Abstract
We prove a conjecture on the second minimal odd periodic orbits with respect to Sharkovski ordering for the continuous endomorphisms on the real line. A -periodic orbit , () is called second minimal for the map f, if is a minimal period of in the Sharkovski ordering. Full classification of second minimal orbits is presented in terms of cyclic permutations and directed graphs of transitions. It is proved that second minimal odd orbits either have a Stefan-type structure like minimal odd orbits or one of the types, each characterized with unique cyclic permutations and directed graphs of transitions with an accuracy up to the inverses. The new concept of second minimal orbits and its classification have an important application towards an understanding of the universal structure of the distribution of the periodic windows in the bifurcation diagram generated by the chaotic dynamics of nonlinear maps on the interval.
Keywords:
discrete dynamical system; continuous endomorphism; directed graph of transitions; Sharkovski’s theorem; minimal periodic orbit; second minimal orbit MSC:
37D05; 37D45
1. Introduction
Let be a continuous endomorphism, and I be a non-degenerate interval on the real line. Let be an n-th iteration of f. A point is called a periodic point of f with period m if , for . The set of m distinct points
is called the orbit of c, or briefly, an m-orbit or periodic m-cycle. In their celebrated paper [1], Sharkovski discovered a law on the coexistence of periodic orbits of continuous endomorphisms on the real line.
Theorem 1
([1]). Let the positive integers be totally ordered in the following way:
If a continuous endomorphism, , has a cycle of period n and , then f also has a periodic orbit of period m.
This result played a fundamental role in the development of the theory of discrete dynamical systems [2,3,4]. Following the standard approach ([2,5]), we characterize each periodic orbit with cyclic permutations and directed graphs of transitions or digraphs. Consider the m-orbit:
Definition 1.
If for , with , then is associated with the cyclic permutation
In the sequel, means either or .
Definition 2.
Let . The digraph of the m-orbit is a directed graph of transitions with vertices and oriented edges if .
Definition 3.
The inverse digraph of the m-orbit is obtained from the digraph of the m-orbit by replacing each with .
The inverse of the digraph associated with the cyclic permutation is a digraph associated with the cyclic permutation , where is the order-reversing permutation:
Definition 4.
A continuous function is called the P-linearization of f if and P is a linear function in each interval
Definition 5.
The arrangement of the minimums and maximums of the map in the open interval will be called the topological structure of the periodic orbit.
The proof of Sharkovski’s theorem significantly uses the concept of a minimal orbit.
Definition 6.
The m-orbit of f is called minimal if m is the minimal period of in the Sharkovski ordering.
Definition 7.
The digraph of the m-orbit contains the red edge Ji→Js if .
The structure of minimal orbits is well understood [2,6,7,8,9,10]. Minimal odd orbits are called Stefan orbits, due to the following characterization:
2. Main Results
The main goal of this paper is the characterization of second minimal odd orbits.
Definition 8.
A -orbit, is called second minimal if is the minimal period of in the Sharkovski ordering.
To achieve the full characterization of second minimal odd orbits, in the next definition, we introduce a new notion of the simplicity of odd periodic orbits. Let , be subsets of a -orbit defined as
Definition 9.
A -orbit is called simple if either
- 1.
- is mapped to ; and is mapped to except for one point; or
- 2.
- is mapped to ; and is mapped to except for one point.
We say a simple -orbit is of type + (resp. type −) if (1) (resp. (2)) is satisfied.
First of all, note that the Stefan orbits or minimal odd orbits are simple according to Definition 9. Our first main result reads:
Theorem 3.
Second minimal -orbits, , are simple.
To pursue a full classification of second minimal odd orbits, first note that second minimal odd orbits may have a Stefan structure as identified in Theorem 2. Indeed, consider a map that is the P-linearization of the minimal -orbit. It has a unique fixed point that is an interior point of one of the two middle intervals. We can replace the linear function in the small neighborhood F of the fixed point with a P-linearization of the minimal -orbit and join this function continuously with the original map outside of the small neighborhood of a size twice that of F. Moreover, we can choose the size of F to be so small that the digraph of the -orbit is not changed and still has a Stefan structure. Obviously, the -orbit is second minimal with respect to the new map, although its Stefan structure is unchanged. Therefore, to complete the full classification, it remains to clarify the structure of all second minimal odd orbits with a non-Stefan structure. Our main classification result reads:
Theorem 4.
Simple positive-type second minimal -orbits are either Stefan orbits or have one of the types, each with a unique digraph and cyclic permutation. Their inverses represent all second minimal -orbits of the simple negative type. The topological structure of all simple positive types of second minimal -orbits with a non-Stefan structure is presented in Table 1. The topological structure of their inverses is obtained by replacing “max” and “min” with each other. The P-linearization of each of the types (and their inverses) presents an example of a continuous map with a second minimal -orbit.
Table 1.
Topological structure of all second minimal -orbits of the simple positive type with a non-Stefan structure.
Theorems 3 and 4 in the particular case were proved in [11]. The proof of Theorems 3 and 4 is constructive, and provides explicit description of all types of second minimal odd orbits in terms of cyclic permutations and digraphs. Second minimal orbits play an important role in the problem on the distribution of periodic windows within the chaotic regime of the bifurcation diagram of the one-parameter family of unimodal maps dependent on a parameter. For example, consider an iterative relation , where the maps satisfy with a single maximum at some point, , interior to the interval . The problem is to comprehend a full characterization of the asymptotic behavior of for and how this behavior depends on the parameter . A prototypical example is the logistic map
In 1978, Fiegenbaum [12,13,14] discovered a universal transition mechanism to chaos through successive period doubling bifurcations. As , with some transition value , the behavior of for large n changes from periodic to chaotic via bifurcations from the periodic cycle to the periodic cycle. Two universal constants and qualitatively characterize the universal transition route. Let be the value of the parameter when -orbit is superstable, i.e., the critical point is one of the elements of the orbit, and let be the directed distance from to the closest element of the orbit:
Then, , and for a class of unimodal maps with a quadratic maximum, has
Having discovered the universality of and numerically, Feigenbaum proposed a mechanism for it based on the renormalization group approach to critical phenomena in statistical mechanics. He revealed that both of these constants are related to a universal function that governs the period-doubling route to chaos and expressed this function as the fixed point of the doubling transformation operator
in the class of symmetric -unimodal maps on with . Moreover, the Frechet derivative of at the fixed point g has a simple eigenvalue equal to , while the remainder of the spectrum is contained in the open unit disk. The rigorous proof of Feigenbaum universality theory in the class of -unimodal maps was completed in [15,16,17] (see also [18]). Thus, the Feigenbaum scenario of transition from periodic to chaotic behavior gives a full characterization of the dynamical system in the range of parameter . There was a long quest to understand the behavior of the dynamical system beyond the transition to chaotic range when . It was well-known even before Feigenbaum’s discovery that one can observe all possible periodic orbits within the chaotic regime. The well-known bifurcation diagram—asymptotic behavior of as (periodic orbits or chaotic attractors) versus parameter demonstrates the periodic windows in the chaotic regime, with the period 3 window being the largest (e.g., see Figure 14 in [11]). In [19], periodic orbits are characterized through their pattern, which is the sequence of R’s and L’s, the kth letter expressing the fact that the kth element of the cycle is on the right or left side of the critical point of the map. In particular, ref. [19] presents a table of the relative positions of periodic orbits of period for the logistic map. Much of the work in this direction was inspired by the paper [20], where the calculus for describing the qualitative behavior of successive iterates of piecewise monotone maps of the interval was invented. We refer to [18], which presents an extensive description of this approach. A full characterization of the distribution of the periodic windows beyond the transition value is achieved in [11]. Through numerical analysis, the universal pattern is revealed for the distribution of periodic orbits within the chaotic regime of the bifurcation diagram of the one-parameter family of unimodal maps, when the parameter changes in the range between the Feigenbaum transition point to chaos and the value when the superstable 3-orbit appears for the first time. Remarkably, the bifurcation diagram in the indicated parameter range is divided into infinitely many Sharkovski s-blocks where all the -orbits are distributed and the pattern is independent of s. Moreover, it is demonstrated that any superstable odd orbit in the indicated parameter range are going through successive period doublings, according to the Feigenbaum scenario, when the parameter decreases to the critical transition point. In particular, this reveals that Feigenbaum universality is true in very general classes of maps, such as the class of maps that are the st iteration of the class of -unimodal maps. This generalization is a driving force of infinitely many Feigenbaum scenarios of a transition to chaos through successive bifurcations of all possible odd orbits in the indicated range when the parameter decreases towards the first transition value to chaos. Ref. [11] outlined the rigorous Feigenbaum universality theory in the general class of maps, which are the st iteration of the class of -unimodal maps. To reveal the role of Sharkovski ordering in Feigenbaum universality, in [11], we pursued a fine classification of periodic orbits via their cyclic permutations and directed graphs of transitions. That was a motivation for introducing a concept of a second minimal periodic orbit with respect to the Sharkovski ordering for continuous endomorphisms on the real line. The results of [11] demonstrated that the first appearance of any orbit in the indicated parameter range is always a minimal orbit. Remarkably, the second appearances of all odd orbits are always second minimal orbits with a Type 1 digraph. The reason for the relevance of Type 1 s minimal (2k + 1)-orbits is that the topological structure of the single maximum unimodal map is equivalent to the topological structure of the piecewise monotonic map associated with Type 1 s minimal (2k + 1)-orbits. In [11], it is proven that there are nine types of second minimal 7-orbits, unique up to their inverses. It was conjectured that there are types of second minimal (2k + 1)-orbits, unique up to their inverses. The goal of this paper is to prove this conjecture and to pursue a full classification of the second minimal orbits in terms of their cyclic permutations and directed graphs of transitions, as is formulated in Theorems 3 and 4.
It should be pointed out that our main results can be formulated in the framework of formalized combinatorial dynamics, where without any reference to orbits and their associated maps, the objects are permutations (or patterns), and the main problem is to identify the forcing relation between various patterns (see [2]). Another interesting open problem in combinatorial dynamics is the genealogy of second minimal odd orbits [21,22,23].
3. Preliminary Results
Lemma 1.
The digraph of an m-orbit, , , possesses the following properties [2]:
- 1.
- The digraph contains a loop: such that .
- 2.
- , and such that ; moreover, it is always possible to choose unless m is even and , and it is always possible to choose unless .
- 3.
- If , , then and such that .
- 4.
- The digraph of a cycle with period contains a subgraph for any .
Definition 10.
A cycle in a digraph is said to be primitive if it does not consist entirely of a cycle of smaller length described several times.
Lemma 2
(Straffin [2,24]). If f has a periodic point of period and its associated digraph contains a primitive cycle of length m, then f has a periodic point y of period m such that .
Lemma 3
(Converse Straffin [2]). Let f have a periodic point of period with a digraph . Suppose f is strictly monotonic on each subinterval for . If f has an orbit of period m in the open interval , then either contains a primitive cycle of length m or m is even and contains a primitive cycle of length .
4. Proofs of Theorems 3 and 4
Let be a continuous endomorphism that has a -orbit () that is second minimal. Let be the ordered elements of this orbit; and let . Such an exists since and . So, ; Let ; thus, we have and hence, . Assume, without loss of generality, . Let . We have , and hence, . From Lemma 1, the existence of the subgraph
follows. Assume that (6) presents the shortest path. Since there are intervals, its length is at most and at least . Indeed, if its length is or less, then Lemma 2 implies the existence of an odd periodic orbit of period or less. Let us change the indices of intervals in (6) successively as and write path (6) as
where , , or ; for simplicity, we are going to use the notation i for . In the sequel, the notation in the second row of the cyclic permutation means that either of the entries a or b is a valid choice for the image of the node in the same column of the first row; means and , the notation means the union of , and all the intervals between them. Note that if and , then .
Since (7) is the shortest path, we have
we also have
unless , . Indeed, otherwise according to Lemma 2, an odd orbit of length less than must exist. From (8) and (9), we can infer the relative position of the intervals to be either (Figure 2)
Figure 2.
Relative positions of intervals in the sub-graph of length m when to the right of .
Or (Figure 3).
Figure 3.
Relative positions of intervals in the sub-graph of length m when to the left of .
If , then the path (7) contains all intervals. From the proof of Theorem 2 (for example, see Proposition 8 in [2]), it follows that the corresponding periodic orbit is a Stefan orbit.
Lemma 4.
The case when produces exactly 2 second minimal -orbits. Cyclic permutations are given in (10) and (11), and the corresponding digraphs are presented in Figure 4 and Figure 5, respectively.
Figure 4.
Digraph of first cyclic permutation (10) when m = 2k − 1.
Figure 5.
Digraph of second cyclic permutation (11) when m = 2k − 1.
Proof.
When the length of the path (7) is , we have exactly one interval, call it , missing. Since , for odd, one of the endpoints of must be mapped to some element of the orbit that separates and . Since , but , it follows that the endpoint of that separates and must be mapped to the element of the orbit that separates and . Therefore, unless there is an interval between and , the element of the orbit that separates and will be an image of two distinct elements of the orbit. Hence, is between and , and the distribution of the intervals is as in Figure 6 or Figure 6 reflected about the center point . Note that the distribution described in Figure 6 is relevant due to our assumption . The other case will provide the associated inverse digraph with . Hence, the structure is as described in Figure 6.
Figure 6.
Complete interval for case when with .
This implies the following cyclic permutation. Note the possible alternation of images of elements 1, , , and k.
- Case :
- Case : ; This produces a simple positive type -orbit given in (10) and Figure 4 with topological structure max-min-max. Next, we analyze the digraph to show that there are no primitive cycles of even length , which would imply by Straffin’s lemma, an existence of odd periodic orbit of length . From Lemma 3, it then follows that the P-linearization of the orbit (10) presents an example of a continuous map with a second minimal -orbit. We split the analysis into two cases:
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not start with chain . Since any such cycle can be formed only by adding on to the starting vertex pairs . Therefore, the length of the cycle (by counting twice) will always be an odd number. Conversely, if the cycle starts with chain , then to close it at , the smallest required even length is .
- (b)
- Consider primitive cycles that do not contain . Obviously, such a cycle does not contain or since these vertices have red edges connecting them all the way to . Additionally, this cycle cannot contain or since is the only vertex (besides itself) with a directed edge to , and is the only vertex with a directed edge to . This leaves 4 vertices: . Since , and , , any cycle formed by these four vertices will consist of a starting vertex followed (or ending vertex preceded) by pairs , added arbitrarily many times, and hence no cycles of even length can be produced.
- Case : , then we have the period 4-suborbit, a contradiction.
- Case : .
- Case : , then we have the period 2-suborbit , a contradiction.
- Case : ; This produces a simple positive type -orbit given in (11) and Figure 5 with topological structure max-min-max. We repeat the argument from Case . First, we analyze the digraph to show that there are no primitive cycles of even length . We split the analysis into two cases:
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as a starting vertex. First, assume that the cycle starts with the edge , with j taking any value between and . Since any such cycle can be formed only by adding to starting vertex pairs . Therefore, the length of the cycle (by counting twice) will be always an odd number. If the cycle starts with the edge , then the only difference from the previous case will be the addition of the pairs and/or arbitrarily many times. Hence, only cycles of odd length will be produced. Conversely, if the cycle starts with the chain or , then to close it at , the smallest required even length is .
- (b)
- Consider a primitive cycle that does not contain . Obviously, such a cycle does not contain or since these vertices have red edges connecting them all the way to . Additionally, this cycle cannot contain since is the only vertex (besides itself) with a directed edge to . This leaves 3 vertices: connected as . Therefore, this triple can only produce cycles when pairs and are added to a starting vertex. Therefore, no cycle of even length can be produced.
□
Now, observe that when the length, m, of path (7) is , it is comprised of distinct intervals and thus there are 2 additional intervals required to complete the periodic orbit of period . From path (7) and the rules (8), it follows that the relative distribution of the intervals is in one of the following 2 forms illustrated in Figure 7 and Figure 8. Call the two missing intervals and . There are slots in Figure 7 and Figure 8 where we can place each of these extra intervals for a total of pairs. However, since swapping the locations of and does not affect the analysis, let us consider the distribution given in Figure 8 in the upper triangular matrix (13), where indicates placing in position i and in position j.
Figure 7.
Relative positions of intervals in the sub-graph of length when is to the right of .
Figure 8.
Relative positions of intervals in the sub-graph of length when is to the left of .
The next lemma specifies all the entries in matrix (13) such that insertion of in can produce second minimal odd orbits.
Lemma 5.
Fix the entry point, i, for , then, to produce second minimal orbit, can only be placed in
- 1.
- position when ,
- 2.
- positions or for ,
- 3.
- and position when .
Proof.
Let for . Let the interval immediately to the left of be called , or the w-th distinct interval in path (7). From the relative positions of the intervals in Figure 3, it is clear that . As depicted in Figure 9, the intervals to the right of have a set path. maps only to , maps only to , etc. Note that while the exact points that these intervals map to might change upon the insertion of , the overall structure must remain the same in order to preserve path (7).
Figure 9.
Relative ordering when and is in position i.
However, this pattern can no longer be continued indefinitely for interval . must be mapped to , by definition. This implies that one end point of is mapped arbitrarily to the left of and the other endpoint is mapped arbitrarily to the right of . According to (8), cannot map to any odd interval greater than . Assuming that is not the rightmost interval, or in other words , then the endpoint of that maps to the right of must map to a point separating and . This could either be a point directly in between and or a new point between and , upon the insertion of .
Note that if , or in other words is the rightmost interval, then no longer exists. Rather than mapping to a point separating and , an endpoint of will just map to the right of .
While it is clear how one endpoint of will map to the right of , it is much less clear how an endpoint of will map to the left of . According to (9), cannot map to or any where and is even. Thus, the arbitrary point to the left of to which an endpoint of must map must be separating and . Thus, the missing interval must be inserted between and . Note that according to the previously mentioned positional notation, this includes all the positions , , …, , .
Suppose that the interval is inserted into a position to the left of . Assume, without any loss of generality, that the interval is inserted into position (between intervals and if , and between and if ), as the contradiction will be the same. The interval immediately to the right of has some trouble mapping to the interval indexed one greater than itself. In the situation where is placed in position , the interval immediately to the right of is , which has trouble mapping to . One endpoint of must map to the left of , while the other must map to the right of . Again, according to (9), cannot map to a lesser odd interval or . Thus, the only available point to the left of and to the right of is the point indexed or the left endpoint of . However, it is important to note that the largest indexed interval, , must also map back to . Furthermore, according to (9), cannot map to a lesser even interval, specifically including . Therefore, an endpoint of must map to the left of , but cannot map to the left of . The only point that fits this description is the one indexed . Thus, the point is already taken, and an endpoint of cannot map to the point indexed . Furthermore, there are no open points that are both to the right of and to the left of . This is an immediate contradiction, as it is now impossible for an endpoint of to map to the right of , making it impossible for to contain .
Now, suppose instead that . If this is the case, then is inserted between and . Again, the image of must contain only and . Thus, one endpoint of must map to the right of , but cannot map to the right of . Therefore, the left endpoint of must map to the point separating and . Now, must map to , but cannot map back to . Thus, one of the endpoints of must map to a point separating and . Both the left endpoint of of and an endpoint of must map to points separating and . There is only one point separating and , so this is an immediate contradiction.
Therefore, it is impossible for to be inserted to the left of position , because the interval immediately to the right of can no longer map to the interval indexed one greater than itself, in the case of . In the case of , a separate contradiction arises when both the left endpoint of of and an endpoint of must map to the singular point separating and . The only two possible positions of that can produce valid second minimal orbits when is inserted into position i, are the positions and .
Suppose that is inserted into position k. By (8), the image of must contain itself. This means, by definition, that one endpoint of must map to the right of itself and the other endpoint of must map to the left of itself. However, by (8), cannot map to . Thus, the endpoint of that maps to the right of itself must map to the left of . In other words, one endpoint of must map to a point separating and . By (8), the image of must contain . Again, this means that one endpoint of maps to the left of and the other endpoint of maps to the right of . However, by (9), the image of cannot contain . Thus, the endpoint of that maps to the left of cannot map to the left of . In other words, an endpoint of must map to points separating and . Both an endpoint of and an endpoint must map to points separating and . Note that, when was inserted into position k, and no longer shared an endpoint. Thus, the two endpoints that map to points separating and must necessarily be two different points. Thus, there must be at least two different points separating and . This can only be achieved by inserting between and , which is position . Or in other words, if is inserted into position k, a valid second minimal orbit can only be constructed if is inserted into position .
Finally, suppose that is inserted into position 1. There are two options here:
- is inserted arbitrarily to the left of .
- is inserted arbitrarily to the right of .
Suppose that is inserted arbitrarily to the left of . If is in any position j, where . By simply changing the notation, where becomes and becomes , we suddenly have the cases already addressed earlier in the proof, with being arbitrarily between and . Note that for none of the cases where , position 1 was not a valid position for . Thus, the only case that has not been considered is when both and are in position 1. For the sake of simplicity, assume that is the first interval, and is the interval between and .
It follows from (8) that the image of must contain only itself and . This is only possible if the left endpoint of , indexed , maps to the right endpoint of , which is indexed ; and the right endpoint of maps to the left endpoint of , indexed . By (8), must contain and no odd interval with a greater index, which is only possible if the left endpoint of , indexed k, maps to the right endpoint of , indexed . Furthermore, by (8), every even interval can contain only the odd interval indexed one greater than itself and no greater odd interval, and conversely, every odd interval can contain only the even interval indexed one greater than itself and no greater even interval. This fact forces the intervals to follow the structure depicted in [6]. This pattern continues until the left endpoint of maps to the right endpoint of and the left endpoint of maps to the right of . This construction yields Figure 10, where the solid red lines represent the Stefan-like structure present when and are both placed in Position 1.
Figure 10.
Fixed ordering for intervals through when both and are in position 1.
By (8), the image of must contain , but cannot map to a lesser even interval, specifically . Therefore, the left endpoint of must map somewhere to the left of but cannot map to the left of . In other words, it must map to a point separating and . The only point that meets this condition is indexed . Therefore, the left endpoint of must map to the point indexed , shown by the dotted red line in Figure 10.
By (8), the image of must contain . Thus, the right endpoint of must map to the left of . However, note if the right endpoint of maps immediately to the left of to the point indexed 3, then two closed sub-orbits of length 2 and of the form are formed. Thus, the right endpoint of can map either to the point indexed 1 or the point indexed 2. Investigating both of these cases individually leads to quick contradictions.
Suppose that the right endpoint of maps to the left endpoint of or the point indexed 1. The only two ‘open’ points, or points that do not already have a point mapping to them, are the ones indexed 2 and 3. Because point 2 cannot map to itself, it must map to the only other open point, indexed 3. The final point, indexed 1, can now only map to point 2, completing the cyclic permutation. However, this can instantly be shown to be an invalid cyclic permutation due to the presence of a 3 orbit of the form .
Since the left endpoint of cannot map to the point indexed 1, the case where the left endpoint of maps to the point indexed 2 is considered. Now, the only two open points are the ones indexed 1 and 3. Because point 1 cannot map to itself, it must map to the only other open point, indexed 3. The final point, indexed 2, can now only map to point 1, completing the cyclic permutation. However, this can instantly be shown to be an invalid cyclic permutation due to the presence of a 3 orbit of the form .
This exhausts all possible options for points that the right endpoint of can map to, proving that it is impossible to form a valid cyclic permutation when and are both in position 1. Furthermore, all cases where is in position 1 and is in an arbitrary position j, where have been proven to lead to contradictions. Thus, any case where is in position 1 and is inserted arbitrarily to the left of cannot lead to the construction of a valid second minimal odd orbit.
A valid second minimal odd orbit for the case where is in position 1 can only be constructed when is inserted arbitrarily to the right of . Consider the case when is inserted between and . Now, assume without any loss of generality that is inserted to the position immediately to the left of , as the contradiction will be the same. The interval immediately to the right of , in this case , has trouble mapping to the interval indexed one greater than itself, in this case . While it is clear how an endpoint of will map to the left of , it is much less clear how an endpoint will map to the right of . Again, according to (9), the image of cannot contain . Thus, an endpoint of must map to a point separating and . The only point that fits this description is the one indexed . However, it is important to note that the largest indexed interval, , must also map back to . Furthermore, according to (9), cannot map to a lesser even interval, specifically including . Therefore, an endpoint of must map to the left of but cannot map to the left of . The only point that fits this description is the one indexed , which is already taken. This is an immediate contradiction, as both an endpoint of and an endpoint of must map to the point indexed . Therefore, it is impossible for to be placed between and . The only possible way to make the construction of valid second minimal odd orbits possible when is placed in position one is by placing into the position or immediately to the right of .
To complete the proof, we show there are no valid settings for , . Note that (13) only includes pairs where , if . Thus, both i and j are to the right of . Assume for the sake of simplicity that the interval closer to is the one labeled . All intervals between and will map according to the minimal structure (2) [2], as described earlier. The Stefan structure comes to an end when the interval immediately to the left of , maps to . Now, the interval to the right of , has trouble mapping to the interval . cannot map to according to the rules (8) and (9), so one of its endpoints must map to a point separating and . The only such point is k. However, as discussed before, k must be mapped to by an endpoint of the interval . Thus, there are no open points between and . Note that because is inserted to the right of , it is impossible for an endpoint of to map to the right of . Thus, it is impossible for to contain when both and are to the right of , which is a clear contradiction. □
Lemma 6.
Placing and in setting produces exactly 2 second minimal orbits. These are given in listings (14) and (15) and the corresponding digraphs are presented in Figure 11 and Figure 12, respectively.
Figure 11.
Digraph for Cyclic Permutation of (14) from Setting (1, 2k − 1).
Figure 12.
Digraph for Cyclic Permutation of (15) from Setting (1, 2k − 1).
Proof.
Having inserted in position , we have the full interval distribution given in Figure 13. Then, using the path (7) and the rules in (8) and (9), we observe that the images of the elements of the cycle from 4 to are uniquely defined following a Stefan structure as demonstrated in (16).
Figure 13.
Complete interval for case when length is with and missing intervals are at setting .
The alteration appears only in images of the elements . By using the path (7) and the rules in (8) and (9) again, we construct the potential cyclic permutation (17) and analyze which of the available choices lead to valid second minimal odd orbits.
- Case (1): Choosing ; this leads to a valid second minimal orbit with the topological structure min-max-min and the associated digraph is presented in Figure 11 and the cyclic permutation is listed in (14). Next, we analyze the digraph to show that there are no primitive cycles of even length , which would imply by Straffin’s lemma an existence of odd periodic orbit of length . From Lemm 3, it then follows that the P-linearization of the orbit (14) presents an example of a continuous map with a second minimal -orbit.
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since , any such cycle can be formed only by adding to starting vertex pairs , . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is .
- (b)
- Consider primitive cycles that do not contain , but contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since any such cycle can be formed only by adding to starting vertex pairs . Therefore, the length of the cycle (by counting twice) will always be an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is . Finally, it is easy to see that by excluding and from the cycle, due to the red edges, all the vertices but must also be excluded, and cycle at is the only possibility.
- Case : ; this leads to a valid second minimal orbit with the topological structure min-max and the associated digraph is presented in Figure 12 and the cyclic permutation is listed in (15). Next, we prove as in previous case that there are no primitive cycles of even length , and, therefore, according to Lemms 3, P-linearization of the orbit (14) presents an example of a continuous map with a second minimal -orbit.
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since any such cycle can be formed only by adding to starting vertex pairs . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is .
- (b)
- Consider primitive cycles that do not contain , but contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since any such cycle can be formed only by adding to starting vertex pairs . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is . Finally, it is easy to see that by excluding and from the cycle, due to the red edges, all the vertices but must be also excluded, and cycle at is the only possibility.
- Case : . The produced cyclic permutation contains the subgraph . According to Straffin’s lemma this subgraph implies the existence of a period 3-orbit, which is a contradiction.
□
Lemma 7.
Placing and in setting produces exactly 3 second minimal orbits. These are given in listings (14), (18), and (19) and the corresponding digraphs are presented in Figure 11, Figure 14, and Figure 15, respectively.
Figure 14.
Digraph of cyclic permutation (18),
in setting (2, 2k − 1).
Figure 15.
Digraph of cyclic permutation (19),
in setting (2, 2k − 1).
Proof.
Having inserted in position and by using the path (7) and the rules in (8) and (9), we observe that the images of the elements of the cycle from 4 to are uniquely defined following a Stefan structure as demonstrated in (20).
The alteration appears only in images of the elements . By using the path (7) and the rules in (8) and (9) again, we construct the potential cyclic permutation (21) and analyze which of the available choices lead to valid second minimal odd orbits.
- If -suborbit , a contradiction.
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If , but we have a second minimal orbit given in (14) with topological structure min-max-min, observe that this is the same as (14) from setting , and so the settings share a cyclic permutation. This is expected since to move from setting to , only the location of is changed and so, in this particular case, the digraph remains unchanged as we simply swap the intervals and .
- This leads to a valid second minimal orbit with the topological structure max-min and the associated digraph is presented in Figure 14 and the cyclic permutation is listed in (18). Next, we prove that there are no primitive cycles of even length , and therefore according to Lemma 3, P-linearization of the orbit (18) presents an example of a continuous map with a second minimal -orbit.
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since and , any such cycle can be formed only by adding to starting vertex pairs , . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is .
- (b)
- Consider primitive cycles that do not contain . It is easy to see that by excluding from the cycle, due to the red edges, all the vertices but must also be excluded, and the cycle at is the only possibility.
- . This produces a second minimal orbit with topological structure max-min and the associated digraph is presented in Figure 15 and the cyclic permutation is listed in (19). As in previous cases, we prove that there are no primitive cycles of even length , and therefore according to Lemma 3, P-linearization of the orbit (19) presents an example of a continuous map with a second minimal -orbit.
- (a)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since (if ) and , , , , any such cycle can be formed only by adding to starting vertex pairs , , , Therefore, the length of the cycle (by counting twice) will always be an odd number. Conversely, if the cycle contains , then to close it at the smallest required even length is .
- (b)
- Consider primitive cycles that do not contain . It is easy to see that by excluding from the cycle, due to the red edges, all the vertices but must be also excluded, and a cycle at and a cycle formed by and are the only possibilities.
□
Lemma 8.
Placing and in setting produces exactly 4 second minimal orbits. These are listed in cyclic permutations (15), (18), (22), and (23) and the corresponding digraphs are presented in Figure 12, Figure 14, Figure 16, and Figure 17, respectively.
Figure 16.
Digraph of cyclic permutation (22),
in setting (2, 2k − 2).
Figure 17.
Digraph of cyclic permutation (23),
in setting (2, 2k − 2).
Proof.
Having inserted in position and by using the path (7) and the rules in (8) and (9), we observe that the images of the elements of the cycle from 5 to are uniquely defined following a Stefan structure as demonstrated in (24).
The alteration appears only in images of the elements . By using the path (7) and the rules in (8) and (9) again, we construct the potential cyclic permutation (25) and analyze which of the available choices lead to valid second minimal odd orbits.
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If , we have a second minimal orbit given in (15) with topological structure min-max, shared with setting .
- (c)
- If -suborbit , a contradiction.
- If
- (a)
- If and -suborbit , a contradiction.
- (b)
- If and , then for , we have the primitive subgraphLemma 2 implies the existence of a -periodic orbit, which is a contradiction. For , we have the subgraphwhich leads to a 3-orbit, a contradiction.
- (c)
- If -suborbit , a contradiction.
- (d)
- If , then for , we have the subgraphLemma 2 implies the existence of a -periodic orbit, which is a contradiction. For , we have the subgraphwhich leads to a 3-orbit, a contradiction.
- If
- (a)
- If and -suborbit , a contradiction.
- (b)
- If and , we have a second minimal orbit given in (18) with topological structure max-min, shared with setting .
- (c)
- If -suborbit , a contradiction.
- (d)
- If , we have a second minimal orbit given in (22) with topological structure max-min-max, and the associated digraph is presented in Figure 16. Next we prove as in previous lemma that there are no primitive cycles of even length , and therefore according to Lemma 3, P-linearization of the orbit (22) presents an example of a continuous map with a second minimal -orbit.
- i.
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since and , , any such cycle can be formed only by adding to starting vertex pairs , . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is .
- ii.
- Consider primitive cycles that do not contain . It is easy to see that by excluding from the cycle, due to the red edges, all the vertices but must be also excluded, and a cycle at and a cycle formed by and are the only possibilities.
- If
- (a)
- If and -suborbit , a contradiction.
- (b)
- If and -suborbit , a contradiction.
- (c)
- If , we have a second minimal orbit given in (23) with topological structure max-min-max, and the associated digraph is presented in Figure 17. Next, we prove as in previous cases that there are no primitive cycles of even length , and therefore according to Lemma 3, P-linearization of the orbit (23) presents an example of a continuous map with a second minimal -orbit.
- (i)
- Consider primitive cycles that contain . Without any loss of generality, choose as the starting vertex. First, assume that the cycle does not contain . Since any such cycle can be formed only by adding to starting vertex pairs . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then to close it at , the smallest required even length is .
- (ii)
- Consider primitive cycles that do not contain . It is easy to see that by excluding from the cycle, due to the red edges, all the vertices but must be also excluded, and a cycle at and a cycle formed by and are the only possibilities.
- (d)
- If -suborbit , a contradiction.
□
Lemma 9.
Each setting with and produces exactly 4 second minimal cycles listed in cyclic permutations (26), (27), (28), and (29). If , (26) repeats the cyclic permutation (23) revealed in Lemma 8. When , the cyclic permutation (29) and (10) from Lemma 4 are identical. The corresponding digraphs are presented in Figure 18, Figure 19, Figure 20, and Figure 21, respectively, when .
Figure 18.
Digraph of cyclic permutation (26),
in setting (i, j), 3 < i < k − 1.
Figure 19.
Digraph of cyclic permutation (27),
in setting (i, j), 3 < i < k − 1.
Figure 20.
Digraph of cyclic permutation (28),
in setting (i, j), 3 < i < k − 1.
Figure 21.
Digraph of cyclic permutation (29),
in setting (i, j), 3 < i < k − 1.
Proof.
We prove this by doing a case by case analysis of the general cyclic permutation listed in (30).
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If -suborbit , a contradiction.
- (c)
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If or we have the closed 2-suborbit . So we must have . Following the proof of Lemma 5, it follows that for , the digraph of the cyclic permutation contains a primitive subgraphand for , the digraph of the cyclic permutation contains a primitive subgraphboth of which have length . By Lemma 2, a periodic orbit of period must exist, which is a contradiction.
- (c)
- If or there is a period 4-suborbit , . Thus, . By repeating the argument of the previous case, we prove the existence of the -orbit, which is a contradiction.
- If
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If and -suborbit , a contradiction.
- (c)
Observe, as i varies between 3 and , the structure of the digraphs associated with the cyclic permutations changes. In particular, for a given cyclic permutation, varying i from 3 to shifts the region of variations from the right to left end of the digraph. We demonstrate this in Figure 22, Figure 23, Figure 24 and Figure 25. Note that in these subgraphs, with the exception of Figure 22a, where , we have .
Figure 22.
Portion with variations in digraphs of cyclic permutation (26), in setting .
Figure 23.
Portion with variations in digraphs of cyclic permutation (27), in setting .
Figure 24.
Portion with variations in digraphs of cyclic permutation (28), in setting .
Figure 25.
Portion with variations in digraphs of cyclic permutation (29), in setting .
Note that all four cyclic permutations are simple. Next, we analyze the digraphs to show that there are no primitive cycles of even length , which would imply by Straffin’s lemma, an existence of an odd periodic orbit of length . From Lemms 3, it then follows that the P-linearization of the orbits (26), (27), (28), and (29) present an example of a continuous map with a second minimal -orbit. The proof coincides with the similar proofs given in previous lemmas.
- Consider primitive cycles that contain . Without any loss of generality, choose a starting vertex as . First, assume that the cycle does not contain . Due to presence of red edges, any such cycle can be formed only by successfully adding to starting vertex pairs , where , . Therefore, the length of the cycle (by counting twice) will be always an odd number. Conversely, if the cycle contains , then, besides the new pair or there is a possibility to add just alone due to the loop at , and hence, to build a primitive subgraph of even length. However, the smallest required even length is , and, therefore, no odd orbits of a period smaller than can be produced.
- Consider primitive cycles that do not contain . Since and are only edges directed to , we have to exclude from the primitive cycle unless it is a loop at . However, then, any primitive cycle formed by the remaining intervals can be formed by adding some of the indicated pairs to the starting vertex, and, therefore, all are of odd length.
□
Lemma 10.
Each setting with and produces exactly 4 second minimal cycles listed in cyclic permutations (31), (32), (33), and (34). Cyclic permutation (32) repeats (28) from Lemma 9. If , (31) repeats the cyclic permutation (22) revealed in Lemma 8, and (34) repeats the cyclic permutation (19) revealed in Lemma 7. The corresponding digraphs are presented in Figure 26, Figure 27, Figure 28 and Figure 29, respectively.
Figure 26.
Digraph of cyclic permutation (31), in setting .
Figure 27.
Digraph of cyclic permutation (32), in setting .
Figure 28.
Digraph of cyclic permutation (33), in setting .
Figure 29.
Digraph of cyclic permutation (34), in setting .
Proof.
We prove this by doing a case by case analysis of the general cyclic permutation listed in (35).
- If -suborbit , a contradiction.
- If
- (a)
- (b)
- If -suborbit , a contradiction.
- (c)
- If and -suborbit , a contradiction.
- (d)
- If and . Following the proof of the Lemma 5, it follows that for , the digraph of the cyclic permutation contains a primitive subgraphand for , the digraph of the cyclic permutation contains a primitive subgraphboth of which have length . By Lemma 2, a periodic orbit of period must exist, which is a contradiction.
- If
- (a)
- (b)
- If -suborbit , a contradiction.
- (c)
- If and . This implies a cyclic permutation whose digraph contains a primitive subgraph of length . The proof coincides with the proof given above in the case (2d). By Lemma 2, a periodic orbit of period must exist, which is a contradiction.
- (d)
- If and -suborbit , a contradiction.
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If , we have a second minimal orbit given in (33) with topological structure max-min-max.
- (c)
- If and -suborbit , a contradiction.
- (d)
As i varies between 3 and , the structure of the digraphs associated with the cyclic permutations changes. In particular, for a given cyclic permutation, varying i from 3 to shifts the region of variations from the right to left end of the digraph. We demonstrate this in Figure 30, Figure 31, Figure 32 and Figure 33. Observe that Figure 24 and Figure 31 are identical. Note that in these subgraphs, with the exception of Figure 30 where , we have .
Figure 30.
Portion with variations in digraphs of cyclic permutation (31), in setting .
Figure 31.
Portion with variations in digraphs of cyclic permutation (32), in setting .
Figure 32.
Portion with variations in digraphs of cyclic permutation (33), in setting .
Figure 33.
Portion with variations in digraphs of cyclic permutation (34), in setting .
Note that all four cyclic permutations are simple. Finally, we aim to analyze the digraphs and demonstrate that there are no primitive cycles of even length , which would imply by Straffin’s lemma, an existence of an odd periodic orbit of length . From Lemms 3, it then follows that the P-linearization of the orbits (31), (32), (33), and (34) present an example of a continuous map with a second minimal -orbit. The proof coincides with the similar proof given in Lemma 9. □
Lemma 11.
Placing in relative positions produces exactly 4 second minimal cycles, listed in cyclic permutations (36), (37), (38), and (39). The corresponding digraphs are presented in Figure 34, Figure 35, Figure 36 and Figure 37, respectively.
Figure 34.
Digraph of cyclic permutation (36), in setting (k, k + 1).
Figure 35.
Digraph of cyclic permutation (37), in setting (k, k + 1).
Figure 36.
Digraph of cyclic permutation (38), in setting (k, k + 1).
Figure 37.
Digraph of cyclic permutation (39), in setting (k, k + 1).
Proof.
We prove this by doing a case by case analysis of the general cyclic permutation listed in (35). Note that in the frame of notation introduced in the proof of Lemma 5, we have ;
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If , then for we have the primitive subgraphof length . Lemma 2 implies the existence of -orbit, which is a contradiction.
- (c)
- If and , we have a second minimal orbit given in (36) with topological structure max-min-max-min-max.
- (d)
- If and -suborbit , a contradiction.
- If
- If -suborbit , a contradiction.
- If
- (a)
- If -suborbit , a contradiction.
- (b)
- If , then for we have the primitive subgraphof length which leads to contradiction as in case (1b).
- (c)
- If and , we have a second minimal orbit given in (39) with topological structure max-min-max-min-max.
- (d)
- If and -suborbit , a contradiction.
Note that all four cyclic permutations are simple. Finally, we aim to analyze the digraphs and demonstrate that there are no primitive cycles of even length , which would imply by Straffin’s lemma an existence of odd periodic orbit of length . From Lemma 3, it then follows that the P-linearization of the orbits (36), (37), (38), and (39) present an example of a continuous map with a second minimal -orbit. The proof coincides with the similar proof given in Lemma 9. □
Lemma 12.
Let be in setting for . For fixed i, this setting shares one cyclic permutation with the setting and another cyclic permutation with the setting . When , the setting shares a cyclic permutation with the case when from Lemma 4.
Proof.
The proof is by direct comparison. Note that if , the cyclic permutation (29) is transformed to (26) after substitution with . If , (26) repeats the cyclic permutation (23). Therefore, the setting shares one cyclic permutation with . We can also see that the cyclic permutations (28) and (32) are identical. So the setting also shares a cyclic permutation with the setting . When , the cyclic permutation (29) and (10) are identical. □
Lemma 13.
Let be in setting for . For fixed i, this setting shares one cyclic permutation with the setting and another cyclic permutation with the setting .
Proof.
The proof is once again by direct comparison. If , the substitution with in (27) implies the cyclic permutation (31) from Lemma 10. If , (31) repeats the cyclic permutation (22), revealed in Lemma 8. If , choose in the cyclic permutation (27) and observe that it is identical to (39). This proves the sharing with setting . Similarly, if the substitution with cyclic permutation (33) is transformed to the cyclic permutation (34). If (34) repeats the cyclic permutation (19), revealed in Lemma 7. If , then by choosing in (33), we see that it is identical to (37). This confirms the sharing with setting . □
The sharing mechanism provided in Lemmas 12 and 13 is illustrated in Figure 38. Each setting and , contain exactly 4 s minimal cyclic permutations, which are shared with neighboring settings. In particular, for setting , two cyclic permutations are inherited from its two neighbors immediately to the right, and another two are shared with neighbors immediately below. Observe that we have also demonstrated the sharing extending to the cases , , , and . To count all the different second minimal cyclic permutations, we start in the upper right corner of the table in Figure 39 and work our way down to the bottom left corner by successively moving down and left. Due to the sharing mechanism, the number of new second minimal cyclic permutations produced in each setting is equal to 2 (written as a superscript to the setting). There are columns, each with 4 distinct cycles, giving a total of distinct cyclic permutations. Adding the 1 remaining permutation from Lemma 4, we have the required number, , of second minimal cyclic permutations of period , unique up to an inverse. They are all of the simple positive type according to Definition 1. All the inverse cyclic permutations of the constructed orbits constitute all the simple negative-type second minimal -orbits. Finally, we count the different types of topological structures of all the positive-type second minimal orbits and present the results in Table 2. The inverse cyclic permutations have the same topological structures with “max” and “min” exchanged.
Figure 38.
The cyclic permutation sharing mechanism for settings and . Red arrows indicate cyclic permutations originating at a node and blue arrows indicate cyclic permutations shared from above.
Figure 39.
Demonstration of counting of distinct cyclic permutations per setting, here indicated with red numbers.
Table 2.
Counts for topological structure of second minimal odd periodic orbits. Green entries correspond to permutations in settings for with . Parentheses indicate permutations that may be shared.
5. Conclusions
This paper proves a conjecture on the second minimal odd periodic orbits with respect to Sharkovski ordering for the continuous endomorphisms on the real line. In 1964, in their celebrated paper, Sharkovski discovered a law of coexistence of periodic orbits of the continuous maps on the real line. The law generates a total ordering in shown in (1). The structure of the periodic orbits can be characterized through cyclic permutations and directed graphs of transitions or digraphs (Definitions 1 and 2). Remarkably, the structure of the periodic orbits is dictated by the location of the minimal period of the map in the Sharkovski ordering. Stefan (1977) [6] revealed that the minimal odd orbits have a unique cyclic permutation and digraph up to their inverses ((2) and Figure 1). Extending this work, the structure of all the minimal orbits are well understood [7,8]. In this paper, we present a full characterization of the second minimal odd orbits, i.e., orbits with a period being next to the minimal period of the map in the Sharkovski ordering. The main results are the following:
- Second minimal and minimal -orbits () are simple, meaning that elements on the right and left of the central element of the orbit are mapped to each other except one point. We call these positive type (or negative type) if the exceptional element is on the right (or on the left) of the central point. Cyclic permutations and digraphs of all the negative-type simple orbits are inverses of all the positive-type simple orbits, respectively.
- Simple positive-type second minimal -orbits are either Stefan orbits, or have one of the types, each with a unique digraph and cyclic permutation. Their inverses represent all second minimal -orbits of the simple negative type.
- The constructive proof presented in this paper revealed explicitly the cyclic permutations and digrahs of all second minimal -orbits (), as well as their topological structure (Table 1).
The new concept of second minimal orbits and its classification have an important application towards an understanding of the universal structure of the distribution of the periodic windows in the bifurcation diagram generated by the chaotic dynamics of nonlinear maps on the interval. In 1978, Feigenbaum discovered a universal transition mechanism to chaos through successive period doubling bifurcations for the one-parameter family of nonlinear maps with a single quadratic maximum. The revealed scenario of a transition from periodic to chaotic behavior gives a full characterization of the dynamical system in the range of the parameter not exceeding the critical value of the transition to chaos. There has been a long quest to understand the behavior of the dynamical system beyond the transition to chaotic range. A recent paper (Abdulla et al., 2017 [11]) revealed the universal law of the distribution of the periodic windows in the chaotic range of the parameter between the critical value of transition to chaos and the value when a stable 3-orbit appears for the first time. Remarkably, the pattern of distribution of the periodic windows is driven by Sharkovski ordering. In particular, it was revealed that the first appearance of all the odd orbits is always a minimal odd orbit, while the second appearance is the second minimal orbit with a Type I digraph. The reason for the relevance of Type 1 s minimal (2k + 1)-orbits, is due to the fact that the topological structure of the single maximum unimodal map is equivalent to the topological structure of the piecewise monotonic map associated with Type 1 s minimal (2k + 1)-orbits (Table 1).
Author Contributions
Conceptualization, U.G.A., N.H.I., M.U.A. and R.U.A.; Methodology, U.G.A., N.H.I., M.U.A. and R.U.A.; Software, N.H.I.; Validation, U.G.A., N.H.I., M.U.A. and R.U.A.; Formal analysis, U.G.A., N.H.I., M.U.A. and R.U.A.; Investigation, U.G.A., N.H.I., M.U.A. and R.U.A.; Writing—original draft, U.G.A., N.H.I., M.U.A. and R.U.A.; Writing—review and editing, U.G.A., N.H.I., M.U.A. and R.U.A.; Visualization, U.G.A., N.H.I., M.U.A. and R.U.A.; Supervision, U.G.A.; Project administration, U.G.A. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Data Availability Statement
Data shairing is not applicable to this article as no new data were created or analyzed in this study.
Conflicts of Interest
Author Rashad U. Abdulla was employed by HyAxiom Inc. The remaining authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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