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Writhes and 2k2k-moves for virtual knots

Kodai Wada Department of Mathematics, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japan [email protected]
Abstract.

A 2k2k-move is a local deformation adding or removing 2k2k half-twists. We show that if two virtual knots are related by a finite sequence of 2k2k-moves, then their nn-writhes are congruent modulo kk for any nonzero integer nn, and their odd writhes are congruent modulo 2k2k. Moreover, we give a necessary and sufficient condition for two virtual knots to have the same congruence class of odd writhes modulo 2k2k.

Key words and phrases:
virtual knot, nn-writhe, odd writhe, 2k2k-move, Ξ\Xi-move
2020 Mathematics Subject Classification:
Primary 57K12; Secondary 57K10
This work was supported by JSPS KAKENHI Grant Numbers JP21K20327 and JP23K12973.

1. Introduction

Let kk be a positive integer. A 2k2k-move on a knot diagram is a local deformation adding or removing 2k2k half-twists as shown in Figure 1.1. A 22-move is equivalent to a crossing change; that is, a 22-move is realized by a crossing change, and vice verse. In this sense, a 2k2k-move can be considered as a generalization of a crossing change. The 2k2k-moves form an important family of local moves in classical knot theory. In fact, they have been well studied by means of many invariants of classical knots and links; for example, Alexander polynomials [12], Jones, HOMFLYPT and Kauffman polynomials [16], Burnside groups [5, 6] and Milnor invariants [14].

\begin{overpic}[width=199.16928pt]{2k-move.pdf} \put(81.0,25.0){$2k$} \put(119.5,-12.0){$2k$ half-twists} \end{overpic}
Figure 1.1. A 2k2k-move

Recently, Jeong, Choi and Kim [8] extended the classical study of 2k2k-moves to the setting of virtual knots, which are a generalization of classical knots discovered by Kauffman [9]. Roughly speaking, a virtual knot is an equivalence class of generalized knot diagrams called virtual knot diagrams under seven types of local deformations. We say that two virtual knots KK and KK^{\prime} are related by a 2k2k-move if a diagram of KK^{\prime} is a result of a 2k2k-move on a diagram of KK.

For a virtual knot KK, Kauffman [10] defined an integer-valued invariant J(K)J(K) called the odd writhe. Satoh and Taniguchi [17] generalized it to a sequence of integer-valued invariants Jn(K)J_{n}(K) of KK called the nn-writhes. This sequence {Jn(K)}n0\{J_{n}(K)\}_{n\neq 0} gives rise to a polynomial invariant PK(t)P_{K}(t) of KK known as the the affine index polynomial [11], which is essentially equivalent to the writhe polynomial [4]. Refer to [3] for a good survey of virtual knot invariants derived from chord index, including J(K)J(K), Jn(K)J_{n}(K) and PK(t)P_{K}(t).

In [8, Theorem 2.3], Jeong, Choi and Kim established a necessary condition for two virtual knots to be related by a finite sequence of 2k2k-moves using their affine index polynomials. Examining the proof of [8, Theorem 2.3], we can find another necessary condition for such a pair of virtual knots in terms of the nn-writhes and odd writhes. The first aim of this paper is to prove the following.

Theorem 1.1.

If two virtual knots KK and KK^{\prime} are related by a finite sequence of 2k2k-moves, then the following hold:

  1. (i)

    Jn(K)Jn(K)(modk)J_{n}(K)\equiv J_{n}(K^{\prime})\pmod{k} for any nonzero integer nn.

  2. (ii)

    J(K)J(K)(mod2k)J(K)\equiv J(K^{\prime})\pmod{2k}.

Although the assertion (i) in this theorem is obtained from [8, Theorem 2.3] immediately, the author believes that it is worth stating it as a separate result.

A Ξ\Xi-move on a virtual knot diagram is a local deformation exchanging the positions of c1c_{1} and c3c_{3} of three consecutive real crossings c1c_{1}, c2c_{2} and c3c_{3} as shown in Figure 1.2, where we omit the over/under information of each crossing cic_{i} (i=1,2,3)(i=1,2,3). The Ξ\Xi-move arises naturally as a diagrammatic characterization of virtual knots having the same odd writhe. In fact, Satoh and Taniguchi [17] proved the following.

\begin{overpic}[width=170.71652pt]{Xi-move.pdf} \put(72.75,33.0){$\Xi$} \put(17.0,40.0){$c_{1}$} \put(17.0,21.0){$c_{2}$} \put(17.0,2.0){$c_{3}$} \put(121.5,52.0){$c_{3}$} \put(121.5,20.0){$c_{2}$} \put(121.5,2.0){$c_{1}$} \end{overpic}
Figure 1.2. A Ξ\Xi-move
Theorem 1.2 ([17, Theorem 1.7]).

For two virtual knots KK and KK^{\prime}, the following are equivalent:

  1. (i)

    J(K)=J(K)J(K)=J(K^{\prime}).

  2. (ii)

    KK and KK^{\prime} are related by a finite sequence of Ξ\Xi-moves.

Inspired by this theorem, we use Ξ\Xi-moves together with 2k2k-moves to characterize virtual knots having the same congruence class of odd writhes modulo 2k2k. The second aim of this paper is to prove the following.

Theorem 1.3.

For two virtual knots KK and KK^{\prime}, the following are equivalent:

  1. (i)

    J(K)J(K)(mod2k)J(K)\equiv J(K^{\prime})\pmod{2k}.

  2. (ii)

    KK and KK^{\prime} are related by a finite sequence of 2k2k-moves and Ξ\Xi-moves.

Although the crossing change is an unknotting operation for classical knots, it was shown by Carter, Kamada and Saito in [1, Proposition 25] that not every virtual knot can be unknotted by crossing changes. This fact justifies the notion of flat virtual knots. A flat virtual knot [9] is an equivalence class of virtual knots up to crossing changes. Equivalently, a flat virtual knot is represented by a virtual knot diagram with all the real crossings replaced by flat crossings, where a flat crossing is a transverse double point with no over/under information.

In [2, Lemma 2.2], Cheng showed that the odd writhe for any virtual knot takes values in even integers. Therefore any virtual knot KK and the trivial one OO satisfy J(K)J(O)0(mod2)J(K)\equiv J(O)\equiv 0\pmod{2}. By Theorem 1.3 for k=1k=1, the two knots KK and OO are related by a finite sequence of crossing changes and Ξ\Xi-moves. In other words, we have the following.

Corollary 1.4.

Any flat virtual knot can be deformed into the trivial knot by a finite sequence of flat Ξ\Xi-moves; that is, the flat Ξ\Xi-move is an unknotting operation for flat virtual knots. Here, a flat Ξ\Xi-move is a Ξ\Xi-move with all the real crossings replaced by flat ones. ∎

The rest of this paper is organized as follows. In Section 2, we review the definitions of a virtual knot, a Gauss diagram, the nn-writhe and the odd writhe, and prove Theorem 1.1. Section 3 is devoted to the proof of Theorem 1.3. Our main tool is the notion of shell-pairs, which are certain pairs of chords of a Gauss diagram introduced in [13]. In the last section, for two virtual knots KK and KK^{\prime} that are related by a finite number of 2k2k-moves, we study their 2k2k-move distance d2k(K,K)\mathrm{d}_{2k}(K,K^{\prime}) defined as the minimal number of such 2k2k-moves. We show that for any virtual knot KK and any positive integer aa, there is a virtual knot KK^{\prime} such that d2k(K,K)=a\mathrm{d}_{2k}(K,K^{\prime})=a (Proposition 4.2).

2. Proof of Theorem 1.1

We begin this section by recalling the definitions of virtual knots and Gauss diagrams from [7, 9].

A virtual knot diagram is the image of an immersion of an oriented circle into the plane whose singularities are only transverse double points. Such double points consist of positive, negative and virtual crossings as shown in Figure 2.1. A positive/negative crossing is also called a real crossing.

\begin{overpic}[width=170.71652pt]{xing.pdf} \put(0.8,-12.0){positive} \put(67.25,-12.0){negative} \put(139.0,-12.0){virtual} \end{overpic}
Figure 2.1. Types of double points

Two virtual knot diagrams are said to be equivalent if they are related by a finite sequence of generalized Reidemeister moves I–VII as shown in Figure 2.2. A virtual knot is the equivalence class of a virtual knot diagram. In particular, a classical knot can be considered as a virtual knot diagram with no virtual crossings, called a classical knot diagram, up to the moves I, II and III. In [7, Theorem 1.B], Goussarov, Polyak and Viro proved that two equivalent classical knot diagrams are related by a finite sequence of moves I, II, and III; in other words, the set of virtual knots contains that of classical knots. In this sense, virtual knots are a generalization of classical knots.

\begin{overpic}[width=341.43306pt]{gReid-move.pdf} \put(33.5,162.0){I} \put(68.5,162.0){I} \put(162.5,162.0){II} \put(278.5,162.0){III} \put(48.0,92.0){IV} \put(162.5,92.0){V} \put(278.5,92.0){VI} \put(158.5,23.0){VII} \end{overpic}
Figure 2.2. Generalized Reidemeister moves I–VII

A Gauss diagram is an oriented circle equipped with a finite number of signed and oriented chords whose endpoints lie disjointly on the circle. In figures the underlying circle and chords of a Gauss diagram will be drawn with thick and thin lines, respectively. Gauss diagrams provide an alternative way of representing virtual knots. For a virtual knot diagram DD with nn real crossings (and some or no virtual crossings), the Gauss diagram GDG_{D} associated with DD is constructed as follows. It consists of a circle and nn chords connecting the preimage of each real crossing of DD. Each chord of GDG_{D} has the sign of the corresponding real crossing of DD, and it is oriented from the overcrossing to the undercrossing. For a virtual knot KK, a Gauss diagram of KK is defined to be a Gauss diagram associated with a virtual knot diagram of KK.

A motivation of introducing virtual knot theory comes from the realization of Gauss diagrams. In fact, the construction above defines a surjective map from virtual knot diagrams onto Gauss diagrams, although not every Gauss diagram can be realized by a classical knot diagram. Moreover, this map induces a bijection between the set of virtual knots and that of Gauss diagrams modulo Reidemeister moves I, II and III defined in the Gauss diagram level as shown in Figure 2.3 [7, Theorem 1.A]. Refer also to [9, Section 3.2]. Therefore a virtual knot can be regarded as the equivalence class of a Gauss diagram.

\begin{overpic}[width=341.43306pt]{Reid-Gauss.pdf} \put(34.0,175.0){I} \put(17.0,161.0){$\varepsilon$} \put(71.0,175.0){I} \put(105.5,161.0){$\varepsilon$} \put(204.0,175.0){II} \put(169.0,178.0){$\varepsilon$} \put(161.5,159.0){$-\varepsilon$} \put(278.5,175.0){II} \put(309.0,178.0){$\varepsilon$} \put(303.5,159.0){$-\varepsilon$} \put(71.8,101.0){III} \put(29.5,113.5){$\varepsilon$} \put(1.0,86.0){$-\varepsilon$} \put(47.0,86.0){$-\varepsilon$} \put(122.5,107.0){$\varepsilon$} \put(103.0,93.5){$-\varepsilon$} \put(131.0,93.5){$-\varepsilon$} \put(257.9,101.0){III} \put(215.0,113.5){$\varepsilon$} \put(200.0,88.0){$\varepsilon$} \put(229.0,88.0){$\varepsilon$} \put(309.0,107.0){$\varepsilon$} \put(293.0,88.0){$\varepsilon$} \put(322.5,88.0){$\varepsilon$} \put(71.8,26.5){III} \put(29.5,39.5){$\varepsilon$} \put(14.0,13.0){$\varepsilon$} \put(41.0,13.0){$-\varepsilon$} \put(122.5,33.0){$\varepsilon$} \put(107.0,13.0){$\varepsilon$} \put(135.0,13.0){$-\varepsilon$} \put(257.9,26.5){III} \put(215.0,39.5){$\varepsilon$} \put(193.0,13.0){$-\varepsilon$} \put(229.0,13.0){$\varepsilon$} \put(309.0,33.0){$\varepsilon$} \put(286.0,13.0){$-\varepsilon$} \put(322.5,13.0){$\varepsilon$} \end{overpic}
Figure 2.3. Reidemeister moves I, II and III on Gauss diagrams (ε=±1\varepsilon=\pm 1)

We will use two local deformations on Gauss diagrams as shown in Figure 2.4 as well as the Reidemeister moves I, II and III. These deformations are the counterparts of a 2k2k-move and a Ξ\Xi-move for Gauss diagrams. More precisely, a 2k2k-move on a Gauss diagram adds or removes 2k2k chords with the same sign ε\varepsilon whose initial and terminal endpoints appear alternatively. Let P1P_{1}, P2P_{2} and P3P_{3} be three consecutive endpoints of chords of a Gauss diagram. A Ξ\Xi-move exchanges the positions of P1P_{1} and P3P_{3} with preserving the signs ε1,ε2,ε3\varepsilon_{1},\varepsilon_{2},\varepsilon_{3} and orientations of the chords. In the right of the figure, a pair of dots \bullet marks the two endpoints P1P_{1} and P3P_{3} exchanged by a Ξ\Xi-move.

\begin{overpic}[width=341.43306pt]{2kXi-Gauss.pdf} \put(76.0,36.0){$2k$} \put(114.0,-12.0){$2k$ chords} \put(100.0,29.5){$\varepsilon$} \put(114.0,29.5){$\varepsilon$} \put(151.0,29.5){$\varepsilon$} \put(165.0,29.5){$\varepsilon$} \put(266.0,36.0){$\Xi$} \put(196.0,41.0){$\varepsilon_{1}$} \put(214.0,41.0){$\varepsilon_{2}$} \put(232.0,41.0){$\varepsilon_{3}$} \put(287.0,41.0){$\varepsilon_{1}$} \put(303.5,41.0){$\varepsilon_{2}$} \put(333.0,41.0){$\varepsilon_{3}$} \put(201.5,-5.0){$P_{1}$} \put(219.5,-5.0){$P_{2}$} \put(237.5,-5.0){$P_{3}$} \put(290.5,-5.0){$P_{3}$} \put(308.5,-5.0){$P_{2}$} \put(326.5,-5.0){$P_{1}$} \par\end{overpic}
Figure 2.4. A 2k2k-move and a Ξ\Xi-move on Gauss diagrams

Using Gauss diagrams, we now define the nn-writhe and the odd writhe of a virtual knot KK. For a Gauss diagram GG of KK, let γ\gamma be a chord of GG. If γ\gamma has a sign ε\varepsilon, then we assign ε\varepsilon and ε-\varepsilon to the terminal and initial endpoints of γ\gamma, respectively. The endpoints of γ\gamma divides the underlying circle of GG into two arcs. Let α\alpha be one of the two oriented arcs that starts at the initial endpoint of γ\gamma. See Figure 2.5. The index of γ\gamma, ind(γ)\mathrm{ind}(\gamma), is the sum of sings of endpoints of chords on α\alpha. For an integer nn, we denote by Jn(G)J_{n}(G) the sum of signs of chords with index nn. In [17, Lemma 2.3], Satoh and Taniguchi proved that Jn(G)J_{n}(G) is an invariant of the virtual knot KK for any n0n\neq 0; that is, it is independent of the choice of GG. This invariant is called the nn-writhe of KK and denoted by Jn(K)J_{n}(K). The odd writhe J(K)J(K) of KK, defined by Kauffman [10], is given by

J(K)=nJ2n1(K).J(K)=\sum_{n\in\mathbb{Z}}J_{2n-1}(K).

Refer to [3, 10, 17] for more details.

\begin{overpic}[width=56.9055pt]{arc.pdf} \put(15.0,26.0){$\gamma$} \put(30.0,26.0){$\varepsilon$} \put(60.0,26.0){$\alpha$} \put(24.0,60.0){$\varepsilon$} \put(20.0,-10.0){$-\varepsilon$} \end{overpic}
Figure 2.5. A chord γ\gamma with sign ε\varepsilon and its specified arc α\alpha

In [8], Jeong, Choi and Kim prepared Lemma 2.2 to show Theorem 2.3 giving the necessary condition mentioned in Section 1. We rephrase and reprove this lemma from the Gauss diagram point of view for the proof of Theorem 1.1.

Lemma 2.1 (cf. [8, Lemma 2.2]).

If two Gauss diagrams GG and GG^{\prime} are related by a single 2k2k-move, then there is a unique integer nn such that

Jn(G)Jn(G)=εk,Jn(G)Jn(G)=εk and Jm(G)=Jm(G)J_{n}(G)-J_{n}(G^{\prime})=\varepsilon k,\ J_{-n}(G)-J_{-n}(G^{\prime})=\varepsilon k\text{ and }J_{m}(G)=J_{m}(G^{\prime})

for some ε=±1\varepsilon=\pm 1 and any integer m±nm\neq\pm n.

Proof.

We may assume that GG^{\prime} is obtained from GG by removing 2k2k chords γ1\gamma_{1}, γ2,,γ2k\gamma_{2},\dots,\gamma_{2k} with sing ε\varepsilon involved in a 2k2k-move as shown in Figure 2.6, where we depict the signs of the initial and terminal endpoints of each γi\gamma_{i} (i=1,2,,2k)(i=1,2,\ldots,2k), instead of omitting the sign of γi\gamma_{i} itself.

\begin{overpic}[width=199.16928pt]{2k-Gauss.pdf} \put(99.0,24.0){$2k$} \put(39.0,-23.0){$G$} \put(157.0,-23.0){$G^{\prime}$} \put(3.0,18.0){$\gamma_{1}$} \put(17.5,18.0){$\gamma_{2}$} \put(73.0,18.0){$\gamma_{2k}$} \put(7.0,42.0){$-\varepsilon$} \put(27.0,42.0){$\varepsilon$} \put(49.0,42.0){$-\varepsilon$} \put(69.0,42.0){$\varepsilon$} \put(12.0,-9.0){$\varepsilon$} \put(21.0,-9.0){$-\varepsilon$} \put(54.5,-9.0){$\varepsilon$} \put(63.5,-9.0){$-\varepsilon$} \end{overpic}
Figure 2.6. GG^{\prime} is a result of a 2k2k-move on GG removing 2k2k chords

For any chord γ\gamma of GG other than the 2k2k chords γ1,,γ2k\gamma_{1},\ldots,\gamma_{2k}, let γ\gamma^{\prime} be the corresponding chord of GG^{\prime}. Then γ\gamma and γ\gamma^{\prime} have the same index; that is, ind(γ)=ind(γ)\mathrm{ind}(\gamma)=\mathrm{ind}(\gamma^{\prime}). In fact, the sum of signs of 2k2k consecutive endpoints of γi\gamma_{i}’s on an arc equals zero.

Let nn\in\mathbb{Z} (possibly zero) be the index of γ1\gamma_{1}. Then we have ind(γ2i1)=n\mathrm{ind}(\gamma_{2i-1})=n and ind(γ2i)=n\mathrm{ind}(\gamma_{2i})=-n for i=1,2,,ki=1,2,\dots,k. Moreover, the sum of signs of kk chords γ1,γ3,,γ2k1\gamma_{1},\gamma_{3},\ldots,\gamma_{2k-1} is equal to εk\varepsilon k, and the sum of signs of kk chords γ2,γ4,,γ2k\gamma_{2},\gamma_{4},\ldots,\gamma_{2k} is also εk\varepsilon k. Therefore we obtain the conclusion. ∎

Proof of Theorem 1.1.

Assume that KK and KK^{\prime} are related by a single 2k2k-move, and let GG and GG^{\prime} be Gauss diagrams of KK and KK^{\prime}, respectively.

Since GG and GG^{\prime} are related by a combination of a single 2k2k-move and Reidemeister moves, it follows from Lemma 2.1 that

Jn(K)Jn(K)=Jn(G)Jn(G){0,±k}J_{n}(K)-J_{n}(K^{\prime})=J_{n}(G)-J_{n}(G^{\prime})\in\{0,\pm k\}

for any nonzero integer nn. Therefore the assertion (i) holds.

If there is an odd integer nn such that Jn(K)Jn(K)=εkJ_{n}(K)-J_{n}(K^{\prime})=\varepsilon k holds for some ε=±1\varepsilon=\pm 1, then we have

Jn(K)Jn(K)=εk and Jm(K)=Jm(K)J_{-n}(K)-J_{-n}(K^{\prime})=\varepsilon k\text{ and }J_{m}(K)=J_{m}(K^{\prime})

for any nonzero integer m±nm\neq\pm n. Otherwise, we have Jm(K)=Jm(K)J_{m}(K)=J_{m}(K^{\prime}) for any odd integer mm. In both cases, it follows that J(K)J(K){0,±2k}J(K)-J(K^{\prime})\in\{0,\pm 2k\}. This completes the proof for the assertion (ii). ∎

Theorem 1.1 together with Theorem 1.2 implies an interesting consequence, which states that the set of 2k2k-move equivalence classes of a virtual knot KK for all k1k\geq 1 determines the Ξ\Xi-move equivalence class of KK.

Proposition 2.2.

If two virtual knots KK and KK^{\prime} are related by a finite sequence of 2k2k-moves for all k1k\geq 1, then KK and KK^{\prime} are related by a finite sequence of Ξ\Xi-moves.

Proof.

By assuming that KK and KK^{\prime} satisfy J(K)J(K)J(K)\neq J(K^{\prime}), there is a positive integer kk such that J(K)J(K)(mod2k)J(K)\not\equiv J(K^{\prime})\pmod{2k}. By Theorem 1.1(ii), this contradicts that KK and KK^{\prime} are related by a finite sequence of 2k2k-moves for all k1k\geq 1. Since we have J(K)=J(K)J(K)=J(K^{\prime}), Theorem 1.2 gives the conclusion. ∎

3. Proof of Theorem 1.3

This section is devoted to the proof of Theorem 1.3. Our main tool is the notion of shell-pairs, which are certain pairs of chords of a Gauss diagram developed in [13] for classifying 22-component virtual links up to Ξ\Xi-moves.

Let P1P_{1}, P2P_{2} and P3P_{3} be three consecutive endpoints of chords of a Gauss diagram GG. We say that a chord of GG is a shell if it connects P1P_{1} and P3P_{3}. See the left of Figure 3.1. Note that the orientation of a shell can be reversed by a Ξ\Xi-move exchanging the positions of P1P_{1} and P3P_{3}. A positive shell-pair (or negative shell-pair) consists of a pair of positive shells (or negative shells) whose four endpoints are consecutive. See the right of the figure, where we omit the orientations of shells.

\begin{overpic}[width=256.0748pt]{shell.pdf} \put(11.0,16.0){$\varepsilon$} \put(6.0,-12.0){$P_{1}$} \put(21.0,-12.0){$P_{2}$} \put(36.0,-12.0){$P_{3}$} \put(124.0,-12.0){positive} \put(205.0,-12.0){negative} \end{overpic}
Figure 3.1. A shell and a positive/negative shell-pair

We prepare three results (Lemmas 3.1, 3.2 and Proposition 3.3) to give the proof of Theorem 1.3. The first and second results will be used to prove the third one.

The following lemma was shown in [13, 17].

Lemma 3.1 ([13, Section 4], [17, Fig. 13]).

Let GG, GG^{\prime} and G′′G^{\prime\prime} be Gauss diagrams.

  1. (i)

    If GG^{\prime} is obtained from GG by a local deformation exchanging the positions of a shell-pair and an endpoint of a chord in GG with preserving the orientations of the chords as shown in the top of Figure 3.2, then GG and GG^{\prime} are related by a finite sequence of Ξ\Xi-moves and Reidemeister moves.

  2. (ii)

    If G′′G^{\prime\prime} is obtained from GG by a local deformation adding or removing two consecutive shell-pairs with opposite signs as shown in the bottom of Figure 3.2, then GG and G′′G^{\prime\prime} are related by a finite sequence of Ξ\Xi-moves and Reidemeister moves.

\begin{overpic}[width=227.62204pt]{shellpair-move.pdf} \put(13.5,74.0){$\varepsilon$} \put(46.0,74.0){$\varepsilon$} \put(134.0,74.0){$\varepsilon$} \put(166.0,74.0){$\varepsilon$} \put(125.0,17.0){$\varepsilon$} \put(157.0,17.0){$\varepsilon$} \put(172.0,17.0){$-\varepsilon$} \put(203.0,17.0){$-\varepsilon$} \end{overpic}
Figure 3.2. Local deformations in Lemma 3.1
Lemma 3.2.

Let GG and GG^{\prime} be Gauss diagrams and kk a positive integer. If GG^{\prime} is obtained from GG by a local deformation adding or removing kk consecutive shell-pairs with the same sign ε\varepsilon as shown in Figure 3.3, then GG and GG^{\prime} are related by a finite sequence of 2k2k-moves, Ξ\Xi-moves and Reidemeister moves.

\begin{overpic}[width=256.0748pt]{censec-shellpairs.pdf} \put(139.0,29.0){$\varepsilon$} \put(165.0,29.0){$\varepsilon$} \put(209.0,29.0){$\varepsilon$} \put(235.0,29.0){$\varepsilon$} \put(164.0,-12.0){$k$ shell-pairs} \end{overpic}
Figure 3.3. Adding or removing kk consecutive shell-pairs
Proof.

We only prove the result for k=2k=2. The other cases are shown similarly.

Assume that GG^{\prime} is obtained from GG by adding two consecutive shell-pairs with sign ε\varepsilon. The proof follows from Figure 3.4, which gives a sequence of Gauss diagrams

G=G0,G1,,G6=GG=G_{0},G_{1},\ldots,G_{6}=G^{\prime}

such that for each i=1,2,,6i=1,2,\ldots,6, GiG_{i} is obtained from Gi1G_{i-1} by a combination of 2k2k-moves, Ξ\Xi-moves and Reidemeister moves. More precisely, we obtain G1G_{1} from G0=GG_{0}=G by a Reidemeister move I adding a positive chord, G2G_{2} from G1G_{1} by a 44-move adding four chords with sign ε\varepsilon, and G3G_{3} from G2G_{2} by a Ξ\Xi-move exchanging the positions of the two endpoints with dots \bullet. By Lemma 3.1(i), we can move the resulting shell-pair (with preserving the orientations of the chords) to get G4G_{4} from G3G_{3}. After deforming G4G_{4} into G5G_{5} by a Ξ\Xi-move, we finally obtain G6=GG_{6}=G^{\prime} by two Ξ\Xi-moves reversing the orientations of shells and a Reidemeister move I removing a positive chord. ∎

\begin{overpic}[width=312.9803pt]{pf-lem-censecutive.pdf} \put(7.0,124.0){$G=G_{0}$} \put(102.0,124.0){$G_{1}$} \put(223.0,124.0){$G_{2}$} \put(80.0,56.0){$G_{3}$} \put(247.0,56.0){$G_{4}$} \put(89.0,-12.0){$G_{5}$} \put(243.0,-12.0){$G_{6}=G^{\prime}$} \put(63.0,156.0){I} \put(147.0,156.0){4} \put(5.5,84.0){$\Xi$} \put(149.5,84.0){Lem~{}\ref{lem-shellpair}} \put(5.5,19.0){$\Xi$} \put(177.5,19.0){$\Xi$, I} \put(216.0,183.0){$\varepsilon$} \put(216.0,174.0){$\varepsilon$} \put(216.0,166.0){$\varepsilon$} \put(216.0,157.0){$\varepsilon$} \par\put(56.0,85.0){$\varepsilon$} \put(82.0,85.0){$\varepsilon$} \put(75.0,111.0){$\varepsilon$} \put(75.0,102.0){$\varepsilon$} \put(205.0,85.0){$\varepsilon$} \put(231.0,85.0){$\varepsilon$} \put(267.0,85.0){$\varepsilon$} \put(267.0,94.0){$\varepsilon$} \put(38.5,21.0){$\varepsilon$} \put(64.5,21.0){$\varepsilon$} \put(86.0,21.0){$\varepsilon$} \put(112.0,21.0){$\varepsilon$} \put(222.0,21.0){$\varepsilon$} \put(248.0,21.0){$\varepsilon$} \put(269.5,21.0){$\varepsilon$} \put(295.5,21.0){$\varepsilon$} \end{overpic}
Figure 3.4. Proof of Lemma 3.2 for k=2k=2

For an integer aa, let G(a)G(a) be the Gauss diagram in Figure 3.5; that is, it consists of |a||a| shell-pairs with sign ε\varepsilon, where ε=1\varepsilon=1 for a>0a>0 and ε=1\varepsilon=-1 for a<0a<0. In particular, G(0)G(0) is the Gauss diagram with no chords. We denote by K(a)K(a) the virtual knot represented by G(a)G(a). We remark that J(K(a))=2aJ(K(a))=2a.

\begin{overpic}[width=170.71652pt]{normalform.pdf} \put(20.0,34.0){$\varepsilon$} \put(59.0,34.0){$\varepsilon$} \put(107.0,34.0){$\varepsilon$} \put(146.0,34.0){$\varepsilon$} \put(55.0,-12.0){$|a|$ shell-pairs} \end{overpic}
Figure 3.5. The Gauss diagram G(a)G(a)

We give a normal form of an equivalence class of virtual knots under 2k2k-moves and Ξ\Xi-moves as follows.

Proposition 3.3.

Any virtual knot KK is related to K(a)K(a) for some aa\in\mathbb{Z} with 0a<k0\leq a<k by a finite sequence of 2k2k-moves and Ξ\Xi-moves.

Proof.

By [17, Proposition 7.2], any Gauss diagram GG of KK can be deformed into G(a)G(a) for some aa\in\mathbb{Z} by a finite sequence of Ξ\Xi-moves and Reidemeister moves. If aa satisfies 0a<k0\leq a<k, then we have the conclusion.

For kak\leq a, there is a unique positive integer pp such that 0apk<k0\leq a-pk<k. Lemma 3.2 allows us to add pkpk consecutive negative shell-pairs to G(a)G(a). From the obtained Gauss diagram, we can remove pkpk pairs of shell-pairs with opposite signs by Lemma 3.1(ii) in order to obtain G(apk)G(a-pk). Therefore GG is related to G(apk)G(a-pk) by a finite sequence of 2k2k-moves, Ξ\Xi-moves and Reidemeister moves.

In the case a<0a<0, let qq be the positive integer such that 0a+qk<k0\leq a+qk<k. Using Lemmas 3.1(ii) and 3.2, we add qkqk consecutive positive shell-pairs to G(a)G(a), and then remove qkqk pairs of shell-pairs with opposite signs. Finally GG is related to G(a+qk)G(a+qk) by a finite sequence of 2k2k-moves, Ξ\Xi-moves and Reidemeister moves. ∎

Now we are ready to prove Theorem 1.3.

Proof of Theorem 1.3.

(i)\Rightarrow(ii): By Proposition 3.3, KK and KK^{\prime} are related to K(a)K(a) and K(a)K(a^{\prime}) for some a,aa,a^{\prime}\in\mathbb{Z} with 0a,a<k0\leq a,a^{\prime}<k, respectively, by a finite sequence of 2k2k-moves and Ξ\Xi-moves. Then it follows from Theorems 1.1(ii) and 1.2 that

J(K)J(K(a))=2a(mod2k)J(K)\equiv J(K(a))=2a\pmod{2k}

and

J(K)J(K(a))=2a(mod2k).J(K^{\prime})\equiv J(K(a^{\prime}))=2a^{\prime}\pmod{2k}.

By assumption, we have 2a2a(mod2k)2a\equiv 2a^{\prime}\pmod{2k}. Since the nonnegative integers aa and aa^{\prime} are less than kk, we have a=aa=a^{\prime}. Therefore K(a)K(a) and K(a)K(a^{\prime}) coincide.

(ii)\Rightarrow(i): This follows from Theorems 1.1(ii) and 1.2. ∎

The following result is an immediate consequence of the proof of Theorem 1.3.

Corollary 3.4.

A complete representative system of the equivalence classes of virtual knots under 2k2k-moves and Ξ\Xi-moves is given by the set

{K(a)a, 0a<k}.\{K(a)\mid a\in\mathbb{Z},\ 0\leq a<k\}.

In particular, the number of equivalence classes is kk. ∎

4. 2k2k-move distance

This section studies the 2k2k-move distance for virtual knots. For two virtual knots KK and KK^{\prime} that are related by a finite sequence of 2k2k-moves, we denote by d2k(K,K)\mathrm{d}_{2k}(K,K^{\prime}) the minimal number of 2k2k-moves needed to deform a diagram of KK into that of KK^{\prime}. In particular, we set u2k(K)=d2k(K,O)\mathrm{u}_{2k}(K)=\mathrm{d}_{2k}(K,O), where OO is the trivial knot. We will show that for any virtual knot KK and any positive integer aa, there is a virtual knot KK^{\prime} such that d2k(K,K)=a\mathrm{d}_{2k}(K,K^{\prime})=a (Proposition 4.2).

In [8, Theorem 2.3], Jeong, Choi and Kim gave a lower bound for d2k(K,K)\mathrm{d}_{2k}(K,K^{\prime}) using the affine index polynomials of KK and KK^{\prime}, which can be rephrased in terms of the nn-writhes as follows.

Theorem 4.1 (cf. [8, Theorem 2.3]).

Let KK and KK^{\prime} be virtual knots such that they are related by a finite sequence of 2k2k-moves. Then we have

d2k(K,K)1kn>0|Jn(K)Jn(K)|=1kn<0|Jn(K)Jn(K)|.\mathrm{d}_{2k}(K,K^{\prime})\geq\frac{1}{k}\sum_{n>0}|J_{n}(K)-J_{n}(K^{\prime})|=\frac{1}{k}\sum_{n<0}|J_{n}(K)-J_{n}(K^{\prime})|.

In particular, when K=OK^{\prime}=O is the trivial knot, we have

u2k(K)1kn>0|Jn(K)|=1kn<0|Jn(K)|.\mathrm{u}_{2k}(K)\geq\frac{1}{k}\sum_{n>0}|J_{n}(K)|=\frac{1}{k}\sum_{n<0}|J_{n}(K)|.

We remark that this theorem is a direct consequence of Lemma 2.1.

In [8, Example 2.4], Jeong, Choi and Kim demonstrated that the lower bound for u2k(K)\mathrm{u}_{2k}(K) in the theorem is sharp for some virtual knots KK. However, they did not make it clear whether for a pair of nontrivial virtual knots KK and KK^{\prime}, the lower bound for d2k(K,K)\mathrm{d}_{2k}(K,K^{\prime}) is sharp. We answer this by proving the following.

Proposition 4.2.

Let aa be a positive integer. For any virtual knot KK, there is a virtual knot KK^{\prime} such that d2k(K,K)=a\mathrm{d}_{2k}(K,K^{\prime})=a.

Proof.

Consider a long virtual knot diagram TT whose closure represents the virtual knot KK. Let KK^{\prime} be the virtual knot represented by the diagram DD in the left of Figure 4.1. The Gauss diagram GDG_{D} associated with DD is given in the right of the figure, where the boxed part depicts the Gauss diagram GTG_{T} corresponding to TT.

\begin{overpic}[width=312.9803pt]{pf-prop-distance.pdf} \put(52.0,65.0){$T$} \put(22.0,9.0){$2ak$ half-twists} \put(176.0,30.0){$G_{T}$} \put(234.0,-3.0){$2ak$ chords} \end{overpic}
Figure 4.1. A diagram DD of KK^{\prime} and its Gauss diagram GDG_{D}

Removing 2ak2ak half-twists from DD by 2k2k-moves aa times, we can deform DD into a diagram of KK. Therefore we have d2k(K,K)a\mathrm{d}_{2k}(K,K^{\prime})\leq a.

The 2ak2ak vertical chords in GDG_{D} consist of akak positive chords with index 11 and akak positive chords with index 1-1, and the remaining one chord of GDG_{D} excluding the chords in GTG_{T} has index 0. Hence it follows from [17, Lemma 4.3] that

Jn(K)={J1(K)+ak(n=1),J1(K)+ak(n=1),Jn(K)(n0,±1).J_{n}(K^{\prime})=\begin{cases}J_{1}(K)+ak&(n=1),\\ J_{-1}(K)+ak&(n=-1),\\ J_{n}(K)&(n\neq 0,\pm 1).\end{cases}

By Theorem 4.1, we have

d2k(K,K)1k|J1(K)J1(K)|=1k|ak|=a,\mathrm{d}_{2k}(K,K^{\prime})\geq\frac{1}{k}|J_{1}(K)-J_{1}(K^{\prime})|=\frac{1}{k}|-ak|=a,

which shows d2k(K,K)=a\mathrm{d}_{2k}(K,K^{\prime})=a. ∎

We remark that for any positive integer aa, there is a family of infinitely many virtual knots {Ks}s=1\{K_{s}\}_{s=1}^{\infty} such that u2k(Ks)=a\mathrm{u}_{2k}(K_{s})=a (s1)(s\geq 1). In fact, let KsK_{s} be the virtual knot represented by the diagram in [15, Figure 2.6] with m=akm=ak. Then by Theorem 4.1, it can be seen that these virtual knots KsK_{s}’s form such a family.

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