Upper bounds on the minimal length of cubic lattice knots

# Upper bounds on the minimal length of cubic lattice knots

Kyungpyo Hong Department of Mathematics, Korea University, Anam-dong, Sungbuk-ku, Seoul 136-701, Korea Sungjong No Department of Mathematics, Korea University, Anam-dong, Sungbuk-ku, Seoul 136-701, Korea  and  Seungsang Oh Department of Mathematics, Korea University, Anam-dong, Sungbuk-ku, Seoul 136-701, Korea
###### Abstract.

Knots have been considered to be useful models for simulating molecular chains such as DNA and proteins. One quantity that we are interested on molecular knots is the minimum number of monomers necessary to realize a knot. In this paper we consider every knot in the cubic lattice. Especially the minimal length of a knot indicates the minimum length necessary to construct the knot in the cubic lattice. Diao introduced this term (he used “minimal edge number” instead) and proved that the minimal length of the trefoil knot is . Also the minimal lengths of the knots and are known to be and , respectively. In the article we find a general upper bound of the minimal length of a nontrivial knot , except the trefoil knot, in terms of the minimal crossing number . The upper bound is . Moreover if is a non-alternating prime knot, then the upper bound is . Our work are considerably direct consequences of the results done by the authors in . Furthermore if is -torus knot, then the upper bound is .

PACS numbers: 02.10.Kn, 82.35.Pq, 02.40.Sf
This work was supported by the National Research Foundation of Korea(NRF) grant funded by the Korea government (MEST) (No. 2009-0074101).

## 1. Introduction

A knot is a closed curve in -space . Knots are commonly found in molecular chains such as DNA and proteins, and they have been considered to be useful models for structural analysis of these molecules. A knot can be embedded in many different ways in -space, smooth or piecewise linear. Polygonal knots are those which consist of finite line segments, called sticks, attached end-to-end. This representation of knots is very useful for many applications in Science. The microscopic level molecules are more similar to rigid sticks than a flexible rope. In fact the DNA strand is made up of small rigid sticks of sugar, phosphorus, nucleotide proteins, and hydrogen bonds. Chemists are also interested in knotted molecules which are formed by a sequence of atoms bonded end-to-end so that the last one is also bonded to the first.

A question that naturally arises from these studies is the following. What is the smallest number of atoms needed to construct a nontrivial knotted molecule? This question has been addressed by a theoretical study of polygonal knots in lattices . Here we aim to determine the minimum length needed to construct a knot in the simple cubic lattice. A lattice knot is a polygonal knot in the cubic lattice . For further studies on lattice knots the readers are referred to [7, 8, 9, 12, 13, 14, 17, 18, 20]. An edge is a line segment of unit length joining two nearby lattice points in . Obviously a stick with length of a lattice knot consists of edges.

The minimum number of edges necessary to realize a knot as a lattice knot is called the minimal length. The minimal length was numerically estimated for various knots [11, 15, 19]. Furthermore such estimation was mathematically confirmed for few small knots. Diao proved rigorously that the minimal length of any nontrivial lattice knot is at least and only the trefoil knot can be realized with edges . Later it was proved that the minimal length of and are and , respectively . Lattice knots with the minimal length of the knots , , and are depicted in Figure 1.

In the article we find a general upper bound of the minimal length of a nontrivial lattice knot in terms of the minimal crossing number . The following theorem is the main result of this article.

###### Theorem 1.

Let be a nontrivial knot which is not the trefoil knot . Then the minimal length of is at most . Moreover if is a non-alternating prime knot, then the minimal length is at most . Furthermore if is -torus knot, then the minimal length is at most .

## 2. Definitions

In this section, we introduce several definitions and terminology. For convenience the notations concerning the and -coordinates will be defined in the same manner as the -coordinate. A stick in parallel to the -axis is called an -stick and an edge parallel to the -axis is called an -edge. We denote an -stick for some integers and . The plane with the equation for some integer is called an -level . So each -stick or -stick lies on an -level for some . Note that the -stick whose endpoints lie on -levels and has length , and so consists of -edges. A lattice knot is said to be properly leveled if each -level (resp. , -level) contains exactly two endpoints of -sticks (resp. , -sticks). If a properly leveled lattice knot has -levels, then we may say that these are -levels like heights without changing the knot type.

###### Lemma 2.

If a properly leveled lattice knot has -levels, then this lattice knot contains at most -edges if is odd, or -edges if is even.

###### Proof.

By proper leveledness there are exactly two -edges between -level and (similarly for and ). And there are at most four -edges between -level and (similarly for and ). Keep going to add two -edges when -levels approach to the middle level. Then the maximum number of -edges is if is odd, or if is even. ∎

There is an open-book decomposition of which has open half-planes as pages and the standard -axis as the binding axis. We may regard each page as a half-plane at angle when the - plane has a polar coordinate. It can be easily shown that every knot can be embedded in an open-book with finitely many pages so that it meets each page in a simple arc. Such an embedding is called an arc presentation of . And the arc index is defined to be the minimal number of pages among all possible arc presentations of . For example, the left figure in Figure 2 shows an arc presentation of figure- knot which has the arc index . Here the points of on the binding axis are called binding indices, assigned by from bottom to top. Also we assign the page numbers to all of the arcs from the back page to the front. For further studies on arc presentation the readers are referred to .

In this paper we find an upper bound of the minimal length in terms of arc index. The following theorem has key role to convert it to an upper bound in terms of crossing number. Bae and Park established an upper bound on arc index in terms of crossing number. In their paper , Corollary and Theorem provide that , and moreover if is a non-alternating prime knot. Later Jin and Park improved the second part of Bae and Park’s theorem. Theorem in  provides that if is a non-alternating prime knot, then .

###### Theorem 3.

Let be any nontrivial knot. Then . Moreover if is a non-alternating prime knot, then .

We move the binding axis to the line on the - plane and replace each arc by two connected sticks which are an -stick and a -stick properly below the line . For better view we slightly perturb each pair of sticks which are overlapped. The resulting is called a lattice arc presentation of the knot on the plane. See the right figure in Figure 2. This lattice arc presentations of knots are very useful to construct lattice knots in .

## 3. Proof of Theorem 1

The key idea of the construction of a proper lattice knot is given by the authors in . The following two lemmas are almost direct consequences of Lemma , , and in the paper. For completeness we recall the proofs of the lemmas.

###### Lemma 4.

Let be a nontrivial knot with the arc index . Then we can realize as a properly leveled lattice knot by using -sticks, -sticks, and -sticks.

###### Proof.

We begin with a lattice arc presentation of with arcs as the right figure in Figure 2. To realize each arc which has the page number and the binding indices and (assume that ) at its endpoints for some , we build two sticks and on . And then we connect each pair of arcs which share a binding index, say , by a -stick where and are the page numbers of the pair. The resulting lattice knot is properly leveled and consists of -sticks, -sticks, and -sticks. See the left figure in Figure 3.

Still we have a chance to reduce more sticks as follows. Consider the two -sticks and the -stick lying on -level . These two -sticks are and (assume that and ), so this -stick is . Delete the shorter -stick , and replace the other two sticks by an -stick and a -stick . We repeat this replacement for the two -sticks and the -stick lying on -level . The final lattice knot is also properly leveled and consists of -sticks, -sticks, and -sticks as the right figure in Figure 3. ∎

###### Lemma 5.

Let be a nontrivial knot with the arc index . Suppose that is not -torus knot. Then we can realize as a properly leveled lattice knot by using -sticks, -sticks, and -sticks.

###### Proof.

The proofs of Lemmas and in  guarantee that if is not -torus knot, then we have a special lattice arc presentation of so that an arc with the page number has the binding indices and , and another arc has the binding indices and satisfying . In more details, this special lattice arc presentation can be obtained from, so called, a non-star shaped arc presentation of as the first paragraph in the proof of Lemma in . Note that if has a star shaped arc presentation and is not -torus knot, then its dual arc presentation, so called, converts into a non-star shaped arc presentation as the last paragraph in the proof of Lemma in .

Let be the page number of the arc . See the figures in Figure 4 for better understanding. We slightly change the related lattice arc presentation so that only the arc lies above the line . This does not change the knot because does not touch the other part of when rotating it around the binding axis. Now repeat the whole part of the proof of Lemma 4. Notice that the arc is not involved in the reduction of two sticks on -level and -level since does not have the binding indices and .

Still we can lift up through the -axis till it reaches the -level with replacing -sticks properly. Indeed the new -stick of lies on the same line containing the -stick of the arc . This means that we can delete an -stick and an -stick. The resulting lattice knot is obviously properly leveled and consists of -sticks, -sticks, and -sticks. ∎

Now we are ready to prove the main theorem.

###### Proof of Theorem 1.

Let be a nontrivial knot which is not the trefoil knot. Suppose that is not -torus knot. By Lemma 5 and Theorem 3, can be realized as a properly leveled lattice knot by using -sticks, -sticks, and -sticks. By using Lemma 2, this lattice knot consists of at most edges if is odd, or edges if is even. These equations imply that the lattice knot consists of at most edges.

Moreover if is a non-alternating prime knot, then -sticks, -sticks, and -sticks are sufficient. The same calculations show that the lattice knot consists of edges.

Suppose that is -torus knot for . These are well-known facts that and . So . By Lemma 4, can be realized as a properly leveled lattice knot by using -sticks , -sticks, and -sticks. By using Lemma 2 again, this lattice knot consists of at most edges. ∎

## 4. Conclusion

Knots are commonly found in molecular chains such as DNA and proteins, and they have been considered to be useful models for structural analysis of these molecules. In the laboratory, the microscopic level molecules are more similar to rigid sticks than a flexible rope. In this context, we will consider a knot which consist of finite line segments in the cubic lattice. It is natural to ask what is the smallest number of atoms needed to construct a nontrivial knotted molecule? We propose upper bounds on the minimal length of any cubic lattice knots. For small knots , and , their minimal lengths are already known as 24, 30 and 34, respectively [5, 19]. Also the minimal length was numerically estimated for various knots [11, 15, 19]. In these papers the upper bounds of the minimal lengths of knots with crossing numbers 4, 5, 6, 7 and 8 are 30, 36, 40, 46 and 52, and our upper bound formula gives the upper bounds as 32, 48, 66, 88 and 112, respectively. These upper bounds are rather loose even for small knots, and will be very loose for knots with larger number of crossings. However, we need to point out that our upper bound formula is obtained by purely analytic calculations instead of numerical calculations.

Finally we better mention the term “minimum ropelength” which is closely related to the minimal length. The ropelength of a knot is defined to be the quotient of its length by its thickness, where thickness is the radius of the largest embedded tubular neighborhood around the knot. Indeed the minimum ropelength of a knot is less than or equal to two times of the minimal length of the knot. In , they found an upper bound of the minimum ropelength of a non-split link which is . Also in , another upper bound is proposed.

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