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Virtualized Delta, sharp, and pass moves for oriented virtual knots and links

Takuji NAKAMURA Faculty of Education, University of Yamanashi, Takeda 4-4-37, Kofu, Yamanashi, 400-8510, Japan [email protected] Yasutaka NAKANISHI Department of Mathematics, Kobe University, Rokkodai-cho 1-1, Nada-ku, Kobe 657-8501, Japan [email protected] Shin SATOH Department of Mathematics, Kobe University, Rokkodai-cho 1-1, Nada-ku, Kobe 657-8501, Japan [email protected]  and  Kodai Wada Department of Mathematics, Kobe University, Rokkodai-cho 1-1, Nada-ku, Kobe 657-8501, Japan [email protected]
Abstract.

We study virtualized Delta, sharp, and pass moves for oriented virtual links, and give necessary and sufficient conditions for two oriented virtual links to be related by the local moves. In particular, they are unknotting operations for oriented virtual knots. We provide lower bounds for the unknotting numbers and prove that they are best possible.

Key words and phrases:
virtual knot, virtual link, virtualized Δ\Delta-move, virtualized \sharp-move, virtualized pass-move, odd writhe, nn-writhe
2020 Mathematics Subject Classification:
57K12, 57K10
This work was supported by JSPS KAKENHI Grant Numbers JP20K03621, JP19K03492, JP22K03287, and JP23K12973.

1. Introduction

A local move is one of the main tools in classical knot theory which studies a relationship between topological and algebraic structures of classical knots and links in the 33-sphere. For example, the Δ\Delta-move corresponds to the set of linking numbers of classical links; that is, two classical links are related by a finite sequence of Δ\Delta-moves if and only if they have the same pairwise linking numbers. In particular, the Δ\Delta-move is an unknotting operation for classical knots.

On the other hand, it is known that the Δ\Delta-move is not an unknotting operation for virtual knots (cf. [7]). In our previous paper [5], we introduced a more elemental move called a virtualized Δ\Delta-move (or a vΔv\Delta-move simply) for unoriented virtual knots and links such that an ordinal Δ\Delta-move is decomposed into a pair of virtualized Δ\Delta-moves. See Figure 1.1. It has been shown in [5] that the virtualized Δ\Delta-move is an unknotting operation for unoriented virtual knots, and corresponds to the set of invariants called the parities for unoriented virtual links.

\begin{overpic}[width=227.62204pt]{vDelta-eps-converted-to.pdf} \put(63.0,26.0){$v\Delta$} \put(152.0,26.0){$v\Delta$} \end{overpic}
Figure 1.1. A virtualized Δ\Delta-move for an oriented virtual knot or link

In this paper, we study virtualized Δ\Delta-moves for oriented virtual knots and links, which are divided into two classes called vΔv\Delta^{\wedge}-moves and vΔv\Delta^{\circ}-moves according to the orientations of the strings involved in the moves. Furthermore we introduce a virtualized \sharp-move (or a vv\sharp-move) and a virtualized pass-move (or a vpvp-move) as elemental versions of an ordinal \sharp-move and an ordinal pass-move, respectively.

For X{vΔ,vΔ,vΔ,v,vp}X\in\{v\Delta,v\Delta^{\wedge},v\Delta^{\circ},v\sharp,vp\}, we say that two oriented virtual links are XX-equivalent if they are related by a finite sequence of XX-moves. Then we will prove the following by using the iith parity pi(L)/2p_{i}(L)\in{\mathbb{Z}}/2{\mathbb{Z}} and iith intersection number λi(L)\lambda_{i}(L)\in{\mathbb{Z}} of an oriented nn-component virtual link LL (i=1,,n)(i=1,\dots,n), which are invariants coming from the linking numbers of LL.

Theorem 1.1.

Let LL and LL^{\prime} be oriented nn-component virtual links with n2n\geq 2. Then the following are equivalent.

  1. (i)

    LL and LL^{\prime} are vΔv\Delta-equivalent.

  2. (ii)

    LL and LL^{\prime} are vΔv\Delta^{\wedge}-equivalent.

  3. (iii)

    LL and LL^{\prime} are vv\sharp-equivalent.

  4. (iv)

    pi(L)=pi(L)p_{i}(L)=p_{i}(L^{\prime}) holds for any i=1,,ni=1,\dots,n.

Theorem 1.2.

Let LL and LL^{\prime} be oriented nn-component virtual links with n2n\geq 2. Then the following are equivalent.

  1. (i)

    LL and LL^{\prime} are vΔv\Delta^{\circ}-equivalent.

  2. (ii)

    LL and LL^{\prime} are vpvp-equivalent.

  3. (iii)

    λi(L)=λi(L)\lambda_{i}(L)=\lambda_{i}(L^{\prime}) holds for any i=1,,ni=1,\dots,n.

For X{vΔ,vΔ,vΔ,v,vp}X\in\{v\Delta,v\Delta^{\wedge},v\Delta^{\circ},v\sharp,vp\}, we see that any two oriented virtual knots are XX-equivalent. In particular, the XX-move is an unknotting operation for oriented virtual knots. Therefore we can define the XX-unknotting number uX(K){\rm u}_{X}(K) of an oriented virtual knot KK, and will prove the following.

Theorem 1.3.

For any X{vΔ,vΔ,v,vp}X\in\{v\Delta^{\wedge},\ v\Delta^{\circ},\ v\sharp,\ vp\} and positive integer mm, there are infinitely many oriented virtual knots KK with uX(K)=m{\rm u}_{X}(K)=m.

This paper is organized as follows. In Section 2, we divide virtualized Δ\Delta-moves into eight types vΔ1,,vΔ4v\Delta_{1}^{\wedge},\dots,v\Delta_{4}^{\wedge} and vΔ1,,vΔ4v\Delta_{1}^{\circ},\dots,v\Delta_{4}^{\circ}, and virtualized \sharp-moves into two types v1v\sharp_{1} and v2v\sharp_{2} according to the orientations of strings. We study their relations and prove Theorem 1.1. Sections 3 and 4 are devoted to the proof of Theorem 1.2. In Section 3, we divide virtualized pass-moves into four types vp1,,vp4vp_{1},\dots,vp_{4} according to the string orientations. We study relations among vpivp_{i}’s and vΔjv\Delta_{j}^{\circ}’s, and prove the equivalence of (i) and (ii) in Theorem 1.2. In Section 4, we construct a family of oriented nn-component virtual links, and prove that any oriented nn-component virtual link LL is vΔv\Delta^{\circ}-equivalent to a certain link belonging to the family. We define invariants λi(L)\lambda_{i}(L) (i=1,,n)(i=1,\dots,n) by using the linking numbers of LL, and prove the equivalence of (i) and (iii) in Theorem 1.2. Finally, in Section 5, we provide lower bounds for the XX-distance between two oriented virtual knots for X{vΔ,vΔ,v,vp}X\in\{v\Delta^{\wedge},\ v\Delta^{\circ},\ v\sharp,\ vp\} in terms of their odd writhes and nn-writhes. By using these lower bounds, we prove Theorem 1.3.

2. Proof of Theorem 1.1

A virtualized Δ\Delta-move or simply a vΔv\Delta-move is a local deformation on a link diagram as shown in Figure 2.1. There are eight oriented types of virtualized Δ\Delta-moves labeled by vΔ1,,vΔ4v\Delta_{1}^{\wedge},\dots,v\Delta_{4}^{\wedge} and vΔ1,,vΔ4v\Delta_{1}^{\circ},\dots,v\Delta_{4}^{\circ} as in the figure. The first four moves are collectively called vΔv\Delta^{\wedge}-moves and the latter vΔv\Delta^{\circ}-moves. We say that two oriented virtual links LL and LL^{\prime} are vΔv\Delta-, vΔv\Delta^{\wedge}-, and vΔv\Delta^{\circ}-equivalent if their diagrams are related by a finite sequence of vΔv\Delta-, vΔv\Delta^{\wedge}-, and vΔv\Delta^{\circ}-moves (up to generalized Reidemeister moves), respectively.

\begin{overpic}[width=312.9803pt]{ori-vdelta-eps-converted-to.pdf} \put(59.5,203.0){$v\Delta_{1}^{\wedge}$} \put(235.0,203.0){$v\Delta_{2}^{\wedge}$} \put(59.5,144.5){$v\Delta_{3}^{\wedge}$} \put(235.0,144.5){$v\Delta_{4}^{\wedge}$} \put(59.5,86.0){$v\Delta_{1}^{\circ}$} \put(235.0,86.0){$v\Delta_{2}^{\circ}$} \put(59.5,27.5){$v\Delta_{3}^{\circ}$} \put(235.0,27.5){$v\Delta_{4}^{\circ}$} \end{overpic}
Figure 2.1. Virtualized Δ\Delta-moves
Lemma 2.1.

For any i{1,,4}i\in\{1,\dots,4\}, we have the following.

  1. (i)

    A crossing change is realized by a vΔiv\Delta_{i}^{\wedge}-move.

  2. (ii)

    A crossing change is realized by a vΔiv\Delta_{i}^{\circ}-move.

Proof.

(i) The sequence in the top row of Figure 2.2 shows that a crossing change is realized by a combination of a vΔ1v\Delta_{1}^{\wedge}-move and several generalized Reidemeister moves, where the symbol R\stackrel{{\scriptstyle\rm R}}{{\longleftrightarrow}} means a combination of generalized Reidemeister moves. For a vΔ2v\Delta_{2}^{\wedge}-move, we may use the above sequence with the orientations of all the strings reversed. See the second row of the figure. For vΔ3v\Delta_{3}^{\wedge}- and vΔ4v\Delta_{4}^{\wedge}-moves, we may use the sequences for vΔ1v\Delta_{1}^{\wedge}- and vΔ2v\Delta_{2}^{\wedge}-moves with opposite crossing information at every real crossing, respectively. See the third and bottom rows of the figure.

\begin{overpic}[width=312.9803pt]{pf-lem-cc-wedge-eps-converted-to.pdf} \put(0.0,245.5){\text@underline{$i=1$}} \put(0.0,179.5){\text@underline{$i=2$}} \put(0.0,113.5){\text@underline{$i=3$}} \put(0.0,47.5){\text@underline{$i=4$}} \put(39.0,217.6){R} \put(147.0,219.9){$v\Delta_{1}^{\wedge}$} \put(266.5,217.6){R} \put(39.0,151.6){R} \put(147.0,155.5){$v\Delta_{2}^{\wedge}$} \put(266.5,151.6){R} \put(39.0,85.6){R} \put(147.0,88.75){$v\Delta_{3}^{\wedge}$} \put(266.5,85.6){R} \put(39.0,19.6){R} \put(147.0,22.0){$v\Delta_{4}^{\wedge}$} \put(266.5,19.6){R} \end{overpic}
Figure 2.2. Proof of Lemma 2.1(i)

(ii) The sequence in Figure 2.3 shows that a crossing change is realized by a combination of a vΔ1v\Delta_{1}^{\circ}-move and several generalized Reidemeister moves. We remark that it is obtained from the sequence for a vΔ1v\Delta_{1}^{\wedge}-move given in (i) by reversing the orientation of the string pointed from the lower right to the upper left. We have a similar sequence for a vΔiv\Delta_{i}^{\circ}-move (i=2,3,4)(i=2,3,4) as shown in the figure. ∎

\begin{overpic}[width=312.9803pt]{pf-lem-cc-circ-eps-converted-to.pdf} \put(0.0,245.5){\text@underline{$i=1$}} \put(0.0,179.5){\text@underline{$i=2$}} \put(0.0,113.5){\text@underline{$i=3$}} \put(0.0,47.5){\text@underline{$i=4$}} \put(39.0,217.6){R} \put(147.0,219.9){$v\Delta_{1}^{\circ}$} \put(266.5,217.6){R} \put(39.0,151.6){R} \put(147.0,155.5){$v\Delta_{2}^{\circ}$} \put(266.5,151.6){R} \put(39.0,85.6){R} \put(147.0,88.75){$v\Delta_{3}^{\circ}$} \put(266.5,85.6){R} \put(39.0,19.6){R} \put(147.0,22.0){$v\Delta_{4}^{\circ}$} \put(266.5,19.6){R} \end{overpic}
Figure 2.3. Proof of Lemma 2.1(ii)

For two local moves XX and YY, we use the notation XYX\Rightarrow Y if a YY-move is realized by a combination of XX-moves and generalized Reidemeister moves.

Lemma 2.2.

For the local moves vΔiv\Delta_{i}^{\wedge} and vΔjv\Delta_{j}^{\circ} (i,j=1,,4)(i,j=1,\dots,4), we have the following.

  1. (i)

    vΔ1vΔ2vΔ3vΔ4v\Delta_{1}^{\wedge}\Leftrightarrow v\Delta_{2}^{\wedge}\Leftrightarrow v\Delta_{3}^{\wedge}\Leftrightarrow v\Delta_{4}^{\wedge}.

  2. (ii)

    vΔ1vΔ2vΔ3vΔ4v\Delta_{1}^{\circ}\Leftrightarrow v\Delta_{2}^{\circ}\Leftrightarrow v\Delta_{3}^{\circ}\Leftrightarrow v\Delta_{4}^{\circ}.

  3. (iii)

    vΔivΔjv\Delta_{i}^{\wedge}\Rightarrow v\Delta_{j}^{\circ} for any ii and jj.

Proof.

(i) It is sufficient to prove

vΔ1vΔ2vΔ4vΔ3vΔ1.v\Delta_{1}^{\wedge}\Rightarrow v\Delta_{2}^{\wedge}\Rightarrow v\Delta_{4}^{\wedge}\Rightarrow v\Delta_{3}^{\wedge}\Rightarrow v\Delta_{1}^{\wedge}.

The sequence in the top row of Figure 2.4 shows that a vΔ2v\Delta_{2}^{\wedge}-move is realized by a combination of a Δ\Delta-move, a vΔ1v\Delta_{1}^{\wedge}-move, and a generalized Reidemeister move. Since a Δ\Delta-move is realized by a combination of two crossing changes and a generalized Reidemeister move, and a crossing change is realized by a vΔ1v\Delta_{1}^{\wedge}-move by Lemma 2.1(i), we have vΔ1vΔ2v\Delta_{1}^{\wedge}\Rightarrow v\Delta_{2}^{\wedge}. The remaining cases are proved similarly as shown in the figure, where cc\stackrel{{\scriptstyle\rm cc}}{{\longleftrightarrow}} means a combination of crossing changes at real crossings.

\begin{overpic}[width=284.52756pt]{pf-lem-delta1-eps-converted-to.pdf} \put(0.0,249.0){\text@underline{$v\Delta_{1}^{\wedge}\Rightarrow v\Delta_{2}^{\wedge}$}} \put(0.0,181.4){\text@underline{$v\Delta_{2}^{\wedge}\Rightarrow v\Delta_{4}^{\wedge}$}} \put(0.0,113.8){\text@underline{$v\Delta_{4}^{\wedge}\Rightarrow v\Delta_{3}^{\wedge}$}} \put(0.0,46.2){\text@underline{$v\Delta_{3}^{\wedge}\Rightarrow v\Delta_{1}^{\wedge}$}} \put(57.6,224.8){$\Delta$} \put(133.0,227.3){$v\Delta_{1}^{\wedge}$} \put(219.0,224.8){R} \put(57.3,157.3){cc} \put(133.0,159.6){$v\Delta_{2}^{\wedge}$} \put(57.6,89.6){$\Delta$} \put(133.0,92.0){$v\Delta_{4}^{\wedge}$} \put(219.0,89.6){R} \put(57.6,22.0){cc} \put(133.0,24.5){$v\Delta_{3}^{\wedge}$} \end{overpic}
Figure 2.4. Proof of Lemma 2.2(i)

(ii) It is sufficient to prove

vΔ1vΔ2vΔ4vΔ3vΔ1.v\Delta_{1}^{\circ}\Rightarrow v\Delta_{2}^{\circ}\Rightarrow v\Delta_{4}^{\circ}\Rightarrow v\Delta_{3}^{\circ}\Rightarrow v\Delta_{1}^{\circ}.

Each of the implications can be proved by reversing the orientation of a certain string in a sequence given in (i). For example, Figure 2.5 shows vΔ1vΔ2v\Delta_{1}^{\circ}\Rightarrow v\Delta_{2}^{\circ}.

\begin{overpic}[width=284.52756pt]{pf-lem-delta2-eps-converted-to.pdf} \put(57.6,22.3){$\Delta$} \put(133.0,24.8){$v\Delta_{1}^{\circ}$} \put(219.0,22.3){R} \end{overpic}
Figure 2.5. Proof of vΔ1vΔ2v\Delta_{1}^{\circ}\Rightarrow v\Delta_{2}^{\circ}

(iii) By (i) and (ii), it is sufficient to prove vΔ2vΔ1v\Delta_{2}^{\wedge}\Rightarrow v\Delta_{1}^{\circ}. Figure 2.6 shows that a vΔ1v\Delta_{1}^{\circ}-move is realized by a combination of three crossing changes, three vΔ2v\Delta_{2}^{\wedge}-moves, and several generalized Reidemesiter moves. Therefore we have vΔ2vΔ1v\Delta_{2}^{\wedge}\Rightarrow v\Delta_{1}^{\circ} by Lemma 2.1(ii). ∎

\begin{overpic}[width=284.52756pt]{pf-lem-delta3-eps-converted-to.pdf} \put(61.3,125.8){R} \put(181.5,125.8){cc} \put(2.0,40.9){$v\Delta_{2}^{\wedge}$} \put(128.0,38.4){R} \end{overpic}
Figure 2.6. Proof of vΔ2vΔ1v\Delta_{2}^{\wedge}\Rightarrow v\Delta_{1}^{\circ}

A virtualized \sharp-move or simply a vv\sharp-move is a local deformation on a link diagram as shown in Figure 2.7. There are two types of virtualized \sharp-moves labeled by v1v\sharp_{1} and v2v\sharp_{2} according to the sign of the real crossings as in the figure. We say that two oriented virtual links LL and LL^{\prime} are vv\sharp-equivalent if their diagrams are related by a finite sequence of vv\sharp-moves (up to generalized Reidemeister moves).

\begin{overpic}[width=199.16928pt]{vsharp-eps-converted-to.pdf} \put(54.5,28.0){$v\sharp_{1}$} \put(132.5,28.0){$v\sharp_{2}$} \end{overpic}
Figure 2.7. Virtualized \sharp-moves
Lemma 2.3.

v1v2v\sharp_{1}\Leftrightarrow v\sharp_{2}. More precisely, a v2v\sharp_{2}-move is realized by a v1v\sharp_{1}-move, and vice versa.

Proof.

Figure 2.8 shows that a v2v\sharp_{2}-move is realized by a combination of a v1v\sharp_{1}-move and several generalized Reidemeister moves. Thus we have v1v2v\sharp_{1}\Rightarrow v\sharp_{2}. The proof of v2v1v\sharp_{2}\Rightarrow v\sharp_{1} is obtained from the above sequence by changing crossing information at every real crossing. ∎

\begin{overpic}[width=341.43306pt]{pf-lem-sharp-eps-converted-to.pdf} \put(43.0,22.3){R} \put(165.0,23.6){$v\sharp_{1}$} \put(293.0,22.3){R} \end{overpic}
Figure 2.8. Proof of v1v2v\sharp_{1}\Rightarrow v\sharp_{2}
Lemma 2.4.

For any i{1,2}i\in\{1,2\}, a crossing change is realized by a viv\sharp_{i}-move.

Proof.

The sequence in Figure 2.9 shows that a crossing change is realized by a combination of a v1v\sharp_{1}-move and several generalized Reidemeister moves. Therefore we have the conclusion by Lemma 2.3

\begin{overpic}[width=312.9803pt]{pf-lem-cc2-eps-converted-to.pdf} \put(39.0,30.3){R} \put(150.0,31.8){$v\sharp_{1}$} \put(266.5,30.3){R} \end{overpic}
Figure 2.9. Proof of Lemma 2.4 for i=1i=1
Lemma 2.5.

For any i{1,2}i\in\{1,2\} and j{1,,4}j\in\{1,\dots,4\}, we have vivΔjv\sharp_{i}\Leftrightarrow v\Delta_{j}^{\wedge}.

Proof.

()(\Rightarrow) By Lemmas 2.2(i) and 2.3, it is sufficient to prove v1vΔ1v\sharp_{1}\Rightarrow v\Delta_{1}^{\wedge}. The sequence in Figure 2.10 shows that a vΔ1v\Delta_{1}^{\wedge}-move is realized by a combination of a crossing change, a v1v\sharp_{1}-move, and several generalized Reidemeister moves. Therefore we have v1vΔ1v\sharp_{1}\Rightarrow v\Delta_{1}^{\wedge} by Lemma 2.4.

\begin{overpic}[width=341.43306pt]{pf-lem-delta-sharp1-eps-converted-to.pdf} \put(54.5,25.2){cc} \put(132.5,25.2){R} \put(203.0,26.7){$v\sharp_{1}$} \put(278.5,25.2){R} \end{overpic}
Figure 2.10. Proof of v1vΔ1v\sharp_{1}\Rightarrow v\Delta_{1}^{\wedge}

()(\Leftarrow) The sequence in Figure 2.11 shows that a v1v\sharp_{1}-move is realized by a combination of two crossing changes, a vΔ1v\Delta_{1}^{\wedge}-move, a vΔ4v\Delta_{4}^{\wedge}-move, and several generalized Reidemeister moves. Therefore we have vΔjviv\Delta_{j}^{\wedge}\Rightarrow v\sharp_{i} by Lemmas 2.1(i), 2.2(i), and 2.3. ∎

\begin{overpic}[width=355.65944pt]{pf-lem-delta-sharp2-eps-converted-to.pdf} \put(46.8,23.5){cc} \put(113.5,23.5){R} \put(201.0,25.9){$v\Delta_{1}^{\wedge}$} \put(201.0,6.7){$v\Delta_{4}^{\wedge}$} \put(300.5,23.5){R} \end{overpic}
Figure 2.11. A v1v\sharp_{1}-move is realized by vΔ1v\Delta_{1}^{\wedge}- and vΔ4v\Delta_{4}^{\wedge}-moves

We are ready to prove Theorem 1.1.

Proof of Theorem 1.1.

(i)\Leftrightarrow(ii). We have (i)\Rightarrow(ii) by Lemma 2.2(iii), and (ii)\Rightarrow(i) by definition.

(ii)\Leftrightarrow(iii). This follows from Lemma 2.5 immediately.

(i)\Leftrightarrow(iv). This has been proved in [5, Theorem 1.5]. ∎

3. Proof of the equivalence of (i) and (ii) in Theorem 1.2

A virtualized pass-move or simply a vp-move is a local move on a link diagram as shown in Figure 3.1. There are four types of virtualized pass-moves labeled by vp1,,vp4vp_{1},\dots,vp_{4} as in the figure. We say that two oriented virtual links LL and LL^{\prime} are vpvp-equivalent if their diagrams are related by a finite sequence of vpvp-moves (up to generalized Reidemeister moves).

\begin{overpic}[width=284.52756pt]{vpass-eps-converted-to.pdf} \put(54.5,97.5){$vp_{1}$} \put(216.5,97.5){$vp_{2}$} \put(95.5,28.0){$vp_{3}$} \put(174.0,28.0){$vp_{4}$} \end{overpic}
Figure 3.1. Virtualized pass-moves
Lemma 3.1.

For any ij{1,,4}i\neq j\in\{1,\dots,4\}, we have vpivpjvp_{i}\Leftrightarrow vp_{j}. More precisely, a vpivp_{i}-move is realized by a vpjvp_{j}-move.

Proof.

Figure 3.2 shows that a vpivp_{i}-move (i=2,3)(i=2,3) is realized by a combination of a vp1vp_{1}-move and several generalized Reidemeister moves. The other cases are proved similarly. ∎

\begin{overpic}[width=341.43306pt]{pf-lem-pass-eps-converted-to.pdf} \put(0.0,130.0){\text@underline{$vp_{1}\Rightarrow vp_{2}$}} \put(0.0,52.0){\text@underline{$vp_{1}\Rightarrow vp_{3}$}} \put(43.5,99.9){R} \put(122.5,101.4){$vp_{1}$} \put(208.5,99.9){R} \put(290.7,99.9){R} \put(43.5,21.5){R} \put(122.5,23.0){$vp_{1}$} \put(208.5,21.5){R} \put(290.7,21.5){R} \end{overpic}
Figure 3.2. A vpivp_{i}-move (i=2,3)(i=2,3) is realized by a vp1vp_{1}-move
Lemma 3.2.

For any i{1,,4}i\in\{1,\dots,4\}, a crossing change is realized by a vpivp_{i}-move.

Proof.

The sequence in Figure 3.3 shows that a crossing change is realized by a combination of a vp1vp_{1}-move and several generalized Reidemeister moves. Therefore we have the conclusion by Lemma 3.1. ∎

\begin{overpic}[width=312.9803pt]{pf-lem-cc3-eps-converted-to.pdf} \put(39.0,30.3){R} \put(150.0,31.8){$vp_{1}$} \put(266.5,30.3){R} \end{overpic}
Figure 3.3. Proof of Lemma 3.2 for i=1i=1
Lemma 3.3.

For any i,j{1,,4}i,j\in\{1,\dots,4\}, we have vpivΔjvp_{i}\Leftrightarrow v\Delta_{j}^{\circ}.

Proof.

()(\Rightarrow) By Lemmas 2.2(ii) and 3.1, it is sufficient to prove vp1vΔ1vp_{1}\Rightarrow v\Delta_{1}^{\circ}. The sequence in Figure 3.4 shows that a vΔ1v\Delta_{1}^{\circ}-move is realized by a combination of a crossing change, a vp1vp_{1}-move, and several generalized Reidemeister moves. Therefore we have vp1vΔ1vp_{1}\Rightarrow v\Delta_{1}^{\circ} by Lemma 3.2.

\begin{overpic}[width=341.43306pt]{pf-lem-delta-pass1-eps-converted-to.pdf} \put(54.5,25.2){cc} \put(132.5,25.2){R} \put(203.0,26.7){$vp_{1}$} \put(278.5,25.2){R} \end{overpic}
Figure 3.4. Proof of vp1vΔ1vp_{1}\Rightarrow v\Delta_{1}^{\circ}

()(\Leftarrow) The sequence in Figure 3.5 shows that a vp1vp_{1}-move is realized by a combination of two crossing changes, a vΔ1v\Delta_{1}^{\circ}-move, a vΔ3v\Delta_{3}^{\circ}-move, and several generalized Reidemeister moves. Therefore we have vΔjvpiv\Delta_{j}^{\circ}\Rightarrow vp_{i} by Lemmas 2.1(ii), 2.2(ii), and 3.1. ∎

\begin{overpic}[width=355.65944pt]{pf-lem-delta-pass2-eps-converted-to.pdf} \put(46.8,23.5){cc} \put(113.5,23.5){R} \put(201.0,25.9){$v\Delta_{1}^{\circ}$} \put(201.0,6.7){$v\Delta_{3}^{\circ}$} \put(300.5,23.5){R} \end{overpic}
Figure 3.5. A vp1vp_{1}-move is realized by vΔ1v\Delta_{1}^{\circ}- and vΔ3v\Delta_{3}^{\circ}-moves
Proof of (i)\Leftrightarrow(ii) in Theorem 1.2.

This follows from Lemma 3.3 immediately. ∎

4. Proof of the equivalence of (i) and (iii) in Theorem 1.2

A Gauss diagram of an oriented nn-component link diagram is a union of nn oriented circles regarded as the preimage of the immersed circles with chords connecting two points in the preimage of each real crossing. Each chord is equipped with the sign of the corresponding real crossing, and it is oriented from the overcrossing to the undercrossing.

A vΔiv\Delta_{i}^{\circ}-move (i=1,,4)(i=1,\dots,4) on a link diagram is described by deleting/adding three chords on a Gauss diagram as shown in Figure 4.1, where the signs of the chords are the same.

\begin{overpic}[width=312.9803pt]{vDelta-circ-Gauss-eps-converted-to.pdf} \put(63.0,96.3){$v\Delta_{1}^{\circ}$} \put(231.0,96.3){$v\Delta_{2}^{\circ}$} \put(63.0,27.2){$v\Delta_{3}^{\circ}$} \put(231.0,27.2){$v\Delta_{4}^{\circ}$} \end{overpic}
Figure 4.1. A vΔiv\Delta_{i}^{\circ}-move (i=1,,4)(i=1,\dots,4) on a Gauss diagram

A forbidden detour move [2, 8] or a fused move [1] on a link diagram is described by exchanging the positions of two consecutive initial and terminal endpoints of chords on a Gauss diagram. There are four types according to the signs of the chords, where we label them by FD1,,FD4FD_{1},\dots,FD_{4} as shown in Figure 4.2.

\begin{overpic}[width=312.9803pt]{fd-Gauss-eps-converted-to.pdf} \put(62.0,90.75){$FD_{1}$} \put(231.0,90.75){$FD_{2}$} \put(62.0,26.0){$FD_{3}$} \put(231.0,26.0){$FD_{4}$} \end{overpic}
Figure 4.2. Forbidden detour moves on Gauss diagrams
Lemma 4.1.

For any ij{1,,4}i\neq j\in\{1,\dots,4\}, we have FDiFDjFD_{i}\Leftrightarrow FD_{j}.

Proof.

It is sufficient to prove

FD1FD2FD4FD3FD1.FD_{1}\Rightarrow FD_{2}\Rightarrow FD_{4}\Rightarrow FD_{3}\Rightarrow FD_{1}.

The sequence in the top of Figure 4.3 shows FD1FD2FD_{1}\Rightarrow FD_{2} for ε=+1\varepsilon=+1 and FD4FD3FD_{4}\Rightarrow FD_{3} for ε=1\varepsilon=-1. We remark that two Reidemeister moves II appear in this sequence. Similarly, the sequence in the bottom of the figure shows FD3FD1FD_{3}\Rightarrow FD_{1} for ε=+1\varepsilon=+1 and FD2FD4FD_{2}\Rightarrow FD_{4} for ε=1\varepsilon=-1. ∎

\begin{overpic}[width=341.43306pt]{pf-lem-fd-eps-converted-to.pdf} \put(0.0,144.5){\text@underline{$FD_{1}\Rightarrow FD_{2}$ for $\varepsilon=+1$ and $FD_{4}\Rightarrow FD_{3}$ for $\varepsilon=-1$}} \put(160.5,122.0){$FD_{1}$} \put(155.0,113.0){\scriptsize{$(\varepsilon=+1)$}} \put(160.5,95.5){$FD_{4}$} \put(155.0,86.5){\scriptsize{$(\varepsilon=-1)$}} \put(72.3,112.0){R} \put(262.3,112.0){R} \put(7.0,104.0){$\varepsilon$} \put(43.5,104.0){$-\varepsilon$} \put(104.0,105.0){$\varepsilon$} \put(116.0,117.0){$-\varepsilon$} \put(129.0,98.0){$\varepsilon$} \put(139.5,98.0){$-\varepsilon$} \put(197.0,105.0){$\varepsilon$} \put(211.0,117.0){$-\varepsilon$} \put(218.5,98.0){$\varepsilon$} \put(235.5,98.0){$-\varepsilon$} \put(296.0,104.0){$\varepsilon$} \put(323.0,104.0){$-\varepsilon$} \put(0.0,55.0){\text@underline{$FD_{3}\Rightarrow FD_{1}$ for $\varepsilon=+1$ and $FD_{2}\Rightarrow FD_{4}$ for $\varepsilon=-1$}} \put(160.5,36.0){$FD_{3}$} \put(155.0,27.0){\scriptsize{$(\varepsilon=+1)$}} \put(160.5,9.4){$FD_{2}$} \put(155.0,0.4){\scriptsize{$(\varepsilon=-1)$}} \put(72.3,25.9){R} \put(262.3,25.9){R} \put(7.0,17.0){$\varepsilon$} \put(45.0,17.0){$\varepsilon$} \put(97.0,9.0){$\varepsilon$} \put(107.0,9.0){$-\varepsilon$} \put(121.0,27.0){$\varepsilon$} \put(135.0,17.0){$\varepsilon$} \put(193.5,9.0){$\varepsilon$} \put(208.5,9.0){$-\varepsilon$} \put(217.0,27.0){$\varepsilon$} \put(234.0,17.0){$\varepsilon$} \put(296.0,17.0){$\varepsilon$} \put(324.0,17.0){$\varepsilon$} \end{overpic}
Figure 4.3. Proof of Lemma 4.1
Lemma 4.2.

For any i,j{1,,4}i,j\in\{1,\dots,4\}, we have vΔiFDjv\Delta_{i}^{\circ}\Rightarrow FD_{j}.

Proof.

The sequence in Figure 4.4 shows that an FD1FD_{1}-move is realized by a combination of a vΔ4v\Delta_{4}^{\circ}-move, a vΔ3v\Delta_{3}^{\circ}-move, and two Reidemeister moves II. By Lemmas 2.2(ii) and 4.1, we have the conclusion. ∎

\begin{overpic}[width=284.52756pt]{pf-lem-delta-fd-eps-converted-to.pdf} \put(83.0,118.4){R} \put(188.5,120.9){$v\Delta_{4}^{\circ}$} \put(5.0,37.2){$v\Delta_{3}^{\circ}$} \put(120.5,34.6){R} \end{overpic}
Figure 4.4. An FD1FD_{1}-move is realized by a vΔ4v\Delta_{4}^{\circ}-move and a vΔ3v\Delta_{3}^{\circ}-move

A forbidden move [3] on a link diagram is described by exchanging the positions of two consecutive endpoints of chords on a Gauss diagram which are both initial or both terminal. There are six types according to the signs and orientations of the chords, where we label them by F1,,F6F_{1},\dots,F_{6} as shown in Figure 4.5. We say that two oriented virtual links LL and LL^{\prime} are FF-equivalent if their diagrams are related by a finite sequence of forbidden moves (up to generalized Reidemeister moves). We remark that any two oriented virtual knots are FF-equivalent [4, 6].

\begin{overpic}[width=312.9803pt]{forbidden-eps-converted-to.pdf} \put(67.5,156.0){$F_{1}$} \put(235.5,156.0){$F_{2}$} \put(67.5,91.0){$F_{3}$} \put(235.5,91.0){$F_{4}$} \put(67.5,26.0){$F_{5}$} \put(235.5,26.0){$F_{6}$} \end{overpic}
Figure 4.5. Forbidden moves
Lemma 4.3.

For any i{1,,4}i\in\{1,\dots,4\} and j{1,,6}j\in\{1,\dots,6\}, we have vΔiFjv\Delta_{i}^{\circ}\Rightarrow F_{j}.

Proof.

We first consider the case j=1j=1. The sequence in Figure 4.6 shows that an F1F_{1}-move is realized by a combination of two crossing changes and an FD2FD_{2}-move. Note that a crossing change at a real crossing on a link diagram is described by changing the sign and orientation of the corresponding chord on a Gauss diagram. Therefore we have vΔiF1v\Delta_{i}^{\circ}\Rightarrow F_{1} by Lemmas 2.1(ii) and 4.2 for any ii.

\begin{overpic}[width=341.43306pt]{pf-lem-delta-f-eps-converted-to.pdf} \put(71.0,25.5){cc} \put(160.5,27.0){$FD_{2}$} \put(261.5,25.5){cc} \end{overpic}
Figure 4.6. Proof of vΔiF1v\Delta_{i}^{\circ}\Rightarrow F_{1}

Similarly, an FjF_{j}-move for j{2,,6}j\in\{2,\dots,6\} is realized by a combination of two crossing changes and an FDkFD_{k}-move for some k{1,,4}k\in\{1,\ldots,4\}. Thus we have the conclusion by Lemmas 2.1(ii) and 4.2. ∎

In the remaining of this section, let nn be an integer with n2n\geq 2. For n1n-1 integers a2,,ana_{2},\dots,a_{n}, let H(a2,,an)=i=1nHiH(a_{2},\dots,a_{n})=\bigcup_{i=1}^{n}H_{i} be the Gauss diagram of an oriented nn-component virtual link such that

  1. (i)

    H(a2,,an)H(a_{2},\dots,a_{n}) has no self-chords,

  2. (ii)

    there are no nonself-chords between HiH_{i} and HjH_{j} (2i<jn2\leq i<j\leq n),

  3. (iii)

    if ai=0a_{i}=0, then there are no nonself-chords between H1H_{1} and HiH_{i},

  4. (iv)

    if ai>0a_{i}>0, then there are aia_{i} parallel nonself-chords oriented from H1H_{1} to HiH_{i} with positive signs,

  5. (v)

    if ai<0a_{i}<0, then there are ai-a_{i} parallel nonself-chords oriented from H1H_{1} to HiH_{i} with negative signs, and

  6. (vi)

    along H1H_{1} with respect to the orientation, we meet the endpoints of the chords between H1H_{1} and HiH_{i} before those between H1H_{1} and HjH_{j} (2i<jn)(2\leq i<j\leq n).

Figure 4.7 shows the Gauss diagram H(2,0,4,3)H(2,0,4,-3) with n=5n=5. Let M(a2,,an)M(a_{2},\dots,a_{n}) be the nn-component virtual link presented by H(a2,,an)H(a_{2},\dots,a_{n}).

\begin{overpic}[width=256.0748pt]{ex-H-eps-converted-to.pdf} \put(-14.8,66.9){$H_{1}$} \put(24.0,-12.0){$H_{2}$} \put(90.5,-12.0){$H_{3}$} \put(157.0,-12.0){$H_{4}$} \put(223.5,-12.0){$H_{5}$} \end{overpic}
Figure 4.7. The Gauss diagram H(2,0,4,3)H(2,0,4,-3)
Proposition 4.4.

Any oriented nn-component virtual link LL is vΔv\Delta^{\circ}-equivalent to M(a2,,an)M(a_{2},\dots,a_{n}) for some a2,,ana_{2},\dots,a_{n}\in{\mathbb{Z}}.

To prove this proposition, we prepare the following lemma.

Lemma 4.5.

Let G=i=1nGiG=\bigcup_{i=1}^{n}G_{i} be a Gauss diagram of an oriented nn-component virtual link. Then any nonself-chord oriented from GiG_{i} to GjG_{j} (2ijn)(2\leq i\neq j\leq n) with sign ε\varepsilon can be replaced with a pair of nonself-chords one of which is oriented from G1G_{1} to GiG_{i} with sign ε-\varepsilon and the other is from G1G_{1} to GjG_{j} with sign ε\varepsilon by a combination of vΔkv\Delta_{k}^{\circ}-moves and a Reidemeister move II for any k{1,,4}k\in\{1,\dots,4\}.

Proof.

The sequence in Figure 4.8 shows that a nonself-chord oriented from GiG_{i} to GjG_{j} with sign ε\varepsilon is replaced with a pair of nonself-chords one of which is oriented from G1G_{1} to GiG_{i} with sign ε-\varepsilon and the other is from G1G_{1} to GjG_{j} with sign ε\varepsilon by a combination of a vΔkv\Delta_{k}^{\circ}-move for some k{1,,4}k\in\{1,\dots,4\}, a crossing change, and a Reidemeister move II. Therefore we have the conclusion by Lemmas 2.1(ii) and 2.2(ii). ∎

\begin{overpic}[width=341.43306pt]{pf-lem-replacement-eps-converted-to.pdf} \put(66.5,27.0){$v\Delta_{k}^{\circ}$} \put(165.0,24.2){R} \put(262.0,24.2){cc} \put(23.5,34.3){$\varepsilon$} \put(-3.0,39.0){$G_{i}$} \put(42.5,39.0){$G_{j}$} \put(20.0,-9.9){$G_{1}$} \put(117.1,39.85){$\varepsilon$} \put(109.3,25.65){$-\varepsilon$} \put(92.2,10.35){$-\varepsilon$} \put(133.0,10.35){$-\varepsilon$} \put(90.5,39.0){$G_{i}$} \put(136.1,39.0){$G_{j}$} \put(114.6,-9.9){$G_{1}$} \put(188.3,14.56){$-\varepsilon$} \put(232.5,14.56){$-\varepsilon$} \put(189.8,39.0){$G_{i}$} \put(234.0,39.0){$G_{j}$} \put(213.0,-9.9){$G_{1}$} \put(286.0,14.56){$-\varepsilon$} \put(331.0,14.56){$\varepsilon$} \put(287.5,39.0){$G_{i}$} \put(332.0,39.0){$G_{j}$} \put(310.0,-9.9){$G_{1}$} \end{overpic}
Figure 4.8. Proof of Lemma 4.5
Proof of Proposition 4.4.

Let G=i=1nGiG=\bigcup_{i=1}^{n}G_{i} be a Gauss diagram of LL. Using forbidden (detour) moves and Reidemeister moves I, we can remove all the self-chords from GG. By Lemmas 4.2 and 4.3, we may assume that GG satisfies the condition (i) up to vΔiv\Delta_{i}^{\circ}-moves and Reidemeister moves.

If there is a nonself-chord between GiG_{i} and GjG_{j} (2ijn)(2\leq i\neq j\leq n), then we can replace it with a pair of chords between G1G_{1} and GiG_{i}, and G1G_{1} and GjG_{j} by Lemma 4.5. Hence we may assume that GG satisfies the conditions (i) and (ii) up to vΔiv\Delta_{i}^{\circ}-moves and Reidemeister moves.

Finally, GG can be deformed into the one satisfying the conditions (i)–(vi) by forbidden (detour) moves, crossing changes, and Reidemeister moves II. Therefore we have the conclusion by Lemmas 2.1(ii), 4.2, and 4.3. ∎

Let L=i=1nKiL=\bigcup_{i=1}^{n}K_{i} be an oriented nn-component virtual link, and G=i=1nGiG=\bigcup_{i=1}^{n}G_{i} a Gauss diagram of LL. The linking number of an ordered pair (Ki,Kj)(K_{i},K_{j}) is the sum of the signs of all the chords oriented from GiG_{i} to GjG_{j} (1ijn)(1\leq i\neq j\leq n), which is an invariant of LL (cf. [3, Section 1.7]). We denote it by Lk(Ki,Kj){\rm Lk}(K_{i},K_{j}).

For a chord γ\gamma of GG, it is convenient to introduce the signs of endpoints of γ\gamma as follows. If the sign of γ\gamma is ε\varepsilon, then we assign ε-\varepsilon and ε\varepsilon to the initial and terminal endpoints of γ\gamma, respectively. Then Lk(Ki,Kj)-{\rm Lk}(K_{i},K_{j}) is equal to the sum of the signs of all the endpoints of chords oriented from GiG_{i} to GjG_{j}.

The iith intersection number of LL, denoted by λi(L)\lambda_{i}(L), is defined by

λi(L)=1jinLk(Kj,Ki)1jinLk(Ki,Kj)\lambda_{i}(L)=\sum_{1\leq j\neq i\leq n}{\rm Lk}(K_{j},K_{i})-\sum_{1\leq j\neq i\leq n}{\rm Lk}(K_{i},K_{j})

for 1in1\leq i\leq n. Equivalently, λi(L)\lambda_{i}(L) is equal to the sum of the signs of all the endpoints of chords between GiG_{i} and GGiG\setminus G_{i}.

Lemma 4.6.

If two oriented nn-component virtual links LL and LL^{\prime} are vΔv\Delta^{\circ}-equivalent, then λi(L)=λi(L)\lambda_{i}(L)=\lambda_{i}(L^{\prime}) holds for any 1in1\leq i\leq n.

Proof.

Every pair of three chords appeared in a vΔiv\Delta_{i}^{\circ}-move has two adjacent endpoints with opposite signs ε\varepsilon and ε-\varepsilon. See Figure 4.9. ∎

\begin{overpic}[width=170.71652pt]{pf-lem-invariant-eps-converted-to.pdf} \put(77.0,29.0){$v\Delta_{i}^{\circ}$} \put(29.0,39.3){$\varepsilon$} \put(5.75,11.0){$\varepsilon$} \put(52.0,11.0){$\varepsilon$} \put(4.1,36.13){$\varepsilon$} \put(53.0,36.13){$-\varepsilon$} \put(-9.8,27.5){$-\varepsilon$} \put(60.8,27.5){$\varepsilon$} \put(21.0,-7.5){$\varepsilon$} \put(29.0,-7.5){$-\varepsilon$} \end{overpic}
Figure 4.9. Proof of Lemma 4.6
Lemma 4.7.

Let L=M(a2,,an)L=M(a_{2},\dots,a_{n}) be the oriented nn-component virtual link given in Proposition 4.4. Then we have

λi(L)={(a2++an)if i=1,aiif i=2,,n.\lambda_{i}(L)=\begin{cases}-(a_{2}+\dots+a_{n})&\text{if }i=1,\\ a_{i}&\text{if }i=2,\dots,n.\end{cases}
Proof.

This follows by definition immediately. ∎

For example, the virtual link L=M(2,0,4,3)L=M(2,0,4,-3) satisfies

λ1(L)=3,λ2(L)=2,λ3(L)=0,λ4(L)=4, and λ5(L)=3.\lambda_{1}(L)=-3,\ \lambda_{2}(L)=2,\ \lambda_{3}(L)=0,\ \lambda_{4}(L)=4,\text{ and }\lambda_{5}(L)=-3.
Proof of (i)\Leftrightarrow(iii) in Theorem 1.2.

(i)\Rightarrow(iii). This follows from Lemma 4.6.

(iii)\Rightarrow(i). By Proposition 4.4, LL and LL^{\prime} are vΔv\Delta^{\circ}-equivalent to

M(a2,,an) and M(a2,,an)M(a_{2},\dots,a_{n})\text{ and }M(a_{2}^{\prime},\dots,a_{n}^{\prime})

for some a2,,ana_{2},\dots,a_{n} and a2,,ana_{2}^{\prime},\dots,a_{n}^{\prime}\in{\mathbb{Z}}, respectively. It follows from Lemmas 4.6 and 4.7 that

ai=λi(L)=λi(L)=aia_{i}=\lambda_{i}(L)=\lambda_{i}(L^{\prime})=a_{i}^{\prime}

for any i=2,,ni=2,\dots,n. Since M(a2,,an)=M(a2,,an)M(a_{2},\dots,a_{n})=M(a_{2}^{\prime},\dots,a_{n}^{\prime}) holds, LL is vΔv\Delta^{\circ}-equivalent to LL^{\prime}. ∎

5. vΔv\Delta^{\wedge}-, vΔv\Delta^{\circ}-, vv\sharp-, and vpvp-unknotting numbers

In this section, we will consider the case of oriented virtual knots.

Lemma 5.1.

For every X{vΔ,vΔ,v,vp}X\in\{v\Delta^{\wedge},\ v\Delta^{\circ},\ v\sharp,\ vp\}, any two oriented virtual knots are XX-equivalent to each other. In particular, the XX-move is an unknotting operation for oriented virtual knots.

Proof.

By Lemmas 2.2(iii), 2.5, 3.3, and 4.3, we have the following.

vΔ1,,vΔ4v\Delta_{1}^{\wedge},\dots,v\Delta_{4}^{\wedge} \Rightarrow vΔ1,,vΔ4v\Delta_{1}^{\circ},\dots,v\Delta_{4}^{\circ} \Rightarrow F1,,F6F_{1},\dots,F_{6}
\Updownarrow \Updownarrow
vp1,,vp4vp_{1},\dots,vp_{4} v1,v2v\sharp_{1},v\sharp_{2}

Therefore we see that if two oriented virtual knots are FF-equivalent, then they are XX-equivalent for every X{vΔ,vΔ,v,vp}X\in\{v\Delta^{\wedge},\ v\Delta^{\circ},\ v\sharp,\ vp\}. Since any two oriented virtual knots are FF-equivalent [4, 6], they are XX-equivalent. ∎

For X{vΔ,vΔ,vΔ,v,vp}X\in\{v\Delta,v\Delta^{\wedge},\ v\Delta^{\circ},\ v\sharp,\ vp\} and two oriented virtual knots KK and KK^{\prime}, we denote by dX(K,K){\rm d}_{X}(K,K^{\prime}) the minimal number of XX-moves which are required to deform a diagram of KK into that of KK^{\prime}. It is called the XX-distance between KK and KK^{\prime}. In particular, we denote dX(K,O){\rm d}_{X}(K,O) by uX(K){\rm u}_{X}(K), and call it the XX-unknotting number of KK, where OO is the trivial knot.

We briefly review the nn-writhe Jn(K)J_{n}(K) and the odd writhe J(K)J(K) of an oriented virtual knot KK, which are invariants of KK (cf. [7]). Let GG be a Gauss diagram of KK, and γ\gamma a chord of GG. The endpoints of γ\gamma divide the underlying oriented circle of GG into two arcs. Let α\alpha be the one of the two arcs oriented from the initial endpoint of γ\gamma to the terminal. The index of γ\gamma is the sum of the signs of all the endpoints of chords on α\alpha, and denoted by Ind(γ){\rm Ind}(\gamma). For n0n\neq 0, the sum of the signs of all the chords with index nn is an invariant of KK. It is called the nn-writhe of KK, and denoted by Jn(K)J_{n}(K). Furthermore the odd writhe of KK is defined to be J(K)=n:oddJn(K)J(K)=\sum_{n{\rm:odd}}J_{n}(K).

Proposition 5.2.

For two oriented virtual knots KK and KK^{\prime}, we have the following.

  1. (i)

    dX(K,K)12|J(K)J(K)|{\rm d}_{X}(K,K^{\prime})\geq\frac{1}{2}|J(K)-J(K^{\prime})| for X{vΔ,vΔ,vp}X\in\{v\Delta^{\wedge},v\Delta^{\circ},vp\}.

  2. (ii)

    dv(K,K)14|J(K)J(K)|{\rm d}_{v\sharp}(K,K^{\prime})\geq\frac{1}{4}|J(K)-J(K^{\prime})|.

In particular, we have

uX(K)12|J(K)| for X{vΔ,vΔ,vp} and uv(K)14|J(K)|.{\rm u}_{X}(K)\geq\tfrac{1}{2}|J(K)|\text{ for }X\in\{v\Delta^{\wedge},v\Delta^{\circ},vp\}\text{ and }{\rm u}_{v\sharp}(K)\geq\tfrac{1}{4}|J(K)|.
Proof.

(i) For X{vΔ,vΔ}X\in\{v\Delta^{\wedge},v\Delta^{\circ}\}, if KK and KK^{\prime} are XX-equivalent, then they are vΔv\Delta-equivalent by definition. Thus we have dX(K,K)dvΔ(K,K){\rm d}_{X}(K,K^{\prime})\geq{\rm d}_{v\Delta}(K,K^{\prime}). Since it follows from [5, Proposition 2.6] that dvΔ(K,K)12|J(K)J(K)|{\rm d}_{v\Delta}(K,K^{\prime})\geq\frac{1}{2}|J(K)-J(K^{\prime})| holds, we have the inequality.

For X=vpX=vp, a vpvp-move contains two positive and two negative real crossings. Therefore a single vpvp-move changes the odd writhe by at most two.

(ii) Since a vv\sharp-move contains four real crossings, a single vv\sharp-move changes the odd writhe by at most four. ∎

Proposition 5.3.

For two oriented virtual knots KK and KK^{\prime}, we have the following.

  1. (i)

    dvΔ(K,K)13n0|Jn(K)Jn(K)|.{\rm d}_{v\Delta^{\circ}}(K,K^{\prime})\geq\frac{1}{3}\sum_{n\neq 0}|J_{n}(K)-J_{n}(K^{\prime})|.

  2. (ii)

    dvp(K,K)14n0|Jn(K)Jn(K)|.{\rm d}_{vp}(K,K^{\prime})\geq\frac{1}{4}\sum_{n\neq 0}|J_{n}(K)-J_{n}(K^{\prime})|.

In particular, we have uvΔ(K)13n0|Jn(K)| and uvp(K)14n0|Jn(K)|.{\rm u}_{v\Delta^{\circ}}(K)\geq\tfrac{1}{3}\sum_{n\neq 0}|J_{n}(K)|\text{ and }{\rm u}_{vp}(K)\geq\frac{1}{4}\sum_{n\neq 0}|J_{n}(K)|.

Proof.

(i) A vΔv\Delta^{\circ}-move does not change the index of any chord except for the three chords involved in the move. See Figure 4.9 again. Therefore if KK and KK^{\prime} are related by a single vΔv\Delta^{\circ}-move, then we have n0|Jn(K)Jn(K)|3\sum_{n\neq 0}|J_{n}(K)-J_{n}(K^{\prime})|\leq 3.

(ii) A vpvp-move does not change the index of any chord except for the four chords involved in the move. See Figure 5.1 as an example. Therefore if KK and KK^{\prime} are related by a single vpvp-move, then we have n0|Jn(K)Jn(K)|4\sum_{n\neq 0}|J_{n}(K)-J_{n}(K^{\prime})|\leq 4. ∎

\begin{overpic}[width=170.71652pt]{delta-pass-n-writhe-eps-converted-to.pdf} \put(81.0,43.0){$vp_{1}$} \end{overpic}
Figure 5.1. An example of a vpvp-move

Theorem 1.3 is decomposed into Theorems 5.45.7 as follows.

Theorem 5.4.

For any positive integer mm, there are infinitely many oriented virtual knots KK with uvΔ(K)=m{\rm u}_{v\Delta^{\wedge}}(K)=m.

Proof.

For an integer s2s\geq 2, we consider a long virtual knot TsT_{s} presented by a diagram as shown in the left of Figure 5.2, where the vertical twists consist of 2s2s positive real crossings and 2s12s-1 virtual crossings. By taking the closure of the product of mm copies of TsT_{s}, we obtain an oriented virtual knot Ks(m)K_{s}(m) as in the right of the figure.

\begin{overpic}[width=312.9803pt]{pf-thm-infinite-vdw-eps-converted-to.pdf} \put(74.0,127.0){\rotatebox{-90.0}{$4s-1$ crossings}} \put(42.5,6.5){$*$} \put(48.0,-13.0){$T_{s}$} \put(201.0,49.0){$m$ copies of $T_{s}$} \put(194.8,12.0){$T_{s}$} \put(265.0,12.0){$T_{s}$} \put(220.0,-13.0){$K_{s}(m)$} \end{overpic}
Figure 5.2. Diagrams of TsT_{s} and Ks(m)K_{s}(m)

As shown in the proof of [5, Theorem 2.9], the set {Ks(m)s2}\{K_{s}(m)\mid s\geq 2\} gives an infinite family of oriented virtual knots with uvΔ(Ks(m))=m{\rm u}_{v\Delta}(K_{s}(m))=m. Since the long knot diagram of TsT_{s} can be unknotted by a vΔv\Delta^{\wedge}-move for the three real crossings around the region with the mark *, we have uvΔ(Ks(m))=m{\rm u}_{v\Delta^{\wedge}}(K_{s}(m))=m. ∎

Theorem 5.5.

For any positive integer mm, there are infinitely many oriented virtual knots KK with uvΔ(K)=m{\rm u}_{v\Delta^{\circ}}(K)=m.

Proof.

For an integer s1s\geq 1, let TsT_{s} be a long virtual knot presented by a diagram as shown in the top of Figure 5.3. Then its Gauss diagram is shown in the bottom of the figure, and has 4s+34s+3 chords aia_{i} (i=1,2,,2s)(i=1,2,\ldots,2s), bjb_{j} (j=1,2,3)(j=1,2,3), and ckc_{k} (k=1,2,,2s)(k=1,2,\ldots,2s) with signs

ε(ai)=+1,ε(bj)=1, and ε(ck)=+1,\varepsilon(a_{i})=+1,\ \varepsilon(b_{j})=-1,\text{ and }\varepsilon(c_{k})=+1,

where ε(γ)\varepsilon(\gamma) denotes the sign of a chord γ\gamma. Let Ks(m)K_{s}(m) be an oriented virtual knot as the closure of the product of mm copies of TsT_{s}.

\begin{overpic}[width=312.9803pt]{pf-thm-infinite-vdc-eps-converted-to.pdf} \put(49.0,122.0){$a_{1}$} \put(107.0,122.0){$a_{2s}$} \put(219.0,122.0){$c_{1}$} \put(277.0,122.0){$c_{2s}$} \put(161.0,138.0){$b_{1}$} \put(171.0,172.0){$b_{2}$} \put(183.0,138.0){$b_{3}$} \put(18.0,22.0){$a_{1}$} \put(53.0,22.0){$a_{2s}$} \put(168.0,22.0){$c_{1}$} \put(202.0,22.0){$c_{2s}$} \put(115.0,69.0){$b_{2}$} \put(190.0,69.0){$b_{3}$} \put(154.0,85.0){$b_{1}$} \end{overpic}
Figure 5.3. A diagram of TsT_{s} and its Gauss diagram

We can apply a vΔv\Delta^{\circ}-move to the three real crossings b1b_{1}, b2b_{2}, and b3b_{3} on the long knot diagram so that TsT_{s} becomes unknotted. Thus we have uvΔ(Ks(m))m{\rm u}_{v\Delta^{\circ}}(K_{s}(m))\leq m.

To prove uvΔ(Ks(m))m{\rm u}_{v\Delta^{\circ}}(K_{s}(m))\geq m, we will calculate the nn-writhe of Ks(m)K_{s}(m) as follows. Since we have

Ind(ai)=Ind(ck)=0,Ind(b1)=4s, and Ind(b2)=Ind(b3)=2s,{\rm Ind}(a_{i})={\rm Ind}(c_{k})=0,\ {\rm Ind}(b_{1})=-4s,\text{ and }{\rm Ind}(b_{2})={\rm Ind}(b_{3})=2s,

it holds that

Jn(Ks(m))={2mif n=2s,mif n=4s,0otherwise.J_{n}(K_{s}(m))=\begin{cases}-2m&\text{if }n=2s,\\ -m&\text{if }n=-4s,\\ 0&\text{otherwise}.\end{cases}

By Proposition 5.3(i), we have uvΔ(Ks(m))13(2m+m)=m{\rm u}_{v\Delta^{\circ}}(K_{s}(m))\geq\frac{1}{3}(2m+m)=m, and hence uvΔ(Ks(m))=m{\rm u}_{v\Delta^{\circ}}(K_{s}(m))=m.

Furthermore for any s>ss>s^{\prime}, since

J2s(Ks(m))=2m0=J2s(Ks(m))J_{2s}(K_{s}(m))=-2m\neq 0=J_{2s}(K_{s^{\prime}}(m))

holds, we have Ks(m)Ks(m)K_{s}(m)\neq K_{s^{\prime}}(m). ∎

Theorem 5.6.

For any positive integer mm, there are infinitely many oriented virtual knots KK with uv(K)=m{\rm u}_{v\sharp}(K)=m.

Proof.

For an integer s3s\geq 3, let TsT_{s} be a long virtual knot presented by a diagram as shown in the top of Figure 5.4. Then its Gauss diagram is shown in the bottom of the figure, and has 2s+62s+6 chords aia_{i} (i=1,2,,2s)(i=1,2,\ldots,2s), bjb_{j} (j=1,2,3,4)(j=1,2,3,4), and ckc_{k} (k=1,2)(k=1,2) with signs

ε(ai)=ε(bj)=ε(c1)=+1, and ε(c2)=1.\varepsilon(a_{i})=\varepsilon(b_{j})=\varepsilon(c_{1})=+1,\text{ and }\varepsilon(c_{2})=-1.

Let Ks(m)K_{s}(m) be an oriented virtual knot as the closure of the product of mm copies of TsT_{s}.

\begin{overpic}[width=284.52756pt]{pf-thm-infinite-vs-eps-converted-to.pdf} \put(48.0,186.0){$c_{1}$} \put(112.0,186.0){$b_{1}$} \put(146.0,186.0){$b_{2}$} \put(164.0,186.0){$c_{2}$} \put(171.0,251.0){$a_{1}$} \put(117.0,251.0){$a_{2s}$} \put(112.0,214.0){$b_{3}$} \put(146.0,214.0){$b_{4}$} \put(103.0,75.0){$c_{1}$} \put(103.0,61.0){$c_{2}$} \put(146.0,128.0){$b_{1}$} \put(146.0,114.5){$b_{2}$} \put(146.0,101.5){$b_{3}$} \put(146.0,88.0){$b_{4}$} \put(68.0,20.0){$a_{1}$} \put(101.0,20.0){$a_{2s}$} \end{overpic}
Figure 5.4. A diagram of TsT_{s} and its Gauss diagram

We can apply a vv\sharp-move to b1b_{1}, b2b_{2}, b3b_{3}, and b4b_{4} so that TsT_{s} becomes unknotted. Thus we have uv(Ks(m))m{\rm u}_{v\sharp}(K_{s}(m))\leq m.

On the other hand, since we have

Ind(ai)=2{\rm Ind}(a_{i})=2,  Ind(b1)=Ind(b2)=Ind(c2)=1{\rm Ind}(b_{1})={\rm Ind}(b_{2})={\rm Ind}(c_{2})=1,
Ind(b3)=Ind(b4)=2s+1{\rm Ind}(b_{3})={\rm Ind}(b_{4})=-2s+1, and Ind(c1)=3{\rm Ind}(c_{1})=-3,

it holds that

Jn(Ks(m))={2msif n=2,mif n=1,3,2mif n=2s+1,0otherwise.J_{n}(K_{s}(m))=\begin{cases}2ms&\text{if }n=2,\\ m&\text{if }n=1,-3,\\ 2m&\text{if }n=-2s+1,\\ 0&\text{otherwise}.\end{cases}

This induces J(Ks(m))=m+m+2m=4mJ(K_{s}(m))=m+m+2m=4m. Therefore we have uv(Ks(m))m{\rm u}_{v\sharp}(K_{s}(m))\geq m by Proposition 5.2(ii), and hence uv(Ks(m))=m{\rm u}_{v\sharp}(K_{s}(m))=m.

Furthermore for any s>ss>s^{\prime}, since

J2s+1(Ks(m))=2m0=J2s+1(Ks(m))J_{-2s+1}(K_{s}(m))=2m\neq 0=J_{-2s+1}(K_{s^{\prime}}(m))

holds, we have Ks(m)Ks(m)K_{s}(m)\neq K_{s^{\prime}}(m). ∎

Theorem 5.7.

For any positive integer mm, there are infinitely many oriented virtual knots KK with uvp(K)=m{\rm u}_{vp}(K)=m.

Proof.

For an integer s1s\geq 1, let TsT_{s} be a long virtual knot presented by a diagram as shown in the top of Figure 5.5. Then its Gauss diagram is shown in the bottom of the figure, and has 4s+84s+8 chords aia_{i} (i=1,2,,2s)(i=1,2,\dots,2s), bjb_{j} (j=1,2,3,4)(j=1,2,3,4), ckc_{k} (k=1,2)(k=1,2), and dd_{\ell} (=1,2,,2s+2)(\ell=1,2,\dots,2s+2) with signs

ε(ai)=ε(b2)=ε(b4)=ε(ck)=ε(d)=+1 and ε(b1)=ε(b3)=1.\varepsilon(a_{i})=\varepsilon(b_{2})=\varepsilon(b_{4})=\varepsilon(c_{k})=\varepsilon(d_{\ell})=+1\text{ and }\varepsilon(b_{1})=\varepsilon(b_{3})=-1.

Let Ks(m)K_{s}(m) be an oriented virtual knot as the closure of the product of mm copies of TsT_{s}.

\begin{overpic}[width=341.43306pt]{pf-thm-infinite-vp-eps-converted-to.pdf} \put(86.0,181.5){$a_{1}$} \put(132.0,181.5){$a_{2s}$} \put(165.0,168.0){$b_{1}$} \put(196.0,168.0){$b_{2}$} \put(196.0,196.0){$b_{3}$} \put(165.0,196.0){$b_{4}$} \put(75.0,144.5){$c_{1}$} \put(99.0,144.5){$c_{2}$} \put(253.0,192.0){$d_{2s+2}$} \put(253.0,144.0){$d_{1}$} \put(5.0,17.0){$a_{1}$} \put(35.0,17.0){$a_{2s}$} \put(109.0,17.0){$c_{1}$} \put(136.0,17.0){$c_{2}$} \put(205.0,17.0){$d_{1}$} \put(235.0,17.0){$d_{2s+2}$} \put(185.0,69.0){$b_{1}$} \put(105.0,55.5){$b_{2}$} \put(205.0,55.5){$b_{3}$} \put(289.0,55.5){$b_{4}$} \end{overpic}
Figure 5.5. A diagram of TsT_{s} and its Gauss diagram

We can apply a vpvp-move to b1b_{1}, b2b_{2}, b3b_{3}, and b4b_{4} so that TsT_{s} becomes unknotted. Thus we have uvp(Ks(m))m{\rm u}_{vp}(K_{s}(m))\leq m.

On the other hand, since we have

Ind(ai)=Ind(ck)=Ind(d)=0,Ind(b1)=2s,Ind(b2)=Ind(b4)=2s+2, and Ind(b3)=2s+4,\begin{split}&{\rm Ind}(a_{i})={\rm Ind}(c_{k})={\rm Ind}(d_{\ell})=0,\ {\rm Ind}(b_{1})=2s,\\ &{\rm Ind}(b_{2})={\rm Ind}(b_{4})=2s+2,\text{ and }{\rm Ind}(b_{3})=2s+4,\end{split}

it holds that

Jn(Ks(m))={mif n=2s,2s+4,2mif n=2s+2,0otherwise.J_{n}(K_{s}(m))=\begin{cases}-m&\text{if }n=2s,2s+4,\\ 2m&\text{if }n=2s+2,\\ 0&\text{otherwise}.\end{cases}

Therefore we have uvp(Ks(m))14(m+m+2m)=m{\rm u}_{vp}(K_{s}(m))\geq\frac{1}{4}(m+m+2m)=m by Proposition 5.3(ii), and hence uvp(Ks(m))=m{\rm u}_{vp}(K_{s}(m))=m.

Furthermore for any s>ss>s^{\prime}, since

J2s+4(Ks(m))=m0=J2s+4(Ks(m))J_{2s+4}(K_{s}(m))=-m\neq 0=J_{2s+4}(K_{s^{\prime}}(m))

holds, we have Ks(m)Ks(m)K_{s}(m)\neq K_{s^{\prime}}(m). ∎

We remark that the oriented virtual knots K=Ks(m)K=K_{s}(m) constructed in the proof of Theorem 5.5 satisfy

uvΔ(K)>12|J(K)| and uvΔ(K)=13n0|Jn(K)|=m.{\rm u}_{v\Delta^{\circ}}(K)>\frac{1}{2}|J(K)|\text{ and }{\rm u}_{v\Delta^{\circ}}(K)=\frac{1}{3}\sum_{n\neq 0}|J_{n}(K)|=m.

In fact, we have J(K)=0J(K)=0. Generally the two lower bounds for uvΔ(K){\rm u}_{v\Delta^{\circ}}(K) given in Propositions 5.2(i) and 5.3(i) are independent in the following sense.

Proposition 5.8.

For any positive integer mm, there are infinitely many oriented virtual knots KK with

uvΔ(K)=12|J(K)|=m and uvΔ(K)>13n0|Jn(K)|.{\rm u}_{v\Delta^{\circ}}(K)=\frac{1}{2}|J(K)|=m\text{ and }{\rm u}_{v\Delta^{\circ}}(K)>\frac{1}{3}\sum_{n\neq 0}|J_{n}(K)|.
Proof.

For an integer s1s\geq 1, let TsT_{s} be a long virtual knot presented by a diagram as shown in the top of Figure 5.6. Then its Gauss diagram is shown in the bottom of the figure, and has 2s+42s+4 positive chords aia_{i} (i=1,2,,2s1)(i=1,2,\ldots,2s-1), bjb_{j} (j=1,2,3)(j=1,2,3), and ckc_{k} (k=1,2)(k=1,2). Let Ks(m)K_{s}(m) be an oriented virtual knot as the closure of the product of mm copies of TsT_{s}.

\begin{overpic}[width=284.52756pt]{ex-infinite-vdc2-eps-converted-to.pdf} \put(96.0,166.0){$b_{1}$} \put(135.5,166.0){$b_{2}$} \put(115.5,190.0){$b_{3}$} \put(190.0,193.0){$a_{1}$} \put(189.0,248.0){{\small$a_{2s-1}$}} \put(117.0,247.0){$c_{1}$} \put(117.0,262.0){$c_{2}$} \put(100.0,105.0){$b_{1}$} \put(59.0,91.0){$b_{2}$} \put(135.0,91.0){$b_{3}$} \put(39.0,22.0){$a_{1}$} \put(71.5,22.0){$a_{2s-1}$} \put(122.0,22.0){$c_{1}$} \put(136.5,22.0){$c_{2}$} \end{overpic}
Figure 5.6. A diagram of TsT_{s} and its Gauss diagram

We can apply a vΔv\Delta^{\circ}-move to b1b_{1}, b2b_{2}, and b3b_{3} so that TsT_{s} becomes unknotted. Thus we have uvΔ(Ks(m))m{\rm u}_{v\Delta^{\circ}}(K_{s}(m))\leq m.

On the other hand, since we have

Ind(ai)=Ind(ck)=Ind(b3)=0,Ind(b1)=2s1,and Ind(b2)=2s+1,{\rm Ind}(a_{i})={\rm Ind}(c_{k})={\rm Ind}(b_{3})=0,\ {\rm Ind}(b_{1})=2s-1,\ \text{and }{\rm Ind}(b_{2})=-2s+1,

it holds that

Jn(Ks(m))={mif n=2s1,2s+1,0otherwise.J_{n}(K_{s}(m))=\begin{cases}m&\text{if }n=2s-1,-2s+1,\\ 0&\text{otherwise}.\end{cases}

This induces J(Ks(m))=m+m=2mJ(K_{s}(m))=m+m=2m. By Propositions 5.2(i) and 5.3(i), we have

uvΔ(Ks(m))=12|J(Ks(m))|=m and uvΔ(Ks(m))>13n0|Jn(Ks(m))|=23m.\begin{split}&{\rm u}_{v\Delta^{\circ}}(K_{s}(m))=\frac{1}{2}|J(K_{s}(m))|=m\text{ and }\\ &{\rm u}_{v\Delta^{\circ}}(K_{s}(m))>\frac{1}{3}\sum_{n\neq 0}|J_{n}(K_{s}(m))|=\dfrac{2}{3}m.\end{split}

Furthermore for any s>ss>s^{\prime}, since

J2s1(Ks(m))=m0=J2s1(Ks(m))J_{2s-1}(K_{s}(m))=m\neq 0=J_{2s-1}(K_{s^{\prime}}(m))

holds, we have Ks(m)Ks(m)K_{s}(m)\neq K_{s^{\prime}}(m). ∎

Similarly to the case above, the oriented virtual knots K=Ks(m)K=K_{s}(m) constructed in the proof of Theorem 5.7 satisfy

uvp(K)>12|J(K)| and uvp(K)=14n0|Jn(K)|=m.{\rm u}_{vp}(K)>\frac{1}{2}|J(K)|\text{ and }{\rm u}_{vp}(K)=\frac{1}{4}\sum_{n\neq 0}|J_{n}(K)|=m.

In fact, we have J(K)=0J(K)=0. Generally the two lower bounds for uvp(K){\rm u}_{vp}(K) given in Propositions 5.2(i) and 5.3(ii) are independent in the following sense.

Proposition 5.9.

For any positive integer mm, there are infinitely many oriented virtual knots KK with

uvp(K)=12|J(K)|=m and uvp(K)>14n0|Jn(K)|.{\rm u}_{vp}(K)=\frac{1}{2}|J(K)|=m\text{ and }{\rm u}_{vp}(K)>\frac{1}{4}\sum_{n\neq 0}|J_{n}(K)|.
Proof.

For an integer s2s\geq 2, let TsT_{s} be a long virtual knot presented by a diagram as shown in the top of Figure 5.7. Then its Gauss diagram is shown in the bottom of the figure, and has 2s+52s+5 chords aia_{i} (i=1,2,,2s)(i=1,2,\ldots,2s), bjb_{j} (j=1,2,3,4)(j=1,2,3,4), and cc with signs

ε(ai)=ε(b1)=ε(b3)=ε(c)=+1 and ε(b2)=ε(b4)=1.\varepsilon(a_{i})=\varepsilon(b_{1})=\varepsilon(b_{3})=\varepsilon(c)=+1\text{ and }\varepsilon(b_{2})=\varepsilon(b_{4})=-1.

Let Ks(m)K_{s}(m) be an oriented virtual knot as the closure of the product of mm copies of TsT_{s}.

\begin{overpic}[width=256.0748pt]{ex-infinite-vp2-eps-converted-to.pdf} \put(51.0,127.0){$b_{1}$} \put(82.0,127.0){$b_{2}$} \put(82.0,153.0){$b_{3}$} \put(51.0,153.0){$b_{4}$} \put(71.0,181.0){$c$} \put(123.0,127.0){$a_{1}$} \put(171.0,127.0){$a_{2s}$} \put(95.0,83.0){$b_{1}$} \put(55.0,69.5){$b_{2}$} \put(116.0,69.5){$b_{3}$} \put(157.5,69.5){$b_{4}$} \put(38.0,18.0){$a_{1}$} \put(69.0,18.0){$a_{2s}$} \put(111.0,18.0){$c$} \end{overpic}
Figure 5.7. A diagram of TsT_{s} and its Gauss diagram

We can apply a vpvp-move to b1b_{1}, b2b_{2}, b3b_{3}, and b4b_{4} so that TsT_{s} becomes unknotted. Thus we have uvp(Ks(m))m{\rm u}_{vp}(K_{s}(m))\leq m.

On the other hand, since we have

Ind(ai)=Ind(c)=Ind(b4)=0,Ind(b1)=2s1,Ind(b2)=2s,and Ind(b3)=1,{\rm Ind}(a_{i})={\rm Ind}(c)={\rm Ind}(b_{4})=0,\ {\rm Ind}(b_{1})=2s-1,\ {\rm Ind}(b_{2})=2s,\text{and }{\rm Ind}(b_{3})=1,

it holds that

Jn(Ks(m))={mif n=1,2s1,mif n=2s,0otherwise.J_{n}(K_{s}(m))=\begin{cases}m&\text{if }n=1,2s-1,\\ -m&\text{if }n=2s,\\ 0&\text{otherwise}.\end{cases}

This induces J(Ks(m))=m+m=2mJ(K_{s}(m))=m+m=2m. By Propositions 5.2(i) and 5.3(ii), we have

uvp(Ks(m))=12|J(Ks(m))|=m and uvp(Ks(m))>14n0|Jn(Ks(m))|=34m.\begin{split}&{\rm u}_{vp}(K_{s}(m))=\frac{1}{2}|J(K_{s}(m))|=m\text{ and }\\ &{\rm u}_{vp}(K_{s}(m))>\frac{1}{4}\sum_{n\neq 0}|J_{n}(K_{s}(m))|=\frac{3}{4}m.\end{split}

Furthermore for any sss\neq s^{\prime}, since

J2s(Ks(m))=m0=J2s(Ks(m))J_{2s}(K_{s}(m))=-m\neq 0=J_{2s}(K_{s^{\prime}}(m))

holds, we have Ks(m)Ks(m)K_{s}(m)\neq K_{s^{\prime}}(m). ∎

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