Alexander polynomials of simple-ribbon knots
Kengo Kishimoto, Tetsuo Shibuya, Tatsuya Tsukamoto, and Tsuneo, Ishikawa

TL;DR
This paper derives a formula for Alexander polynomials of simple-ribbon knots, enabling identification of such knots among 10-crossing knots and exploring their fusion properties.
Contribution
It provides a new formula for Alexander polynomials of simple-ribbon knots and characterizes their fusion structures, advancing understanding of ribbon knot classifications.
Findings
Formula for Alexander polynomials of simple-ribbon knots
Criterion to identify 10-crossing simple-ribbon knots
Conditions for knots to be both m- and n-simple-ribbon knots
Abstract
In a previous paper, we introduced special types of fusions, so called simple-ribbon fusions on links. A knot obtained from the trivial knot by a finite sequence of simple-ribbon fusions is called a simple-ribbon knot. Every ribbon knot with <10 crossings is a simple-ribbon knot. In this paper, we give a formula for the Alexander polynomials of simple-ribbon knots. Using the formula, we determine if a knot with 10 crossings is a simple-ribbon knot. Every simple-ribbon fusion can be realized by ``elementary" simple-ribbon fusions. We call a knot a p-simple-ribbon knot if the knot is obtained from the trivial knot by a finite sequence of elementary p-simple-ribbon fusions for a fixed positive integer p. We provide a condition for a simple-ribbon knot to be both of an m-simple-ribbon knot and an n-simple-ribbon knot for positive integers m and n.
| simple-ribbon | det(K) | ||||
|---|---|---|---|---|---|
| 0 | 9 | ||||
| 5 | 25 | ||||
| 7 | 25 | ||||
| 9 | 9 | ||||
| 5 | 49 | ||||
| 7 | 49 | ||||
| 0 | 9 | ||||
| 1 | 25 | ||||
| 11 | 49 | ||||
| 1 | 49 | ||||
| 9 | 81 | ||||
| 91 | 49 | ||||
| 9 | 81 | ||||
| 0 | 81 | ||||
| 81 | 81 | ||||
| 1 | 121 | ||||
| 5 | 25 | ||||
| 1 | 25 | ||||
| 9 | 9 | ||||
| 35 | 1 | ||||
| 7 | 25 | ||||
| 9 | 9 | ||||
| 1 | 25 | ||||
| 121 | 25 | ||||
| 1 | 49 |
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Alexander polynomials of simple-ribbon knots
Kengo Kishimoto, Tetsuo Shibuya, Tatsuya Tsukamoto, and Tsuneo Ishikawa
2010 Mathematics Subject Classification. 57M25
This work was supported by JSPS KAKENHI Grant Number JP16K05162.
Abstract
This is a revised version of [6]. We revised the diagrams of , in Figure 3, and the values of of for , and the value of of for in Table 1. In [4], we introduced special types of fusions, so called simple-ribbon fusions on links. A knot obtained from the trivial knot by a finite sequence of simple-ribbon fusions is called a simple-ribbon knot. Every ribbon knot with crossings is a simple-ribbon knot. In this paper, we give a formula for the Alexander polynomials of simple-ribbon knots. Using the formula, we determine if a knot with crossings is a simple-ribbon knot. Every simple-ribbon fusion can be realized by “elementary” simple-ribbon fusions. We call a knot an -simple-ribbon knot if the knot is obtained from the trivial knot by a finite sequence of elementary -simple-ribbon fusions for a fixed positive integer . We provide a condition for a simple-ribbon knot to be both of an -simple-ribbon knot and an -simple-ribbon knot for positive integers and .
1. Introduction
Knots and links are assumed to be ordered and oriented, and they are considered up to ambient isotopy in an oriented -sphere . In [4], we introduced special types of fusions, so called simple-ribbon fusions. A (-)ribbon fusion on a link is an -fusion ([3, Definition 13.1.1]) on the split union of and an -component trivial link such that each component of is attached to a component of by a single band. Note that any knot obtained from the trivial knot by a finite sequence of ribbon fusions is a ribbon knot ([3, Definition 13.1.9]), and that any ribbon knot can be obtained from the trivial knot by ribbon fusions. Here we only define an elementary simple-ribbon fusion. A general simple-ribbon fusion can be realized by elementary simple-ribbon fusions. Refer [4] for precise definition.
Let be a link and the -component trivial link which is split from . Let be a disjoint union of non-singular disks with and (), and let be a disjoint union of disks for an -fusion, called bands, on the split union of and satisfying the following (see Figure 1 for example):
- (i)
a single arc ;
- (ii)
a single arc ; and
- (iii)
a single arc of ribbon type .
Let be a link obtained from the split union of and by the -fusion along , i.e., . Then we say that is obtained from by an elementary (-)simple-ribbon fusion or an elementary (-)SR-fusion (with respect to ). If a knot is obtained from the trivial knot by a finite sequence of elementary SR-fusions, then we call a simple-ribbon knot (or an SR-knot). Since an elementary SR-fusion is a ribbon fusion, any SR-knot is a ribbon knot. We also call the trivial knot an SR-knot. As illustrated in Figure 1, all the ribbon knots with crossings are SR-knots.
Let and be disks and an immersion such that and . We denote the arc of by and let and be the subdisks of such that , , and . Take a point on (, , ) and an arc on so that and oriented from to (see Figure 2). Then is an oriented simple loop and we call an attendant knot of . Moreover, we denote the pre-images of (resp. ) on and by and (resp. and ), respectively.
is oriented so that induced orientations on boundaries are compatible with the orientation of . Then we can see that each band intersects with in two ways, i.e. when we pass through from to , we pass through either from the negative side to the positive side of , or from the positive side to the negative side of . In the former and latter cases, we say that is positive and negative, respectively. Then we have the following.
Theorem 1.1**.**
Let be a knot obtained from a knot by an elementary -SR-fusion with an attendant knot and with positive bands. Let and . Then we have the following.
[TABLE]
Remark. We can also write as , i.e.
[TABLE]
Corollary 1.2**.**
Let be a knot obtained from a knot by a finite sequence of elementary SR-fusions, i.e., there exists a finite sequence , , , of knots such that is obtained from by an elementary -SR-fusion with an attendant knot and with positive bands . Let and . Then we have the following.
[TABLE]
As mentioned in the beginning, all the ribbon knots with crossings are SR-knots. Using Corollary 1.2, we can determine if a ribbon knot with crossings is an SR-knot. To do this, we use a value derived from the Alexander polynomial. For a knot , let be the polynomial such that and . Then define as [math] if and as the largest odd factor of if . Note that if is a simple-ribbon knot, then is a product of the integers of the form from Corollary 1.2.
Lemma 1.3**.**
If is a simple-ribbon knot such that , then we have the following for a non-negative integer .
[TABLE]
Proof.
Since is a simple-ribbon knot, we have the following from Corollary 1.2, where , , , and are integers .
Let and . Then we have that for an integer . Since , each of and is a power of , and thus , , or (). Thus, each of and is , [math], or for each , and hence is or , since . Therefore we have that , , or . In the first two cases and the last case, we have that and , respectively. Hence we obtain the conclusion. ∎
Proposition 1.4**.**
Among the ribbon knots with crossings, , , , , , , , , and are simple-ribbon knots and , , , , , , and are not.
Proof.
The former statement is from Figure 3. To show the latter statement, we consider for each knot. Since , , and from Table 1 and none of , , , and is for a non-negative integer , we know that these knots are not simple-ribbon knots. For the other knots, we have that , and the following from Table 1. Hence we know that they are not simple-ribbon knots from Lemma 1.3.
,
∎
Note that the above proof of Proposition 1.4 implies that for any ribbon knot with crossings, if can be written as equation (1.3), then is a simple-ribbon knot. However, it does not hold in general.
Theorem 1.5**.**
For any polynomial , there exists a ribbon knot whose Alexander polynomial is and which is not a simple-ribbon knot.
If an SR-knot is obtained from the trivial knot by a finite sequence of elementary -SR-fusions for a fixed positive integer , then we call the SR-knot -SR-knot. For example, is a -SR-knot and is a -SR-knot and also a -SR-knot as we can see in Figure 1. It is natural to ask if there exists a simple-ribbon knot which is an -SR-knot and also an -SR-knot for distinct positive integers and other than . We give a partial answer to this question using equation (1.3). Let be a positive integer and the set of non-trivial -SR-knots. Then we have the following.
Theorem 1.6**.**
If for positive integers and with , then we have either that , , or .
2. Proofs of Theorem 1.1 and Theorem 1.5
Let be a knot obtained from a knot by an elementary -SR-fusion with respect to with its attendant knot . Let be a Seifert surface for . Here we may take so that . Let . We first transform into “standard” position and construct a Seifert surface for from in standard position. Then, we calculate using .
We may take so that the intersections with are only arcs of and . Then we divide the set of singularities of into two: one which consists of , denoted by , and the other which consists of , denoted by . Thus the set of singularities of is . We say that is in standard position if and (see Figure 9 for example). To transform into standard position, we need the following three transformations. Here note that each transformation changes neither , , nor the knot type of .
Sliding a disk along a band : Deforming by deformation retraction into a regular neighborhood of and slide along toward . Here follows (see Figure 4 for example). We allow to pass through . Then an additional intersection of and is created.
Winding a band along : Winding along in a regular neighborhood of either from negative side to positive side or from positive side to negative side (see Figure 5 for example). Here an additional intersection of and is created.
Tubing : Removing two disks and from and attatch an annulus so that and the result is orientable (see Figure 6 for example).
Proposition 2.1**.**
Let be a knot obtained from a knot by an elementary -SR-fusion with respect to with its attendant knot . Let be a Seifert surface for such that and let . Then we may transform into standard position by sliding a disk along a band, winding a band along , and tubing .
Proof.
First if , then take the smallest index such that and slide along just next to so that (See Figure 4 for example). Then slide along inductively just next to so that .
Next if , then take an arbitrary and let , , be its singularities which are placed close to on in this order. Assume that is oriented as from towards and let be the signed intersection number of and at . First wind along depending on . If (resp. ), then wind along from negative side to positive side (resp. from positive side to negative side) as illustrated in Figure 5. Here we make these transformations from to in this order, and notice that each transformation creates a new intersection with . Then make a tubing so to erase and from to in this order as illustrated in Figure 6, and now is in standard position. ∎
Proof of Theorem 1.1. Let be a Seifert surface for such that and let . Here we may assume that is in standard position from Proposition 2.1. Thus the set of singularities of is . Erase and to have a Seifert surface for by orientation preserving cut and deformation as illustrated in the second left of Figure 7 and Figure 8, respectively (see Figure 10 for example of ).
Take a basis , , , , , , , , , , , , , , of as illustrated in Figure 7 and Figure 8 (see Figure 10 for example), where , , is a basis of . Then we have the following Seifert matrix with respect to the basis.
[TABLE]
where is a Seifert matrix for , is the zero matrix,
is an matrix with p^{1}_{ij}=\mathrm{lk}(x_{i},z_{j}^{+})=\left\{\begin{array}[]{ll}\!\!\!-(\varepsilon_{i}+1)/2&\text{if i=j}\\ ~{}\>~{}\>~{}\>~{}\>~{}\varepsilon_{i}&\text{if i=1j=m},\\ &\text{or 2\leq i\leq mj=i-1}\\ ~{}\>~{}\>~{}\>~{}\>~{}0&\text{otherwise,}\end{array}\right.
is an matrix with p^{2}_{ij}=\mathrm{lk}(x_{i},w_{j}^{+})=\left\{\begin{array}[]{ll}~{}\>~{}\>~{}\>~{}\>~{}\varepsilon_{1}{}{}{}{}{}{}&\text{if i=1j=|l|}\\ ~{}\>~{}\>~{}\>~{}\>~{}0{}{}{}{}{}{}&\text{otherwise,}\end{array}\right.
is an matrix with p^{3}_{ij}=\mathrm{lk}(y_{i},z_{j}^{+})~{}=\left\{\begin{array}[]{ll}~{}\>~{}\>~{}\>~{}\>~{}\varepsilon{}{}{}{}{}{}{}&\text{if j=m}\\ ~{}\>~{}\>~{}\>~{}\>~{}0{}{}{}{}{}{}{}&\text{otherwise,}\end{array}\right.
is an matrix with p^{4}_{ij}=\mathrm{lk}(y_{i},w_{j}^{+})=\left\{\begin{array}[]{ll}(\varepsilon+1)/2{}{}&\text{if i=j}\\ (\varepsilon-1)/2{}{}&\text{if 2\leq i\leq|l|j=i-1}\\ ~{}\>~{}\>~{}\>~{}\>~{}0&\text{otherwise,}\end{array}\right.
if , and if ,
is an matrix with q^{1}_{ij}=\mathrm{lk}(z_{i},x_{j}^{+})=\left\{\begin{array}[]{ll}\!\!\!-(\varepsilon_{i}-1)/2&\text{if i=j}\\ ~{}\>~{}\>~{}\>~{}\>~{}\varepsilon_{i}&\text{if i=mj=1},\\ &\text{or 1\leq i\leq m-1j=i+1}\\ ~{}\>~{}\>~{}\>~{}\>~{}0&\text{otherwise,}\end{array}\right.
is an matrix with q^{2}_{ij}=\mathrm{lk}(z_{i},y_{j}^{+})~{}=\left\{\begin{array}[]{ll}~{}\>~{}\>~{}\>~{}\>~{}\varepsilon{}{}{}{}{}{}{}&\text{if i=m}\\ ~{}\>~{}\>~{}\>~{}\>~{}0{}{}{}{}{}{}{}&\text{otherwise,}\end{array}\right.
is an matrix with q^{3}_{ij}=\mathrm{lk}(w_{i},x_{j}^{+})=\left\{\begin{array}[]{ll}~{}\>~{}\>~{}\>~{}\>~{}\varepsilon_{1}{}{}{}{}{}{}&\text{if i=|l|j=1}\\ ~{}\>~{}\>~{}\>~{}\>~{}0{}{}{}{}{}{}&\text{otherwise, and}\end{array}\right.
is an matrix with q^{4}_{ij}=\mathrm{lk}(w_{i},y_{j}^{+})=\left\{\begin{array}[]{ll}(\varepsilon-1)/2{}{}&\text{if i=j}\\ (\varepsilon+1)/2{}{}&\text{if 1\leq i\leq|l|-1j=i+1}\\ ~{}\>~{}\>~{}\>~{}\>~{}\>~{}0&\text{otherwise,}\end{array}\right.
if , and if , and \varepsilon=\left\{\begin{array}[]{rl}1&\text{if lis positive}\\ -1&\text{ifl is negative}\end{array}\right., \varepsilon_{i}=\left\{\begin{array}[]{rl}1&\text{if B_{i}is positive}\\ -1&\text{ifB_{i} is negative}\end{array}\right.
. Letting , , , and , we have the following.
P\!=\!\bordermatrix{&\!z^{+}_{1}\!&\!z^{+}_{2}\!&\!\cdots\!&\!z^{+}_{m-1}\!&\!z_{m}\!&\!w^{+}_{1}\!&\!w^{+}_{2}\!&\!\cdots\!&\!w^{+}_{|l|-1}\!\!&\!\!w^{+}_{|l|}\!\cr x_{1}&-a_{1}\!\!\!\!&&&&\!\!\!\!\varepsilon_{1}\!\!\!\!&&&&&\!\!\!\!\varepsilon_{1}\!\!\!\!\cr x_{2}&\varepsilon_{2}\!\!\!\!&\!\!\!\!-a_{2}\!\!\!\!&&&&&&&&\cr~{}\vdots&&\!\!\!\!\ddots\!\!\!\!&\!\!\!\!\ddots\!\!\!\!&&&&&&&\cr x_{m-1}&&&\!\!\!\!\ddots\!\!\!\!&\!\!\!\!-a_{m-1}\!\!\!\!&&&&&&\cr x_{m}&&&&\!\!\!\!\varepsilon_{m}\!\!\!\!&\!\!\!\!-a_{m}\!\!\!\!&&&&&\cr y_{1}&&&&&\varepsilon&\!\!\!a\!\!\!&&&&\cr y_{2}&&&&&\varepsilon&\!\!\!b\!\!\!&\!\!\!a\!\!\!&&&\cr~{}\vdots&&&&&\varepsilon&&\!\!\!\ddots\!\!\!&\!\!\!\ddots\!\!\!&&\cr y_{|l|-1}&&&&&\varepsilon&&&\!\!\!\ddots\!\!\!&\!\!\!a\!\!\!&\cr y_{|l|}&&&&&\varepsilon&&&&\!\!\!b\!\!\!&\!\!\!a\!\!\!\cr}, Q\!=\!\bordermatrix{&\!x^{+}_{1}\!&\!x^{+}_{2}\!&\!\cdots\!&\!x^{+}_{m-1}\!&\!x_{m}\!&\!y^{+}_{1}\!&\!y^{+}_{2}\!&\!\cdots\!&\!y^{+}_{|l|-1}\!\!&\!\!y^{+}_{|l|}\!\cr z_{1}&-b_{1}\!\!\!\!&\!\!\!\!\varepsilon_{2}\!\!\!\!&&&&&&&&\cr z_{2}&&\!\!\!\!-b_{2}\!\!\!\!&\!\!\!\!\ddots\!\!\!\!&&&&&&&\cr\vdots&&&\!\!\!\!\ddots\!\!\!\!&\!\!\!\!\ddots\!\!\!\!&&&&&&\cr z_{m-1}&&&&\!\!\!\!-b_{m-1}\!\!\!\!&\!\!\!\!\varepsilon_{m}\!\!\!\!&&&&&\cr z_{m}&\!\varepsilon_{1}\!&&&&\!\!\!\!-b_{m}\!\!\!\!&\varepsilon&\varepsilon&\varepsilon&\varepsilon&\varepsilon\cr w_{1}&&&&&&b&a&&&\cr w_{2}&&&&&&&b&a&&\cr\vdots&&&&&&&&\!\!\!\ddots\!\!\!&\!\!\!\ddots\!\!\!&\cr w_{|l|-1}&&&&&&&&&\!\!\!b\!\!\!&a\cr w_{|l|}&\!\varepsilon_{1}\!&&&&&&&&&b\cr}
Then the Alexander polynomial of is the product of the Alexander polynomial of , , and .
Claim 2.2**.**
We have the following, where , , , , , and .
[TABLE]
*Proof. * First we calculate noticing that .
If , then we have that |P\!-\!t\,Q^{T}|=\begin{array}[]{|ccccc|}\!-c_{1}\!\!&&&&e_{1}\\[-2.15277pt] \!e_{2}\!&\!\!-c_{2}\!\!\!&&&\\[-4.30554pt] &\!\!\!\ddots\!\!\!&\!\!\ddots\!\!\!&&\\[-6.45831pt] &&\!\!\ddots\!\!\!&\!-c_{m-1}\!\!\!&\\[-2.15277pt] &&&e_{m}&\!\!-c_{m}\!\!\end{array} .
If , then we have that
|P\!-tQ^{T}|=\begin{array}[]{|ccccc|c|}\!-c_{1}\!\!&&&&e_{1}\!\!\!&e_{1}\!\\[-2.15277pt] \!e_{2}\!&\!\!-c_{2}\!\!\!&&&&\\[-4.30554pt] &\!\!\!\ddots\!\!\!&\!\!\ddots\!\!\!&&&\\[-6.45831pt] &&\!\!\ddots\!\!\!&\!-c_{m-1}\!\!\!&&\\[-2.15277pt] &&&e_{m}&\!\!-c_{m}\!\!&\\ \hline\cr&&&&e&c\end{array}=\begin{array}[]{|ccccc|c|}\!-c_{1}\!\!&&&&0\!\!\!&e_{1}\!\\[-2.15277pt] \!e_{2}\!&\!\!-c_{2}\!\!\!&&&&\\[-4.30554pt] &\!\!\!\ddots\!\!\!&\!\!\ddots\!\!\!&&&\\[-6.45831pt] &&\!\!\ddots\!\!\!&\!-c_{m-1}\!\!\!&&\\[-2.15277pt] &&&e_{m}&\!\!-c_{m}\!\!&\\ \hline\cr&&&&d&c\end{array}\, .
If , then we have that
|P\!-tQ^{T}|=\begin{array}[]{|ccccc|ccccc|}\!-c_{1}\!\!&&&&e_{1}\!\!\!&&&&&e_{1}\!\\[-2.15277pt] \!e_{2}\!&\!\!-c_{2}\!\!\!&&&&&&&&\\[-4.30554pt] &\!\!\!\ddots\!\!\!&\!\!\ddots\!\!\!&&&&&&&\\[-6.45831pt] &&\!\!\ddots\!\!\!&\!-c_{m-1}\!\!\!&&&&&&\\[-2.15277pt] &&&e_{m}&\!\!-c_{m}\!\!&&&&&\\ \hline\cr&&&&e&c&&&&\\[-2.15277pt] &&&&e&d&c&&&\\[-5.16663pt] &&&&e&&\ddots&\ddots&&\\[-6.45831pt] &&&&e&&&\ddots&c&\\[-2.15277pt] &&&&e&&&&d&c\!\\[-2.15277pt] \end{array}=\begin{array}[]{|ccccc|ccccc|}\!-c_{1}\!\!&&&&0&&&&&e_{1}\!\!\\[-2.15277pt] \!e_{2}\!&\!\!-c_{2}\!\!\!&&&&&&&&\\[-4.30554pt] &\!\!\!\ddots\!\!\!&\!\!\ddots\!\!\!&&&&&&&\\[-6.45831pt] &&\!\!\ddots\!\!\!&\!-c_{m-1}\!\!\!&&&&&&\\[-2.15277pt] &&&e_{m}&\!\!-c_{m}\!\!&&&&&\\ \hline\cr&&&&d&c&&&&\\[-2.15277pt] &&&&0&d&c&&&\\[-5.16663pt] &&&&0&&\ddots&\ddots&&\\[-6.45831pt] &&&&0&&&\ddots&c&\\[-2.15277pt] &&&&0&&&&d&c\!\!\\[-2.15277pt] \end{array}\,
.
Next we calculate noticing that .
If , then we have that |Q-t\,P^{T}|=\begin{array}[]{|ccccc|}\!\!-d_{1}\!\!&e_{2}\!\!\!&&&\\[-4.30554pt] &\!\!-d_{2}\!\!\!\!\!&\ddots\!\!&&\\[-5.16663pt] &&\ddots\!\!&\ddots\!\!&\\[-2.15277pt] &&&\!\!\!\!-d_{m-1}\!\!\!&e_{m}\\[-2.15277pt] e_{1}\!\!\!&&&&\!\!\!-d_{m}\!\!\end{array}=\displaystyle d^{\,0}\prod_{i=1}^{m}(-d_{i})+(-1)^{0+m+1}c^{\,0}\prod_{i=1}^{m}e_{i}.
If , then we have that
|\,Q\!-tP^{T}|=\begin{array}[]{|ccccc|c|}\!\!-d_{1}\!\!&e_{2}\!\!\!&&&&\\[-2.15277pt] &\!\!-d_{2}\!\!\!\!\!&\ddots\!\!&&&\\[-5.16663pt] &&\ddots\!\!&\ddots\!\!&&\\[-2.15277pt] &&&\!\!\!\!-d_{m-1}\!\!\!&e_{m}&\\[-1.29167pt] e_{1}\!\!\!&&&&\!\!\!-d_{m}\!\!&e\\ \hline\cr e_{1}\!\!\!&&&&&d\\[-2.15277pt] \end{array}=\begin{array}[]{|ccccc|c|}\!\!-d_{1}\!\!&e_{2}\!\!\!&&&&\\[-2.15277pt] &\!\!-d_{2}\!\!\!\!\!&\ddots\!\!&&&\\[-5.16663pt] &&\ddots\!\!&\ddots\!\!&&\\[-2.15277pt] &&&\!\!\!\!-d_{m-1}\!\!\!&e_{m}&\\[-1.29167pt] 0&&&&\!\!\!-d_{m}\!\!&c\\ \hline\cr e_{1}\!\!\!&&&&&d\\[-2.15277pt] \end{array} .
If , then we have that
|\,Q\!-tP^{T}|=\begin{array}[]{|ccccc|ccccc|}\!\!-d_{1}\!\!&e_{2}\!\!\!&&&&&&&&\\[-2.15277pt] &\!\!-d_{2}\!\!\!\!\!&\ddots\!\!&&&&&&&\\[-5.16663pt] &&\ddots\!\!&\ddots\!\!&&&&&&\\[-2.15277pt] &&&\!\!-d_{m-1}\!\!\!&e_{m}&&&&&\\[-1.29167pt] e_{1}\!\!\!&&&&\!\!\!-d_{m}\!\!&e&e&\cdots&e&e\\ \hline\cr&&&&&d&c&&&\\[-2.15277pt] &&&&&&d&\ddots&&\\[-5.16663pt] &&&&&&&\ddots&\ddots&\\[-2.15277pt] &&&&&&&&d&c\\[-2.15277pt] e_{1}\!\!\!&&&&&&&&&d\\[-2.15277pt] \end{array}=\begin{array}[]{|ccccc|ccccc|}\!\!-d_{1}\!\!&e_{2}\!\!\!&&&&&&&&\\[-2.15277pt] &\!\!-d_{2}\!\!\!\!\!&\ddots\!\!&&&&&&&\\[-5.16663pt] &&\ddots\!\!&\ddots\!\!&&&&&&\\[-2.15277pt] &&&\!\!-d_{m-1}\!\!\!&e_{m}&&&&&\\[-1.29167pt] 0&&&&\!\!\!-d_{m}\!\!&c&0&\cdots&0&0\\ \hline\cr&&&&&d&c&&&\\[-2.15277pt] &&&&&&d&\ddots&&\\[-5.16663pt] &&&&&&&\ddots&\ddots&\\[-2.15277pt] &&&&&&&&d&c\\[-2.15277pt] e_{1}\!\!\!&&&&&&&&&d\\[-2.15277pt] \end{array}
.
Now we calculate the Alexander polynomial of diving the case into two depending on the value of ; or . Here note the following.
[TABLE]
Case : From the above table, we have the following;
Case : From the above table, we have the following;
In both cases, we obtain that , and thus we complete the proof.
Proof of Theorem 1.5. For each , we can construct a simple-ribbon knot with by following the proof of Theorem 1.1 (see also Figure 9). Let be the connected sum of , , , . Then is a simple-ribbon knot such that . Let be the set of disks and bands which gives the SR-fusion on the trivial knot producing . Take a -ball which is a small neighborhood of a point of and a trivial knot in which intersects twice so that . Let be the closure of . Since is the trivial knot, is an unknotted torus which contains with , where is the absolute value of the algebraic intersection number of with a meridian disk of .
Let be a tubular neighborhood of the Kinoshita-Terasaka knot and a faithful homeomorphism of onto , i.e. maps the preferred longitude of onto the preferred longitude of . Since , we obtain that for by Proposition 8.23 of [1]. Since is faithful and both of and are ribbon knots, is also a ribbon knot by Lemma 3 of [9]111 Lemma 3 shows that is ribbon cobordant to if is a ribbon knot, although it states that is cobordant to .. On the other hand, as and is a non-trivial knot, is not a simple ribbon knot by Corollary 1.8 of [5].
3. Proof of Theorem 1.6
Note that if is a knot of , then for some non-negative integers and by Corollary 1.2. Moreover if is also a knot of , then for some non-negative integers and , and thus the set of prime factors of and coinside, where for , , , and .
Let be the set of prime factors of an integer , and the greatest common divisor of positive integers and . Note that if and , then we have that . Here we prepare several lemmas, the first one of which is the theorem by P. Mihăilescu (the Catalan conjecture).
Lemma 3.1**.**
([7, Theorem 5])* The following equation has no other integer solutions but .*
[TABLE]
Lemma 3.2**.**
([2, Theorem 1])* Let , , and be integers such that and . Then if and only if , , and for an integer .*
Lemma 3.3**.**
Let be an integer such that . Then the followings hold.
- (1)
* for an odd integer if and only if and .*
- (2)
* for an even integer if and only if and for an integer .*
Proof.
Since the if parts are easy to be checked, we only show the only if parts.
(1) First the following equation holds, since is odd.
[TABLE]
If is prime, then we have that from equation (3.2), and thus that , since . Moreover, we have that mod also from equation (3.2), since mod , mod . Hence we obtain that . If , then we also have that
[TABLE]
since . However then it contradicts that . Therefore we have that . Then we have that from equation (3.2), and thus that , since , which completes the proof.
If is not prime, then let be a prime factor of , and let and . Since and are odd, we have that divides and that divides . Hence we have that , since . Hence we have that , since . Thus from the previous case, we have that and , and thus and . However then, we have that , which contradicts that is not prime.
(2) Since is even, we have that . Hence we have that , and thus that . Thus we have that from Lemma 3.2. If , then we have that and thus that and are not coprime, since . Hence we have that , since . Therefore we obtain that for , which completes the proof. ∎
Using Lemma 3.1 and Lemma 3.3, we show the following.
Proposition 3.4**.**
Let , , and be integers such that and , . Then we have the following.
- (1)
* if and only if , , and ;*
- (2)
* if and only if one of the following holds.*
- (i)
, , and
- (ii)
, , and
- (iii)
, , and and
- (iv)
, , and for an integer .
Proof.
First we have the following for indeterminate and positive integers , , and and a non-negative integer such that .
[TABLE]
[TABLE]
Let . Then we have the following.
Claim 3.5**.**
, or .
Proof.
For positive integers and , let be the sequence obtained by the Euclidian algorithm. Then letting , we also have the following from equations (3.4) and (3.5).
[TABLE]
[TABLE]
Hence by letting or , we have that , is either or , which induces the conclusion. ∎
Since the if parts are easy to be checked, we only show the only if parts.
(1) Since , we have that and are not coprime, and thus that or from Claim 3.5. In the former case, we have that . Thus, and for , since . However then, we have that , which contradicts that . In the latter case, we have that and that with an odd integer from equation (3.4). If , then , which contradicts that . Thus is odd and . Then we have that and by Lemma 3.3 (1), and thus that , , . Hence we have that , since , which completes the proof.
(2) Since , we have that and are not coprime, and thus that or from Claim 3.5. In the former case, we have that , and thus that or . If , then , which contradicts that . If and , then we have that and , and thus that . Then by Lemma 3.1, we have that , and thus obtain condition (i).
In the latter case, we have that and that with an odd integer from equation (3.4). Consider the case where . Then we have that and by Lemma 3.3 (1), and thus that , , . Since , and thus and , we have that and thus that . Therefore we obtain condition (ii).
Next consider the case where , i.e., . Hence let and . Thus we have that and that . Therefore is even, since otherwise does not divide . Then we have that and for by Lemma 3.3 (2). If and , then the equation has the unique solution by Lemma 3.1, and thus we obtain condition (iii). If , then we have that and for , i.e., condition condition (iv). If (resp. ), then we have that (resp. ) and , and thus that condition (iv). ∎
Now using Proposition 3.4 and Lemma 3.2 we obtain the following.
Lemma 3.6**.**
Let , , , , , be positive integers with . Then we have the following.
- (1)
.
- (2)
If , then , , and .
- (3)
If , then , , or , , .
- (4)
- (5)
If , then , .
- (6)
If , then , , .
Proof.
Note that if positive integers , and non-negative integers , satisfies the equation , then . The first three statements are obtained by Lemma 3.2, Proposition 3.4 (1), and Proposition 3.4 (2), respectively. For the last three statements, note that . Therefore (4) and (5) are obtained by Lemma 3.2, and (6) is obtained by Proposition 3.4 (2). ∎
Proof of Theorem 1.6. Let be a knot of . Then we have that for some non-negative integers , , , and by Corollary 1.2. Thus we obtain the conclusion by Lemma 3.6.
Acknowledgement
The authors would like to thank Alexander Zupan for informing us errors of the diagrams of and in Figure 3 of [6].
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] G. Burde and H. Zieschang, Knots, de Gruyter, 1985.
- 2[2] T. Ishikawa, N. Ishida and Y. Yukimoto, On prime factors of A n − 1 superscript 𝐴 𝑛 1 A^{n}-1 , Amer. Math. Monthly, 111 (2004), 243–245.
- 3[3] A. Kawauchi, A survey of knot theory, Birkhuser Verlag, Basel, 1996.
- 4[4] K. Kishimoto, T. Shibuya and T. Tsukamoto, Simple-ribbon fusions and genera of links , J. Math. Soc. Japan, 68 (2016), 1033–1045.
- 5[5] K. Kishimoto, T. Shibuya and T. Tsukamoto, Simple-ribbon concordance of knots , Kobe J. Math, 37 (2020), 1–17.
- 6[6] K. Kishimoto, T. Shibuya T. Tsukamoto and T. Ishikawa, Alexander polynomials of simple-ribbon knots , Osaka J. Math, 58 (2021), 41–57.
- 7[7] P. Mihăilescu, Primary Cyclotomic Units and a Proof of Catalan’s Conjecture , J. Reine Angew. Math., 572 (2004), 167–195.
- 8[8] H. Schubert, Knoten und vollringe , Acta Mathematica, 90 (1953), 131–286.
