
The present research applies an improved version of the modified Extended Direct Algebraic Method (mEDAM) called r+mEDAM to examine soliton phenomena in a notable mathematical model, namely the (2+1)-dimensional Nizhnik-Novikov-Veselov Model (NNVM), which possesses potential applications in exponentially localized structure interactions. The generalized hyperbolic and trigonometric functions are used to disclose a variety of soliton solutions, including kinks, anti-kink, bell-shaped and periodic soliton. Some 3D graphs are plotted for visual representations of these solutions which highlight their adaptability. The results provide a basis for practical usage and expansions to related mathematical models or physical systems. They also expand our understanding of the NNVM's dynamics, providing insights into its behavior and prospective applications.
Citation: Saima Noor, Azzh Saad Alshehry, Asfandyar Khan, Imran Khan. Analysis of soliton phenomena in (2+1)-dimensional Nizhnik-Novikov-Veselov model via a modified analytical technique[J]. AIMS Mathematics, 2023, 8(11): 28120-28142. doi: 10.3934/math.20231439
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The present research applies an improved version of the modified Extended Direct Algebraic Method (mEDAM) called r+mEDAM to examine soliton phenomena in a notable mathematical model, namely the (2+1)-dimensional Nizhnik-Novikov-Veselov Model (NNVM), which possesses potential applications in exponentially localized structure interactions. The generalized hyperbolic and trigonometric functions are used to disclose a variety of soliton solutions, including kinks, anti-kink, bell-shaped and periodic soliton. Some 3D graphs are plotted for visual representations of these solutions which highlight their adaptability. The results provide a basis for practical usage and expansions to related mathematical models or physical systems. They also expand our understanding of the NNVM's dynamics, providing insights into its behavior and prospective applications.
Let ψ be a simple, connected graph with vertex set V(ψ) and edge set E(ψ). The distance d(ρ1,ρ2), ρ1,ρ2∈V(ψ) is the length of shortest path between ρ1 and ρ2. Let Q={v1,v2,…,vj} be an ordered set of vertices of ψ. Let ρ1∈V(ψ), the representations denoted by r(ρ1|Q) is the j-tuple distances as (d(ρ1|v1),d(ρ1|v2),…,d(ρ1|vj)). If distinct vertices of ψ have distinct representation w.r.t. Q then Q is called the resolving set. The minimum number of j in the resolving set is known as the metric dimension of ψ and written as dim(ψ). Motivated by the problem of determining an intruder's location in a network in a unique way, Slater introduced the definition of metric dimension in [27] and later independently by Harary and Melter in [11]. The concept of resolving set, metric basis and metric dimension appeared in the literature [4,6,8,9,10,12,15,19,28,30,31].
A partition of a set is collection of its subsets, no pair of which overlap, such that the union of all the subsets is the whole set and partition dimension is related to the partitioning of the vertex set V(Ω) and resolvability. The partition dimension is a generalized variant of matric dimension. Another type of dimension of a graph, is called partition dimension. Let Γ={Γ1,Γ2…,Γj} and r(ρ1|Γ)={d(ρ1,Γ1),d(ρ1,Γ2),…,d(ρ1,Γj)} are named as j-ordered partition of vertices and j-tuple representations respectively. If the representations of every ρ1 in V(ψ) w.r.t. Γ is different, then Γ is the resolving partition of the vertex set and the minimum count of the resolving partition set of V(ψ) is named as the partition dimension of ψ and it is represented by pd(ψ) [7]. The problem of determining the resolving set of a graph is NP-hard [20]. As, the problem of finding the partition dimension is a generalize version of metric dimension, therefore partition dimension is also a NP-complete problem. It is natural to think that there is a relation between metric and partition dimension, [7] proved for any non-trivial connected graph ψ,
pd(ψ)≤dim(ψ)+1. | (1.1) |
In [22], fullerene graph of chemical structure is discussed and proved that the graph has constant and bounded partition dimension. For more and interesting results on constant partition dimension can see [16,21,24]. To find the exact value of partition dimension of a graph is not easy therefore, various results on the bounds of the partition dimension are discussed in literature, such as the partition dimension of Cartesian product operation on different graphs are studies and provided extensive bounds on partition dimension [29]. In [1] different bounds of partition dimension of subdivision of different graphs are discussed. In [25,26] provide bounds of partition dimension of tree and uni-cyclic graphs in the form of subgraphs.
The applications of partition resolving sets can be found in different fields such as robot navigation [19], Djokovic-Winkler relation [9], strategies for the mastermind game [10], network discovery and verification [5], in chemistry for representing chemical compounds [17,18] and in problems of pattern recognition and image processing, some of which involve the use of hierarchical data structures [23] for more applications see [6,11]. Following theorems are very helpful in finding the partition dimension of a graph.
Theorem 1.1. [7] Let Γ be a resolving partition of V(ψ) and ρ1,ρ2∈V(ψ). If d(ρ1,z)=d(ρ2,z) for all vertices z∈V(ψ)∖(ρ1,ρ2), then ρ1,ρ2 belong to different classes of Γ.
Theorem 1.2. [7] Let ψ be a simple and connected graph, then
● pd(ψ) is 2 iff ψ is a path graph
● pd(ψ) is n iff ψ is a complete graph,
Let R be a family of connected graphs Gn:R=(Gn)n≥1, where |V(ψ)|=λ(n) and limn→∞λ(n)=∞. If there exists a constant α≥1 such that pd(ψ)≤α,n≥1, then R has bounded partition dimension otherwise unbounded. Imran et al. [14] studied the metric dimension of Rpn, Dpn, and Qpn, convex polytopes which motivates us to find the partition dimension of same families of convex polytopes. In this paper, the partition dimension of same families of convex polytopes are studied. We determine the partition dimension of Rpn, in second section. In the third section, the partition dimension of the graph Dpn of a convex polytope with pendent edges is presented. The fourth section remains for the partition dimension of the graph Qpn.
The convex polytope Rpn (p for pendant edges) is a planar graph and obtained from the convex polytope Rn defined in [13]. If we attach a pendant edge at each vertex of outer layer of Rn then we obtained a new planer graph Rpn as shown in Figure 1. The vertex set of Rpn, V(RPn)={V(Rn)}∪{xα:1≤α≤n} and edge set of Rpn, E(RPn)={E(Rn)}∪{wαxα:1≤α≤n}.
For calculation, {uα:1≤α≤n} represents the inner cycle, the cycle induced by {vα:1≤α≤n} is interior cycle, exterior cycle containing {wα:1≤α≤n} set of vertices and pendant vertices named {xα:1≤α≤n}.
Theorem 2.1. Let Rpn be a polytopes with n≥6. Then pd(Rpn)≤4.
Proof. We splits the proof into following two cases.
Case 1: When n=2β,β≥3,β∈N. We partition the vertices of Rpn into four partition resolving sets Θ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Rpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertex of Rpn have different representation w.r.t. resolving set Γ, then pd(Rpn)≤4. We give the representations of all vertices w.r.t. resolving partition set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If β+2≤α≤2β, then r(uβ|Γ)=(2β−α+1,2β−α+2,α−β−1,0). There are no two vertices have same representation in inner cycle of Rpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If α=1, then r(vβ|Γ)=(1,1,β,0). If 2≤α≤β, then r(vβ|Γ)=(α,α−1,β−α+1,0). If α=β+1, then r(vβ|Γ)=(β,β,1,0). If β+2≤α≤2β, then r(vβ|Γ)=(2β−α+1,2β−α+2,α−β,0). There are also no two vertices have same representation in interior cycle of Rpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If α=1, then r(wβ|Γ)=(2,2,β+1,0). If 2≤α≤β+1, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+2, then r(wβ|Γ)=(β+1,β+1,2,0). If β+3≤α≤2β, then r(wβ|Γ)=(2β−α+2,2β−α+3,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Rpn. The representations of pendant vertices w.r.t. Γ are shown in Table 1. Again we can see that there are no two vertices have same representation of pendant vertices of Rpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
It is easy to verify that all the vertices of Rpn have unique representation w.r.t. resolving partition Γ. Its means we can resolve the vertices of Rpn into four partition resolving sets, when n is even.
Case 2: When n=2β+1,β≥3,β∈N. Again we resolve the vertices of Rpn into four partition resolving sets Γ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Rpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertices of Rpn have different representation w.r.t. resolving set Γ, then pd(Rpn)≤4. {We give the representations of all vertices Γ4 w.r.t. resolving set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If α=β+2, then r(uβ|Γ)=(β,β,1,0). If β+3≤α≤2β+1, then r(uβ|Γ)=(2β−α+2,2β−α+3,α−β−1,0). There are no two vertices have same representation in inner cycle of Rpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If α=1, then r(vβ|Γ)=(1,1,β,0). If 2≤α≤β, then r(vβ|Γ)=(α,α−1,β−α+1,0). If α=β+1, then r(vβ|Γ)=(β+1,β,1,0). If β+2≤α≤2β+1, then r(vβ|Γ)=(2β−α+2,2β−α+3,α−β,0). There are also no two vertices have same representation in interior cycle of Rpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are: If α=1, then r(wβ|Γ)=(2,2,β+1,0). If 2≤α≤β, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+1, then r(wβ|Γ)=(β+2,β+1,2,0). If β+2≤α≤2β+1, then r(wβ|Γ)=(2β−α+3,2β−α+4,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Rpn.
The pendant vertices having the representations w.r.t. Γ shown in Table 2. Again we can see that there are no two vertices have same representation of pendant vertices of Rpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+3 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
It is easy to verify that all the vertices of Rpn have unique representation w.r.t. resolving partition Γ. Its means we can also resolve the vertices of Rpn into four partition resolving sets, when n is odd.
We note that from Case 1 and 2, there are no two vertices having the same representations implying that pd(Rpn)≤4.
The convex polytope DPn is a planar graph and if we attach a pendant edge at each vertex of outer cycle of Dn [2] then we obtained a new plane graph DPn as shown in Figure 2. The vertex and edge set V(DPn)={V(Dn)}∪{yα:1≤α≤n}, E(DPn)={E(Dn)}∪{xαyα:1≤α≤n} are respectively. For calculation, {uα:1≤α≤n} represents the inner cycle, the cycle induced by {vα:1≤α≤n} is interior cycle, exterior cycle containing {wα:1≤α≤n} set of vertices, {xα:1≤α≤n} labeled as outer cycle and pendant vertices named for {yα:1≤α≤n}.
Theorem 3.1. Let DPn be a polytopes with n≥6. Then pd(DPn)≤4.
Proof. We split the proof of above theorem into following two cases.
Case 1: When n=2β,β≥3,β∈N. We partition the vertices of Dpn into four partition sets Γ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Dpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertices of Dpn have different representation w.r.t. resolving set Γ, then pd(Dpn)≤4. We give the representations of all vertices Γ4 w.r.t. resolving set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If β+2≤α≤2β, then r(uβ|Γ)=(2β−α+1,2β−α+2,α−β−1,0). There are no two vertices have same representation in inner cycle of Dpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If α=1, then r(vβ|Γ)=(1,2,β+1,0). If 2≤α≤β, then r(vβ|Γ)=(α,α−1,β−α+2,0). If α=β+1, then r(vβ|Γ)=(β,β,1,0). If β+2≤α≤2β, then r(vβ|Γ)=(2β−α+2,2β−α+3,α−β,0). There are also no two vertices have same representation in interior cycle of Dpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If α=1, then r(wβ|Γ)=(2,2,β+1,0). If 2≤α≤β, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+1, then r(wβ|Γ)=(β+1,β+1,2,0). If β+2≤α≤2β, then r(wβ|Γ)=(2β−α+2,2β−α+3,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Dpn.
The vertices on outer cycle and pendant vertices having the representations w.r.t. Γ as shown in Tables 3 and 4. Again we can see that there are no two vertices have same representation in outer cycle and pendant vertices of Dpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β−1 | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
It is easy to verify that all the vertices of Dpn have unique representation w.r.t. resolving partition Γ. Its means we can resolve the vertices of Dpn into four partition resolving sets, when n is even.
Case 2: When n=2β+1,β≥3,β∈N. Again we resolve the vertices of Dpn into four partition resolving sets Γ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Dpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertices of Dpn have different representation w.r.t. resolving set Γ, then pd(Dpn)≤4. We give the representations of all vertices Γ4 w.r.t. resolving set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If α=β+2, then r(uβ|Γ)=(β,β,1,0). If β+3≤α≤2β+1, then r(uβ|Γ)=(2β−α+1,2β−α+2,α−β−1,0). There are no two vertices have same representation in inner cycle of Dpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If α=1, then r(vβ|Γ)=(1,2,β+1,0). If 2≤α≤β+1, then r(vβ|Γ)=(α,α−1,β−α+2,0). If α=β+2, then r(vβ|Γ)=(β+1,β+1,2,0). If β+3≤α≤2β+1, then r(vβ|Γ)=(2β−α+2,2β−α+3,α−β,0). There are also no two vertices have same representation in interior cycle of Dpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If α=1, then r(wβ|Γ)=(2,2,β+1,0). If 2≤α≤β, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+1, then r(wβ|Γ)=(β+2,β+1,2,0). If β+2≤α≤2β+1, then r(wβ|Γ)=(2β−α+3,2β−α+4,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Dpn.
The vertices on outer cycle and pendant vertices having the representations w.r.t. Γ as shown in Tables 5 and 6. Again we can see that there are no two vertices have same representation in outer cycle and pendant vertices of Dpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 4 | 4 | β+3 | 0 |
xα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
xα: α=β+1 | β+3 | β+3 | 4 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |
It is easy to verify that all the vertices of Dpn have unique representation w.r.t. resolving partition Γ. Its means we can also resolve the vertices of Dpn into four partition resolving sets, when n is odd.
We note that from Case 1 and 2, there are no two vertices having the same representations implying that pd(Tpn)≤4.
The convex polytope QPn is a planar graph and If we attach a pendant edge at each vertex of outer cycle of Qn [3] then we obtained a new plane graph QPn as shown in Figure 3. The vertex and edge set V(QPn)={V(αn)}∪{yα:1≤α≤n}, E(QPn)={E(Qn)}∪{xαyα:1≤α≤n} are respectively.
For convenience, {uα:1≤α≤n} represents the inner cycle, the cycle induced by {vα:1≤α≤n} is interior cycle, exterior cycle containing {wα:1≤α≤n} set of vertices, {xα:1≤α≤n} are exterior vertices, and pendant vertices named for {yα:1≤α≤n}.
Theorem 4.1. Let QPn be a polytopes with n≥6. Then pd(QPn)≤4.
Proof. Case 1: When n=2β,β≥3,β∈N. We partition the vertices of Qpn into four partition resolving sets Γ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Qpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertices of Qpn have different representation w.r.t. resolving set Γ, then pd(Qpn)≤4. We give the representations of all vertices Γ4 w.r.t. resolving set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If β+2≤α≤2β, then r(uβ|Γ)=(2β−α+1,2β−α+2,α−β−1,0). There are no two vertices have same representation in inner cycle of Qpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(1,2,α+1,0). If 2≤α≤β, then r(vβ|Γ)=(α,α−1,β−α+2,0). If β+2≤α≤2β, then r(vβ|Γ)=(2β−α+2,2β−α+3,α−β,0). There are also no two vertices have same representation in interior cycle of Qpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(2,2,α+1,0). If 2≤α≤β, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+1, then r(vβ|Γ)=(α+1,α+1,2,0). If β+2≤α≤2β, then r(wβ|Γ)=(2β−α+2,2β−α+3,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Qpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(3,3,α+2,0). If 2≤α≤β, then r(wβ|Γ)=(α+2,α+1,β−α+3,0). If α=β+1, then r(vβ|Γ)=(α+2,α+2,3,0). If β+2≤α≤2β, then r(wβ|Γ)=(2β−α+3,2β−α+4,α−β+2,0). Again there are no two vertices have same representation also in exterior cycle of Qpn.
The pendant vertices having the representations w.r.t. Γ as shown in Table 7. Again we can see that there are no two vertices have same representation in pendant vertices of Qpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
It is easy to verify that all the vertices of Qpn have unique representation w.r.t. resolving partition Γ. Its means we can resolve the vertices of Qpn into four partition resolving sets, when n is even.
Case 2: When n=2β+1,β≥3,β∈N. Again we resolve the vertices of Qpn into four partition resolving sets Γ={Γ1,Γ2,Γ3,Γ4} where Γ1={u1}, Γ2={u2}, Γ3={uβ+1} and Γ4={∀V(Qpn)|∉{Γ1,Γ2,Γ3}}. It suffice to show that if every vertices of Qpn have different representation w.r.t. resolving set Γ, then pd(Qpn)≤4. We give the representations of all vertices Γ4 w.r.t. resolving set Γ are following.
The vertices on inner cycle having the representations w.r.t. Γ which are:
If 3≤α≤β, then r(uβ|Γ)=(α−1,α−2,β−α+1,0). If α=β+2, then r(uβ|Γ)=(β,β,1,0). If β+3≤α≤2β+1, then r(uβ|Γ)=(2β−α+1,2β−α+2,α−β−1,0). There are no two vertices have same representation in inner cycle of Qpn.
The vertices on interior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(1,2,α+1,0). If 2≤α≤β, then r(vβ|Γ)=(α,α−1,β−α+2,0). If α=β+2, then r(vβ|Γ)=(β+1,β+1,2,0). If β+3≤α≤2β+1, then r(vβ|Γ)=(2β−α+2,2β−α+3,α−β,0). There are also no two vertices have same representation in interior cycle of Qpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(2,2,α+1,0). If 2≤α≤β, then r(wβ|Γ)=(α+1,α,β−α+2,0). If α=β+1, then r(wβ|Γ)=(β+2,β+1,2,0). If β+2≤α≤2β+1, then r(wβ|Γ)=(2β−α+3,2β−α+4,α−β+1,0). Again there are no two vertices have same representation also in exterior cycle of Qpn.
The vertices on exterior cycle having the representations w.r.t. Γ which are:
If β=1, then r(vβ|Γ)=(3,3,α+2,0). If 2≤α≤β, then r(wβ|Γ)=(α+2,α+1,β−α+3,0). If α=β+1, then r(wβ|Γ)=(β+2,β+2,3,0). If β+2≤α≤2β+1, then r(wβ|Γ)=(2β−α+4,2β−α+5,α−β+2,0). Again there are no two vertices have same representation also in exterior cycle of Qpn.
The pendant vertices having the representations w.r.t. Γ as shown in Table 8. Again we can see that there are no two vertices have same representation in pendant vertices of Qpn.
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+4 | β+3 | 4 | 0 |
yα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |
It is easy to verify that all the vertices of Qpn have unique representation w.r.t. resolving partition Γ. Its means we can also resolve the vertices of Qpn into four partition resolving sets, when n is odd.
We note that from Case 1 and 2, there are no two vertices having the same representations implying that pd(Upn)≤4.
The core of the problem of the partition dimension is deciding the resolving partition set for a graph. In this paper, we have studies the partition dimension of some families of convex polytopes graph such as Rpn, Dpn and Qpn, which are obtained from the convex polytopes by adding a pendant edge at each vertex of outer cycle. In this research work, we have proved that partition dimension of these convex polytopes are bounded. Consequently, we propose the following open problems.
Conjecture 5.1. The following equalities hold:
pd(Rpn)=pd(Dpn)=pd(Qpn)=4 |
The authors declare there is no conflict of interest.
[1] |
K. Xu, Y. Guo, Y. Liu, X. Deng, Q. Chen, Z. Ma, 60-GHz compact dual-mode on-chip bandpass filter using GaAs technology, IEEE Electr. Device L., 42 (2021), 1120–1123. https://doi.org/10.1109/LED.2021.3091277 doi: 10.1109/LED.2021.3091277
![]() |
[2] |
H. Khan, R. Shah, P. Kumam, M. Arif, Analytical solutions of fractional-order heat and wave equations by the natural transform decomposition method, Entropy, 21 (2019), 597. https://doi.org/10.3390/e21060597 doi: 10.3390/e21060597
![]() |
[3] |
Z. Li, K. Wang, W. Li, S. Yan, F. Chen, S. Peng, Analysis of surface pressure pulsation characteristics of centrifugal pump magnetic liquid sealing film, Front. Energy, 10 (2022), 937299. https://doi.org/10.3389/fenrg.2022.937299 doi: 10.3389/fenrg.2022.937299
![]() |
[4] |
H. Khan, R. Shah, J. F. G. Aguilar, D. Baleanu, P. Kumam, Travelling waves solution for fractional-order biological population model, Math. Model. Nat. Pheno., 16 (2021), 32. https://doi.org/10.1051/mmnp/2021016 doi: 10.1051/mmnp/2021016
![]() |
[5] |
Z. Xiao, H. Fang, H. Jiang, J. Bai, V. Havyarimana, H. Chen, et al., Understanding private car aggregation effect via spatio-temporal analysis of trajectory data, IEEE T. Cybernetics, 53 (2023), 2346–2357. https://doi.org/10.1109/TCYB.2021.3117705 doi: 10.1109/TCYB.2021.3117705
![]() |
[6] | M. J. Ablowitz, P. A. Clarkson, Solitons, nonlinear evolution equations and inverse scattering, Cambridge University Press, 149 (1991). https://doi.org/10.1017/CBO9780511623998 |
[7] |
G. F. Yu, H. W. Tam, A vector asymmetrical NNV equation: Soliton solutions, bilinear Bäcklund transformation and Lax pair, J. Math. Anal. Appl., 344 (2008), 593–600. https://doi.org/10.1016/j.jmaa.2008.02.057 doi: 10.1016/j.jmaa.2008.02.057
![]() |
[8] | V. B. Matveev, M. A. Salle, Darboux transformations and solitons, Berlin: Springer, 17 (1991). https://doi.org/10.1007/978-3-662-00922-2 |
[9] |
Y. L. Ma, Y. L. Li, Y. Y. Fu, A series of the solutions for the Heisenberg ferromagnetic spin chain equation, Math. Method. Appl. Sci., 41 (2018), 3316–3322. https://doi.org/10.1002/mma.4818 doi: 10.1002/mma.4818
![]() |
[10] |
Y. Ma, B. Li, C. Wang, A series of abundant exact travelling wave solutions for a modified generalized Vakhnenko equation using auxiliary equation method, Appl. Math. Comput., 211 (2009), 102–107. https://doi.org/10.1016/j.amc.2009.01.036 doi: 10.1016/j.amc.2009.01.036
![]() |
[11] |
B. Q. Li, Y. L. Ma, Periodic solutions and solitons to two complex short pulse (CSP) equations in optical fiber, Optik, 144 (2017), 149–155. https://doi.org/10.1016/j.ijleo.2017.06.114 doi: 10.1016/j.ijleo.2017.06.114
![]() |
[12] |
B. Q. Li, Y. L. Ma, Rich soliton structures for the Kraenkel-Manna-Merle (KMM) system in ferromagnetic materials, J. Supercond. Nov. Magn., 31 (2018), 1773–1778. https://doi.org/10.1007/s10948-017-4406-9 doi: 10.1007/s10948-017-4406-9
![]() |
[13] |
B. Li, Y. Ma, The non-traveling wave solutions and novel fractal soliton for the (2+1)-dimensional Broer-Kaup equations with variable coefficients, Commun. Nonlinear Sci., 16 (2011), 144–149. https://doi.org/10.1016/j.cnsns.2010.02.011 doi: 10.1016/j.cnsns.2010.02.011
![]() |
[14] |
M. Zhang, Y. L. Ma, B. Q. Li, Novel loop-like solitons for the generalized Vakhnenko equation, Chinese Phys. B, 22 (2013), 030511. https://doi.org/10.1088/1674-1056/22/3/030511 doi: 10.1088/1674-1056/22/3/030511
![]() |
[15] |
M. S. Osman, Nonlinear interaction of solitary waves described by multi-rational wave solutions of the (2+1)-dimensional Kadomtsev-Petviashvili equation with variable coefficients, Nonlinear Dynam., 87 (2017), 1209–1216. https://doi.org/10.1007/s11071-016-3110-9 doi: 10.1007/s11071-016-3110-9
![]() |
[16] |
H. I. A. Gawad, Towards a unified method for exact solutions of evolution equations. An application to reaction diffusion equations with finite memory transport, J. Stat. Phys., 147 (2012), 506–518. https://doi.org/10.1007/s10955-012-0467-0 doi: 10.1007/s10955-012-0467-0
![]() |
[17] | R. Hirota, The direct method in soliton theory, Cambridge University Press, 155 (2004). https://doi.org/10.1017/CBO9780511543043 |
[18] |
B. Q. Li, Y. L. Ma, Multiple-lump waves for a (3+1)-dimensional Boiti-Leon-Manna-Pempinelli equation arising from incompressible fluid, Comput. Math. Appl., 76 (2018), 204–214. https://doi.org/10.1016/j.camwa.2018.04.015 doi: 10.1016/j.camwa.2018.04.015
![]() |
[19] |
Y. L. Ma, B. Q. Li, Mixed lump and soliton solutions for a generalized (3+1)-dimensional Kadomtsev-Petviashvili equation, AIMS Math., 5 (2020), 1162–1176. https://doi.org/10.3934/math.2020080 doi: 10.3934/math.2020080
![]() |
[20] |
Y. L. Ma, A. M. Wazwaz, B. Q. Li, New extended Kadomtsev-Petviashvili equation: Multiple soliton solutions, breather, lump and interaction solutions, Nonlinear Dynam., 104 (2021), 1581–1594. https://doi.org/10.1007/s11071-021-06357-8 doi: 10.1007/s11071-021-06357-8
![]() |
[21] |
C. F. Wei, New solitary wave aolutions for the fractional Jaulent-Miodek hierarchy model, Fractals, 2023, 2350060. https://doi.org/10.1142/S0218348X23500603 doi: 10.1142/S0218348X23500603
![]() |
[22] |
S. M. M. Alizamini, H. Rezazadeh, K. Srinivasa, A. Bekir, New closed form solutions of the new coupled Konno-Oono equation using the new extended direct algebraic method, Pramana, 94 (2020), 1–12. https://doi.org/10.1007/s12043-020-1921-1 doi: 10.1007/s12043-020-1921-1
![]() |
[23] |
D. Chen, Q. Wang, Y. Li, Y. Li, H. Zhou, Y. Fan, A general linear free energy relationship for predicting partition coefficients of neutral organic compounds, Chemosphere, 247 (2020), 125869. https://doi.org/10.1016/j.chemosphere.2020.125869 doi: 10.1016/j.chemosphere.2020.125869
![]() |
[24] |
M. B. Hossen, H. O. Roshid, M. Z. Ali, Characteristics of the solitary waves and rogue waves with interaction phenomena in a (2+1)-dimensional Breaking Soliton equation, Phys. Lett. A, 382 (2018), 1268–1274. https://doi.org/10.1016/j.physleta.2018.03.016 doi: 10.1016/j.physleta.2018.03.016
![]() |
[25] |
F. Huang, X. Y. Tang, S. Y. Lou, Exact solutions for a higher-order nonlinear Schrödinger equation in atmospheric dynamics, Commun. Theor. Phys., 45 (2006), 573. https://doi.org/10.1088/0253-6102/45/3/039 doi: 10.1088/0253-6102/45/3/039
![]() |
[26] |
Z. Wu, J. Cao, Y. Wang, Y. Wang, L. Zhang, J. Wu, hPSD: A Hybrid PU-learning-based spammer detection model for product reviews, IEEE T. Cybernetics, 50 (2020), 1595–1606. https://doi.org/10.1109/TCYB.2018.2877161 doi: 10.1109/TCYB.2018.2877161
![]() |
[27] |
W. Q. Peng, S. F. Tian, T. T. Zhang, Analysis on lump, lumpoff and rogue waves with predictability to the (2+1)-dimensional B-type Kadomtsev-Petviashvili equation, Phys. Lett. A, 382 (2018), 2701–2708. https://doi.org/10.1016/j.physleta.2018.08.002 doi: 10.1016/j.physleta.2018.08.002
![]() |
[28] |
H. Khan, S. Barak, P. Kumam, M. Arif, Analytical solutions of fractional Klein-Gordon and gas dynamics equations, via the (G'/G)-expansion method, Symmetry, 11 (2019), 566. https://doi.org/10.3390/sym11040566 doi: 10.3390/sym11040566
![]() |
[29] |
H. Khan, D. Baleanu, P. Kumam, J. F. Al-Zaidy, Families of travelling waves solutions for fractional-order extended shallow water wave equations, using an innovative analytical method, IEEE Access, 7 (2019), 107523–107532. https://doi.org/10.1109/ACCESS.2019.2933188 doi: 10.1109/ACCESS.2019.2933188
![]() |
[30] |
H. Yasmin, N. H. Aljahdaly, A. M. Saeed, R. Shah, Investigating symmetric soliton solutions for the fractional coupled Konno-Onno system using improved versions of a novel analytical technique, Mathematics, 11 (2023), 2686. https://doi.org/10.3390/math11122686 doi: 10.3390/math11122686
![]() |
[31] |
R. Meng, X. Xiao, J. Wang, Rating the crisis of online public opinion using a multi-level index system, Int. Arab J. Inf. Techn., 19 (2022), 597–608. https://doi.org/10.34028/iajit/19/4/4 doi: 10.34028/iajit/19/4/4
![]() |
[32] |
M. M. Khater, Abundant wave solutions of the perturbed Gerdjikov-Ivanov equation in telecommunication industry, Mod. Phys. Lett. B, 35 (2021), 2150456. https://doi.org/10.1142/S021798492150456X doi: 10.1142/S021798492150456X
![]() |
[33] |
L. Yan, Y. H. Sun, Y. Qian, Z. Y. Sun, C. Z. Wang, Method of reaching consensus on probability of food safety based on the integration of finite credible data on block chain, IEEE Access, 9 (2021), 123764–123776. https://doi.org/10.1109/ACCESS.2021.3108178 doi: 10.1109/ACCESS.2021.3108178
![]() |
[34] |
C. Zong, Z. Wan, Container ship cell guide accuracy check technology based on improved 3D point cloud instance segmentation, Brodogradnja, 73 (2022), 23–35. https://doi.org/10.21278/brod73102 doi: 10.21278/brod73102
![]() |
[35] |
J. Xu, K. Guo, P. Z. H. Sun, Driving performance under violations of traffic rules: Novice vs. experienced drivers, IEEE T. Intell. Vehicl., 2022. https://doi.org/10.1109/TIV.2022.3200592 doi: 10.1109/TIV.2022.3200592
![]() |
[36] |
M. S. Iqbal, A. R. Seadawy, M. Z. Baber, Demonstration of unique problems from soliton solutions to nonlinear Selkov-Schnakenberg system, Chaos Soliton. Fract., 162 (2022), 112485. https://doi.org/10.1016/j.chaos.2022.112485 doi: 10.1016/j.chaos.2022.112485
![]() |
[37] |
C. Guo, J. Hu, Time base generator based practical predefined-time stabilization of high-order systems with unknown disturbance, IEEE T. Circuits-II, 2023. https://doi.org/10.1109/TCSII.2023.3242856 doi: 10.1109/TCSII.2023.3242856
![]() |
[38] |
W. Hereman, A. Nuseir, Symbolic methods to construct exact solutions of nonlinear partial differential equations, Math. Comput. Simulat., 43 (1997), 13–27. https://doi.org/10.1016/S0378-4754(96)00053-5 doi: 10.1016/S0378-4754(96)00053-5
![]() |
[39] |
Z. Zhao, Y. Chen, B. Han, Lump soliton, mixed lump stripe and periodic lump solutions of a (2+1)-dimensional asymmetrical Nizhnik-Novikov-Veselov equation, Mod. Phys. Lett. B, 31 (2017), 1750157. https://doi.org/10.1142/S0217984917501573 doi: 10.1142/S0217984917501573
![]() |
[40] |
Q. Meng, Q. Ma, Y. Shi, Adaptive fixed-time stabilization for a class of uncertain nonlinear systems, IEEE T. Automat. Contr., 2023. https://doi.org/10.1109/TAC.2023.3244151 doi: 10.1109/TAC.2023.3244151
![]() |
[41] |
D. Chen, Q. Wang, Y. Li, Y. Li, H. Zhou, Y. Fan, A general linear free energy relationship for predicting partition coefficients of neutral organic compounds, Chemosphere, 247 (2020), 125869. https://doi.org/10.1016/j.chemosphere.2020.125869 doi: 10.1016/j.chemosphere.2020.125869
![]() |
[42] |
M. A. Helal, Soliton solution of some nonlinear partial differential equations and its applications in fluid mechanics, Chaos Soliton. Fract., 13 (2002), 1917–1929. https://doi.org/10.1016/S0960-0779(01)00189-8 doi: 10.1016/S0960-0779(01)00189-8
![]() |
[43] |
N. C. Freeman, Soliton solutions of non-linear evolution equations, IMA J. Appl. Math., 32 (1984), 125–145. https://doi.org/10.1093/imamat/32.1-3.125 doi: 10.1093/imamat/32.1-3.125
![]() |
[44] |
S. Javeed, K. S. Alimgeer, S. Nawaz, A. Waheed, M. Suleman, D. Baleanu, et al., Soliton solutions of mathematical physics models using the exponential function technique, Symmetry, 12 (2020), 176. https://doi.org/10.3390/sym12010176 doi: 10.3390/sym12010176
![]() |
[45] |
Z. Y. Wang, S. F. Tian, J. Cheng, The ∂−-dressing method and soliton solutions for the three-component coupled Hirota equations, J. Math. Phys., 62 (2021). https://doi.org/10.1063/5.0046806 doi: 10.1063/5.0046806
![]() |
[46] |
S. F. Tian, M. J. Xu, T. T. Zhang, A symmetry-preserving difference scheme and analytical solutions of a generalized higher-order beam equation, P. Roy. Soc. A, 477 (2021), 20210455. https://doi.org/10.1098/rspa.2021.0455 doi: 10.1098/rspa.2021.0455
![]() |
[47] |
Y. Li, S. F. Tian, J. J. Yang, Riemann-Hilbert problem and interactions of solitons in the component nonlinear Schrödinger equations, Stud. Appl. Math., 148 (2022), 577–605. https://doi.org/10.1111/sapm.12450 doi: 10.1111/sapm.12450
![]() |
[48] |
Z. Q. Li, S. F. Tian, J. J. Yang, On the soliton resolution and the asymptotic stability of N-soliton solution for the Wadati-Konno-Ichikawa equation with finite density initial data in space-time solitonic regions, Adv. Math., 409 (2022), 108639. https://doi.org/10.1016/j.aim.2022.108639 doi: 10.1016/j.aim.2022.108639
![]() |
[49] | T. Akturk, A. Kubal, Analysis of wave solutions of (2+1)-dimensional Nizhnik-Novikov-Veselov equation, Ordu Üniv. Bilim ve Teknoloji Dergisi, 11 (2021), 13–24. |
[50] |
P. G. Estévez, S. Leble, A wave equation in 2+1: Painlevé analysis and solutions, Inverse Probl., 11 (1995), 925. https://doi.org/10.1088/0266-5611/11/4/018 doi: 10.1088/0266-5611/11/4/018
![]() |
[51] |
Y. Ren, H. Zhang, New generalized hyperbolic functions and auto-Bäcklund transformation to find new exact solutions of the -dimensional NNV equation, Phys. Lett. A, 357 (2006), 438–448. https://doi.org/10.1016/j.physleta.2006.04.082 doi: 10.1016/j.physleta.2006.04.082
![]() |
[52] | L. P. Nizhnik, Integration of multidimensional nonlinear equations by the method of the inverse problem, Dokl. Akademii Nauk, 254 (1980), 332–335. |
[53] |
X. Bai, Y. He, M. Xu, Low-thrust reconfiguration strategy and optimization for formation flying using Jordan normal form, IEEE T. Aero. Elec. Sys., 57 (2021), 3279–3295. https://doi.org/10.1109/TAES.2021.3074204 doi: 10.1109/TAES.2021.3074204
![]() |
[54] |
Q. Liu, H. Peng, Z. Wang, Convergence to nonlinear diffusion waves for a hyperbolic-parabolic chemotaxis system modelling vasculogenesis, J. Differ. Equations, 314 (2022), 251–286. https://doi.org/10.1016/j.jde.2022.01.021 doi: 10.1016/j.jde.2022.01.021
![]() |
[55] |
H. Jin, Z. Wang, L. Wu, Global dynamics of a three-species spatial food chain model, J. Differ. Equations, 333 (2022), 144–183. https://doi.org/10.1016/j.jde.2022.06.007 doi: 10.1016/j.jde.2022.06.007
![]() |
[56] |
M. B. Hossen, H. O. Roshid, M. Z. Ali, Multi-soliton, breathers, lumps and interaction solution to the (2+1)-dimensional asymmetric Nizhnik-Novikov-Veselov equation, Heliyon, 5, (2019). https://doi.org/10.1016/j.heliyon.2019.e02548 doi: 10.1016/j.heliyon.2019.e02548
![]() |
[57] |
A. M. Wazwaz, M. S. Osman, Analyzing the combined multi-waves polynomial solutions in a two-layer-liquid medium, Comput. Math. Appl., 76 (2018), 276–283. https://doi.org/10.1016/j.camwa.2018.04.018 doi: 10.1016/j.camwa.2018.04.018
![]() |
[58] |
M. S. Osman, H. I. A. Gawad, Multi-wave solutions of the (2+1)-dimensional Nizhnik-Novikov-Veselov equations with variable coefficients, Eur. Phys. J. Plus, 130 (2015), 1–11. https://doi.org/10.1140/epjp/i2015-15215-1 doi: 10.1140/epjp/i2015-15215-1
![]() |
[59] |
S. Y. Lou, X. B. Hu, Infinitely many Lax pairs and symmetry constraints of the KP equation, J. Math. Phys., 38 (1997), 6401–6427. https://doi.org/10.1063/1.532219 doi: 10.1063/1.532219
![]() |
[60] |
P. Liu, J. P. Shi, Z. A. Wang, Pattern formation of the attraction-repulsion Keller-Segel system, Discrete Cont. Dyn.-B, 18 (2013), 2597–2625. https://doi.org/ 10.3934/dcdsb.2013.18.2597 doi: 10.3934/dcdsb.2013.18.2597
![]() |
[61] |
H. Chen, W. Chen, X. Liu, X. Liu, Establishing the first hidden-charm pentaquark with strangeness, Eur. Phys. J. C, 81 (2021), 409. https://doi.org/10.1140/epjc/s10052-021-09196-4 doi: 10.1140/epjc/s10052-021-09196-4
![]() |
[62] |
Y. Zhang, Y. He, H. Wang, L. Sun, Y. Su, Ultra-broadband mode size converter using on-chip metamaterial-based Luneburg lens, ACS Photonics, 8 (2021), 202–208. https://doi.org/10.1021/acsphotonics.0c01269 doi: 10.1021/acsphotonics.0c01269
![]() |
[63] |
H. Yasmin, N. H. Aljahdaly, A. M. Saeed, R. Shah, Investigating families of soliton solutions for the complex structured coupled fractional Biswas-Arshed model in birefringent fibers using a novel analytical technique, Fractal Fract., 7 (2023), 491. https://doi.org/10.3390/fractalfract7070491 doi: 10.3390/fractalfract7070491
![]() |
[64] |
H. Yasmin, N. H. Aljahdaly, A. M. Saeed, R. Shah, Probing families of optical soliton solutions in fractional perturbed Radhakrishnan-Kundu-Lakshmanan model with improved versions of extended direct algebraic method, Fractal Fract., 7 (2023), 512. https://doi.org/10.3390/fractalfract7070512 doi: 10.3390/fractalfract7070512
![]() |
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Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+3 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β−1 | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 4 | 4 | β+3 | 0 |
xα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
xα: α=β+1 | β+3 | β+3 | 4 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+4 | β+3 | 4 | 0 |
yα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+3 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β | 2β−α+3 | 2β−α+4 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β−1 | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 3 | 3 | β+2 | 0 |
xα: 2≤α≤β | α+2 | α+1 | β−α+3 | 0 |
xα: α=β+1 | β+2 | β+2 | 3 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+4 | 2β−α+5 | α−β+2 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
xα: α=1 | 4 | 4 | β+3 | 0 |
xα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
xα: α=β+1 | β+3 | β+3 | 4 | 0 |
xα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+3 | β+3 | 4 | 0 |
yα: β+2≤α≤2β | 2β−α+4 | 2β−α+5 | α−β+3 | 0 |
Representation | Γ1 | Γ2 | Γ3 | Γ4 |
yα: α=1 | 4 | 4 | β+3 | 0 |
yα: 2≤α≤β | α+3 | α+2 | β−α+4 | 0 |
yα: α=β+1 | β+4 | β+3 | 4 | 0 |
yα: β+2≤α≤2β+1 | 2β−α+5 | 2β−α+6 | α−β+3 | 0 |