. T preserves the division into these two halves. However since αi)\alpha_{i}) has no ss-inflection points, there exists a δ\delta neighborhood of t0t_{0}, BδB_{\delta} such that αi(Bδ))\alpha_{i}(B_{\delta})) only on one side of this plane. Therefore T(αi(Bδ)))T(\alpha_{i}(B_{\delta}))) is only on one side of the plane, and thus only on one side of the tangent line so p0p_{0} is not an ss-inflection point.

Note that if we consider any map in the family of linear transformations

{fs(x,0,z)=(1s)P(x,0,z)+s(x,0,z)=(x+sxzhz,szhz,ztz)}\{f_{s}(x,0,z)=(1-s)P(x,0,z)+s(x,0,z)=(x+\frac{sxz}{h-z},\frac{sz}{h-z},z-tz)\}

and apply any of these fsf_{s} (where s[0,1]s\in[0,1]) to the spiral knot projection, there will be no inflection points in the image.

Finally, we assert that the transformation maintains minimal spiral form. Assume to the contrary, that the spiral number of the resulting projection is greater than the spiral number of the original projection. Then there must exist some s0s_{0} such that the image of the knot projection under fs0εf_{s_{0}-\varepsilon} differs in spiral number by one from the image of the knot projection under fs0+εf_{s_{0}+\varepsilon} for all ε>0\varepsilon>0 which are sufficiently small. The only way to transition to a higher spiral number requires a cusp. However, since αi\alpha_{i} is smooth, fsαif_{s}\circ\alpha_{i} is also smooth for any s[0,1]s\in[0,1] and therefore has no cusps.

Thus TT preserves minimal spiral form and gives us a projection of the knot which has an exterior arc which subtends an angle of at least π\pi. Using these spiral projections of K1K_{1} and K2K_{2} we can compose them by deleting the exterior arc subtending an angle of π\pi and connecting the loose ends with straight horizontal lines. This yields a spiral form of K1#K2K_{1}\#K_{2} which has spiral number equal to sp(K1)+sp(K2)1sp(K_{1})+sp(K_{2})-1 giving us the upper bound. ∎

Corollary 2.10.

There exist knots with arbitrarily large gaps between sp[K]sp[K] and β[K]\beta[K].

Proof.

Consider the knot 616_{1}, which has spiral index 3 and braid index 4, and compose it with n1n-1 copies of itself. Denote the resulting knot n61n6_{1}. Since braid index is subadditive under composition, β[n61]\beta[n6_{1}] increases by 33 as nn increases by 11. Since the spiral form of 616_{1} has two exterior arcs of curvature π\pi, we can compose it with itself nn times along these arcs and obtain a spiral form whose spiral number is nsp[61]nnsp[6_{1}]-n which means the spiral index can increase by at most 22 for each nn. Therefore the braid index becomes arbitrarily higher than the spiral index as nn increases. ∎

Note that an identical proof holds for any combination of curly knots composed with one another.

3. Projective Superbridge Number

We begin this section by introducing the projective superbridge number of a knot. This invariant minimizes the greatest number of maxima of a knot seen in a given projection.

Definition 4.

Let KK be a conformation of a knot in 3-space and, given vS2v\in S^{2}, let Pv(K)P_{v}(K) be the projection of KK onto a plane PP orthogonal vv. Now let μ(w,Pv(K))\mu(w,P_{v}(K)) denote the number of maxima of the knot projection with respect to its projection onto the vector wS1Pw\in S^{1}\subset P.

psb[K]=minK[K]minvS2maxwS1μ(w,PvK)psb[K]=\min_{K\in[K]}\min_{v\in S^{2}}\max_{w\in S^{1}}\mu(w,P_{v}K)

Note that we can define bridge index analogously as

b[K]=minK[K]minvS2minwS1μ(w,PvK)b[K]=\min_{K\in[K]}\min_{v\in S^{2}}\min_{w\in S^{1}}\mu(w,P_{v}K)

Moreover, the superbridge index of [5] is given by

sb[K]=minK[K]maxvS2maxwS1μ(w,PvK)sb[K]=\min_{K\in[K]}\max_{v\in S^{2}}\max_{w\in S^{1}}\mu(w,P_{v}K)

It follows immediately that b[K]psb[K]sb[K]b[K]\leq psb[K]\leq sb[K].

One of our primary interests in projective superbridge number is its relation to the stick index, s[K]s[K], of a knot KK. Stick index is the least number of line segments in 3-space, attached end to end, needed to realize a conformation of the given knot. The following result is useful in determining lower bounds for stick index.

Proposition 3.1.

For a knot KK, we have

s[K]2psb[K]+1s[K]\geq 2psb[K]+1
Proof.

Let KK be in minimal stick conformation and let vS2v\in S^{2} be a vector parallel to some edge of KK. Then in the projection Pv(K)P_{v}(K) only s[K]1s[K]-1 sticks are visible since we have projected directly down the chosen stick. Because in a generic stick projection extrema will only occur at the vertices, and half the extrema must be minima, our projection realizes at most s[K]12\frac{s[K]-1}{2} maxima relative to any vector in the plane. Further, there must be some vector wS1w\in S^{1} relative to which we see at least psb[K]psb[K] maxima. After minimizing over all conformations, we obtain the desired inequality. ∎

We now turn to the relationship between projective superbridge number and spiral index. Since a projection of a knot in spiral form has the same number of maxima over all directions in the plane, the greatest number of maxima in that projection is equal to the spiral number of that projection. After we minimize over all projections and all conformations, we see psb[K]sp[K]psb[K]\leq sp[K]. Because projective superbridge serves as a lower bound on stick number, we are interested in knots, KK, such that b[K]<psb[K]b[K]<psb[K]. For this case we see that s[K]2(b[K]+1)+1=2b[K]+3s[K]\geq 2(b[K]+1)+1=2b[K]+3. To this end, we have the following proposition.

Proposition 3.2.

If KK is a knot such that b[K]=psb[K]b[K]=psb[K], then sp[K]=b[K]sp[K]=b[K].

Proof.

Let b[K]=psb[K]b[K]=psb[K]. Then there is a projection P(K)P(K) of KK that realizes both b[K]b[K] and psb[K]psb[K]. Thus

minwS1μ(w,P(K))=maxwS1μ(w,P(K))\min_{w\in S^{1}}\mu(w,P(K))=\max_{w\in S^{1}}\mu(w,P(K))

This implies μ(w,C)\mu(w,C) is constant over all wS1Pw\in S^{1}\subset P. Hence, P(K)P(K) is in spiral form with μ(w,P(K))=b[K]\mu(w,P(K))=b[K] spirals so sp[K]b[K]sp[K]\leq b[K]. Since the reverse inequality always holds, the proposition follows. ∎

An example will help to illustrate the significance of the proposition above.

Example 1.

Consider 41#n314_{1}\#n3_{1}, the composition of the figure eight knot with n copies of the trefoil. This knot can be realized with 7+2n7+2n sticks. Since both bridge index and braid index are subadditive under composition and b[31]=b[41]=β[31]=2b[3_{1}]=b[4_{1}]=\beta[3_{1}]=2, β[41]=3\beta[4_{1}]=3, we have

b[41#n31]=n+2b[4_{1}\#n3_{1}]=n+2
β[41#n31]=n+3.\beta[4_{1}\#n3_{1}]=n+3.

If one could show b[41#n31]<psb[41#n31]b[4_{1}\#n3_{1}]<psb[4_{1}\#n3_{1}] or b[41#n31]<sp[41#n31]b[4_{1}\#n3_{1}]<sp[4_{1}\#n3_{1}] it would follow that s[41#n31]7+2ns[4_{1}\#n3_{1}]\geq 7+2n. This would provide the necessary lower bound in order to obtain the stick indices for this infinite family of knots. Note that we know that this is the case when n=1n=1.

Thus proving a subaddivity rule for spiral number under composition akin to that of braid index or bridge index would lead not only to a better understanding of that invariant but also to additional tools for calculating stick number.

Although a similar subadditivity result for projective superbridge index would give us useful bounds, we can in fact show by counterexample that projective superbridge index is not subadditive under composition.

Proposition 3.3.

The projective superbridge number of a knot is not always additive minus one under composition

Proof.

Consider the knot K=946K=9_{46}, which has the following properties:

b[K]\displaystyle b[K] =\displaystyle= 3\displaystyle 3
psb[K]\displaystyle psb[K] =\displaystyle= 4\displaystyle 4
s[K]\displaystyle s[K] =\displaystyle= 9\displaystyle 9

We know sp[K]=4sp[K]=4 (KK is not a 33-spiral knot and it is possible to put it in 44-spiral form). Apply 3.2 to get psb[K]=4psb[K]=4. Assume for sake of contradiction that psb[K1#K2]=psb[K1]+psb[K2]1psb[K_{1}\#K_{2}]=psb[K_{1}]+psb[K_{2}]-1. Then

psb[946#946]=4+41=7psb[9_{46}\#9_{46}]=4+4-1=7

Since 2psb[K]+1s[K]2psb[K]+1\leq s[K], we have

2(7)+1=15s[946]2(7)+1=15\leq s[9_{46}]

On the other hand 9469_{46} satisfies the conditions described in [2] so that we can save four sticks in composition to obtain the following upper bound on stick number:

s[K]9+94=14s[K]\leq 9+9-4=14

This implies that 15s[K]1415\leq s[K]\leq 14, providing a contradiction. ∎

4. Milnor’s Curvature-Torsion Invariant

We now relate the spiral index and the projective superbridge number of a knot to the curvature-torsion invariant defined by Milnor in [8]. For a knot KK, denote the number of inflection points in the projection Pv(K)P_{v}(K) by ν(Pv(K))\nu(P_{v}(K)), and the number of extrema in that projection with respect to a vector ww by μ^(w,Pv(K))\hat{\mu}(w,P_{v}(K)). Notice that for any projection Pv(K)P_{v}(K) and for any ww, μ^(w,Pv(K))=2μ(w,Pv(K))\hat{\mu}(w,P_{v}(K))=2\mu(w,P_{v}(K)).

Milnor defined the invariant curvature-torsion of a knot KK as

(κ+τ)[K]=infK[K]K(κ+|τ|)(\kappa+\tau)[K]=\inf_{K\in[K]}\int_{K}(\kappa+|\tau|)

More recently, Honma and Saeki proved the following theorem, which characterizes (κ+τ)[K](\kappa+\tau)[K] in terms of the number of critical points of the knot projection.

Theorem 4.1.

[4] Let KK be a knot. Then

1π(κ+τ)[K]=minK[K]minvS2minwS1(μ^(w,Pv(K))+ν(Pv(K)))\frac{1}{\pi}(\kappa+\tau)[K]=\min_{K\in[K]}\min_{v\in S^{2}}\min_{w\in S^{1}}(\hat{\mu}(w,P_{v}(K))+\nu(P_{v}(K)))

This characterization of (κ+τ)[K](\kappa+\tau)[K] allows us to relate this invariant to projective superbridge and allows us to answer an open question about (κ+τ)[K](\kappa+\tau)[K] that was posed by Honma and Saeki.

Theorem 4.2.

For a knot KK, we have

2πpsb[K](κ+τ)[K]2\pi psb[K]\leq(\kappa+\tau)[K]

Let P(K)P(K) be a smooth oriented projection of a knot conformation KK into some plane PP. Then extrema in this projection are measured relative to vectors wS1Pw\in S^{1}\subset P. We call vS1v\in S^{1} a local extrema changing vector at xP(K)x\in P(K) if for any neighborhood xBP(K)x\in B\subset P(K),

(3) μ^(v+ε,B)=μ^(vε,B)±2n\displaystyle\hat{\mu}(v+\varepsilon,B)=\hat{\mu}(v-\varepsilon,B)\pm 2n

for all sufficiently small ε\varepsilon. We will call nn the local multiplicity of vv at xx. We call vv an extrema changing vector with multiplicity nn if (3) holds for B=P(K).B=P(K).

Denote the unit tangent vector to P(K)P(K) at pp by TpT_{p}. Define NpN_{p} to be the rotation of TpT_{p} by π2\frac{\pi}{2} in the counterclockwise direction. Given any point pP(K)p\in P(K), pp is a critical point with respect to a vector ww when TpT_{p} is orthogonal to ww. Assuming that TpT_{p} is orthogonal to ww, note that if TqT_{q}, for a point qpq\neq p, is some oriented angle θ\theta away from TpT_{p} then qq is a critical point with respect to some w~\tilde{w} which is θ\theta away from ww. This corresponds to rotating the Frenet frame by the angle θ\theta. Further, if our curve has nonzero curvature at qq then qq is an extremum with respect to w~\tilde{w}. To prove our theorem we will need the following lemma.

Lemma 4.3.

Let α\alpha be a immersed curve in 2\mathbb{R}^{2} with no uu-inflection points. Then for each extrema changing vector v0v_{0} with multiplicity nn there are nn ss-inflection points xix_{i} such that v0=±Nxiv_{0}=\pm N_{x_{i}}. Further, if xx is an ss-inflection point on α\alpha, then ±Nx\pm N_{x} are local extrema changing vectors.

Proof.

Let α(t)\alpha(t) be an immersed curve with no uu-inflection points. Given some extrema changing vector, v0S1v_{0}\in S^{1}, consider the set of points, α(t1)=x1,,α(tn)=xn\alpha(t_{1})=x_{1},...,\alpha(t_{n})=x_{n} such that v0=±Nxiv_{0}=\pm N_{x_{i}}. These are the critical points on α\alpha with respect to v0v_{0}. Let ε>0\varepsilon>0 and let B(v0,ε)B(v_{0},\varepsilon) be a neighborhood of v0v_{0} in S1S^{1} of all vectors whose angle from v0v_{0} is less than ε\varepsilon. We first show that for any α(t0)=yxi\alpha(t_{0})=y\neq x_{i}, there is a neighborhood ByαB_{y}\subset\alpha of yy such that for any zByz\in B_{y}, zz is not a critical point with respect to any vB(v0,ε)v\in B(v_{0},\varepsilon).

Consider the continuous function

g:S1×S1g:S^{1}\times S^{1}\rightarrow\mathbb{R}

defined by g(t,v)=α(t)vg(t,v)=\alpha^{\prime}(t)\cdot v. Let y=α(t0)xiy=\alpha(t_{0})\neq x_{i} for any ii. Then g(t0,v0)0g(t_{0},v_{0})\neq 0 and there exists an open product neighborhood U×VU\times V of (t0,v0)(t_{0},v_{0}) such that g(s,v)0g(s,v)\neq 0 for any (s,v)U×V(s,v)\in U\times V. Set By=α(U)B_{y}=\alpha(U). Therefore there is a neighborhood of α(t0)\alpha(t_{0}) such that none of the points in that neighborhood are critical points with respect to any vv in some neighborhood of v0v_{0}. Thus, in order to locate the critical points of α\alpha with respect to vectors close to v0v_{0} it suffices to restrict ourselves to neighborhoods of the points xix_{i}.

Now we prove that the only possible extrema changing points with respect to v0v_{0} are places where curvature is zero. Reorder so that α(t1)=x1,,α(tk)=xk\alpha(t_{1})=x_{1},...,\alpha(t_{k})=x_{k} are all the critical points which are not inflection points. Using the same function gg as above, g(ti,v0)=0g(t_{i},v_{0})=0 and

gt(ti,v0)=α′′(ti)v0=±κ(α(ti))0\frac{\partial g}{\partial t}(t_{i},v_{0})=\alpha^{\prime\prime}(t_{i})\cdot v_{0}=\pm\kappa(\alpha(t_{i}))\neq 0

for 1ik1\leq i\leq k. Therefore, by the implicit function theorem there are functions

hi:UVih_{i}:U\rightarrow V_{i}

where UU is a neighborhood of v0v_{0} and ViV_{i} is a neighborhood of tit_{i} such that g(v,hi(v))=0g(v,h_{i}(v))=0 for all vUv\in U. Thus we have a continuous, one to one correspondence between vectors vv in a neighborhood of v0v_{0} and points xx in a neighborhood of xix_{i} such that xx is an extrema with respect to vv. Then on either side of v0v_{0} there is one extrema with respect to that vector in α(Vi)\alpha(V_{i}) for each 1ik1\leq i\leq k, which implies that v0v_{0} is not locally extrema changing near xix_{i} for 1ik1\leq i\leq k. By our first argument all extrema changes must occur in neighborhoods of the xix_{i}, 1in1\leq i\leq n. Therefore the bridge change across v0v_{0} is at most 2(nk)2(n-k). (Note nkn-k is the number of inflection points whose normal is ±v\pm v.)

We now show that the normal vector to an ss-inflection point on α\alpha is an extrema changing vector with local multiplicity 22. Since any extrema changing vector must be the normal or antinormal of an inflection point and the normal of each inflection point changes the extrema count locally by 22, this will imply that a extrema changing vector with multiplicity nn will be the normal or antinormal of nn inflection points.

At an ss-inflection point, α(ti)=xi\alpha(t_{i})=x_{i}, curvature changes signs. Without loss of generality assume κ(tiε)<0\kappa(t_{i}-\varepsilon)<0 and κ(ti+ε)>0\kappa(t_{i}+\varepsilon)>0 for all sufficiently small ε>0\varepsilon>0. Then, in this neighborhood of tit_{i} the Frenet frame rotates clockwise as tt increases through parameter in (tiε,ti)(t_{i}-\varepsilon,t_{i}) and counterclockwise as tt increases through (ti,ti+ε)(t_{i},t_{i}+\varepsilon). Then all points within this neighborhood of tit_{i} have normal vectors counterclockwise of NxiN_{x_{i}}. Thus in any small neighborhood of NxiN_{x_{i}}, vectors clockwise to NxiN_{x_{i}} are not the normal vectors to any points α(t)\alpha(t) for all t(tε,t+ε)t\in(t-\varepsilon,t+\varepsilon) and each vector in this neighborhood counterclockwise of vv is the normal vector to exactly two extrema in (tε,t+ε)(t-\varepsilon,t+\varepsilon). Then since the normal vector to each inflection point on the curve corresponds to a local extrema change of two and any bridge changing vector must be the normal vector of some inflection point, the lemma follows. ∎

Proof of Theorem 4.2.

We begin by noting that the projection that minimized μ^(w,Pv(K))+ν(Pv(K))\hat{\mu}(w,P_{v}(K))+\nu(P_{v}(K)) cannot have a uu-inflection point. Otherwise, we may eliminate the inflection point, xx, by a planar isotopy that gives xx the sign of curvature corresponding to the curvature in some deleted neighborhood of xx.

Now consider a knot projection that minimizes μ^(w,Pv(K))+ν(Pv(K))\hat{\mu}(w,P_{v}(K))+\nu(P_{v}(K)) and contains no cusps. Such a projection is guaranteed to exist by the results of Honma and Saeki [4]. Then we may parameterize our knot projection by an immersed curve α\alpha with no uu-inflection points. By the previous lemma each change in number of extrema by 22 along α\alpha has a corresponding inflection point. Consider vv such that μ^(v,P(K))\hat{\mu}(v,P(K)) is minimal among vS1v\in S^{1}. Because μ^(v,P(K))=μ^(v,P(K))\hat{\mu}(v,P(K))=\hat{\mu}(-v,P(K)), the maximal number of extrema occurs between vv and v-v. To get to the direction, say ww, with the maximal number of extrema, we need one inflection point for each pair of extrema. Since we gain the same number of extrema between vv and ww and between v-v and ww, we get that

maxwS1μ^(w,α)minwS1μ^(w,α)ν(α)\max_{w\in S^{1}}\hat{\mu}(w,\alpha)-\min_{w\in S^{1}}\hat{\mu}(w,\alpha)\leq\nu(\alpha)

Then we have

2maxvS1μ(v,α)=maxvS1μ^(v,α)minK[K]minvS2minwS1(μ^(w,Pv(K))+ν(Pv(K)))2\max_{v\in S^{1}}\mu(v,\alpha)=\max_{v\in S^{1}}\hat{\mu}(v,\alpha)\leq\min_{K\in[K]}\min_{v\in S^{2}}\min_{w\in S^{1}}(\hat{\mu}(w,P_{v}(K))+\nu(P_{v}(K)))

By the previous theorem, the right side of this equality equals (κ+τ)[K]π\frac{(\kappa+\tau)[K]}{\pi}. Further, minimizing the left side of the inequality over both projections and conformation of KK provides 2psb[K]2psb[K]. Hence, we obtain the desired inequality. ∎

The bound on curvature-torsion given in [4] and the previous theorem provide the following bound for projective superbridge in terms of bridge index.

Proposition 4.4.

For a knot KK, psb[K]2b[K]1psb[K]\leq 2b[K]-1.

Proof.

Honma and Saeki [4] prove that for every knot KK,

(κ+τ)[K]2π2(κ[K]2π)(\kappa+\tau)[K]-2\pi\leq 2(\kappa[K]-2\pi)

where κ[K]\kappa[K] denotes the total curvature of [K][K]. By a result of Milnor [8], we know that κ[K]=2πb[K]\kappa[K]=2\pi b[K]. Applying this and Theorem 4.2 to the above inequality, we get that

2π(psb[K])2π2(2πb[K]2π)2\pi(psb[K])-2\pi\leq 2(2\pi b[K]-2\pi)

and obtain psb[K]2b[K]1psb[K]\leq 2b[K]-1. ∎

We now relate the curvature-torsion of a knot to its spiral index.

Proposition 4.5.

For any knot KK, (κ+τ)[K]2πsp[K](\kappa+\tau)[K]\leq 2\pi sp[K].

Proof.

Consider a spiral projection P(K)P(K) of a conformation of KK which realizes sp[K]sp[K]. Then P(K)P(K) has no ss-inflection points and, as in the above proof, we may elimate each uu-inflection points while remaining in spiral form. Thus, P(K)P(K) has 2sp[K]sp[K] extrema, which implies that

μ^(v,P(K))+ν(P(K))=μ^(v,P(K))=2sp[K]\hat{\mu}(v,P(K))+\nu(P(K))=\hat{\mu}(v,P(K))=2sp[K]

Minimizing the left side of this equation over all projections and conformations provides the desired equality. ∎

We now have the tools necessary to characterize all knots KK for which
(κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi, a question posed in [4].

Proposition 4.6.

For a knot KK, (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi if and only if psb[K]=3psb[K]=3. Further, these knots are precisely the 2-bridge knots that are not 2-braid and the 3-spiral knots.

Proof.

If (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi then psb[K]3psb[K]\leq 3. However, if psb[K]=2psb[K]=2 then sp[K]=β[K]=2sp[K]=\beta[K]=2 and KK is a 2-braid knot. However, Milnor has proved that 2-braid knots have curvature-torsion equal to 4π4\pi. Therefore, (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi implies that psb[K]=3psb[K]=3.

Conversely, assume that psb[K]=3psb[K]=3. Then b[K]b[K] is either 22 or 33. If b[K]=2b[K]=2 then Honma and Saeki have proved that (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi whenever β[K]>2\beta[K]>2. If b[K]=3b[K]=3, then b[K]=psb[K]=sp[K]=3b[K]=psb[K]=sp[K]=3 and (κ+τ)[K]6π(\kappa+\tau)[K]\leq 6\pi since curvature-torsion is no greater than spiral index times 2π2\pi. Since (κ+τ)[K](\kappa+\tau)[K] is greater than or equal to 2πpsb[K]2\pi psb[K], (κ+τ)[K]=6π(\kappa+\tau)[K]=6\pi.

By the argument above, psb[K]=3psb[K]=3 implies that either b[k]=2b[k]=2 with β[K]>2\beta[K]>2 or sp[K]=3sp[K]=3 as desired. Further, if b[K]=2b[K]=2 then psb[K]2b[K]1=3psb[K]\leq 2b[K]-1=3. If β>2\beta>2 then psb[K]2psb[K]\neq 2 implying that psb[K]=3psb[K]=3. If sp[K]=3sp[K]=3 then psb[K]=3psb[K]=3, since psb[K]=2psb[K]=2 would imply that KK is a 2-braid. ∎

We have also determined that for a knot KK with fewer than 99 crossings, 2πpsb[K]=(κ+τ)[K]2\pi psb[K]=(\kappa+\tau)[K]. It remains open whether there exists a knot KK where 2πpsb[K]<(κ+τ)[K]2\pi psb[K]<(\kappa+\tau)[K].

References

  • [1] J.W. Alexander. A lemma on systems of knotted curves. Proceedings of the National Academy of Sciences of the United States of America, 9(3):93–95, Mar. 1923.
  • [2] B. Brennan C. Adams and D. Greilsheimer. Stick numbers and compositions of knots and links. Journal of Knot Theory and its Ramifications, 6(2):149–161, 1997.
  • [3] J. Franks and R.F. Williams. Braids and the Jones polynomial. Transactions of the American Mathematical Society, 303(1):97–108, Sep. 1987.
  • [4] N. Honma and O. Saeki. On Milnor’s curvature-torsion invariant for knots and links. Kobe J. Math, 11(2):225–239, 1994.
  • [5] N. Kuiper. A new knot invariant. Math. Ann., 278:193–209, 1987.
  • [6] W. Menasco. Closed incompressible surfaces in alternating knots and link complements. Topology, 23(1):37–44, 1984.
  • [7] W. Menasco and M. Thistlethwaite. The classification of alternating links. Annals of Mathematics, 138(1):113–171, 1993.
  • [8] J. Milnor. On total curvatures of closed space curves. Mathematica Scandinavica, pages 289–296, 1953.
  • [9] H.R. Morton. Seifert circles and knot polynomials. Math. Proc. Cambridge Philos. Soc., 99(1):107–109, 1986.
  • [10] S. Yamada. The minimal number of seifert circles equals the braid index of a link. Inventiones Mathematicae, 89(2):347–356, Jun. 1987.