
The aim of this paper is to illustrate how degree sequences may successfully be used over some graph products. Moreover, by taking into account the degree sequence, we will expose some new distinguishing results on special graph products. We will first consider the degree sequences of tensor and cartesian products of graphs and will obtain the omega invariant of them. After that we will conclude that the set of graphs forms an abelian semigroup in the case of tensor product whereas this same set is actually an abelian monoid in the case of cartesian product. As a consequence of these two operations, we also give a result on distributive law which would be important for future studies.
Citation: Bao-Hua Xing, Nurten Urlu Ozalan, Jia-Bao Liu. The degree sequence on tensor and cartesian products of graphs and their omega index[J]. AIMS Mathematics, 2023, 8(7): 16618-16632. doi: 10.3934/math.2023850
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The aim of this paper is to illustrate how degree sequences may successfully be used over some graph products. Moreover, by taking into account the degree sequence, we will expose some new distinguishing results on special graph products. We will first consider the degree sequences of tensor and cartesian products of graphs and will obtain the omega invariant of them. After that we will conclude that the set of graphs forms an abelian semigroup in the case of tensor product whereas this same set is actually an abelian monoid in the case of cartesian product. As a consequence of these two operations, we also give a result on distributive law which would be important for future studies.
Let G=(V,E) be a finite, simple and undirected graph (molecular graph) with vertex set |V(G)|=n and edge set |E(G)|=m. The degree degG(v) of a vertex v of G is the number of vertices adjacent to v. We denote by δ and Δ the minimum and maximum degrees of vertices of G, respectively. The degree sequence of G, DS(G)={1(a1),2(a2),3(a3),…,Δ(aΔ)}, is a sequence of degrees of vertices of G. We may suggest the book [13] for some unmentioned terminology in here.
Let Pn, Kn, Cn, Sn, Km,n be path, complete, cycle, star, complete bipartite graphs, respectively. (See Figure 1 for examples of them).
The number of vertices, edges and degree sequences of these well known graph classes are presented in Table 1.
G | Vertices | Edges | Degree sequence |
Pn | n | (n−1) | {12,2n−2} |
Kn | n | n(n−1)/2 | {(n−1)n} |
Cn | n | n | {2n} |
Sn | n | (n−1) | {1n−1,(n−1)1} |
Km,n | m+n | mn | {mn,nm} |
By considering the degree sequence, it has been introduced a new graph invariant
Ω(G)=Δ∑i=1(i−2)ai | (1.1) |
under the name of omega index Ω(G) (see [4]). Clearly Ω(G) can also be written as a3+2a4+3a5+⋯+(Δ−2)aΔ−a1. This invariant presented direct information on the realizability, number of realizations, connectedness, being acyclic or cyclic, number of components, chords, loops, pendant edges, faces and bridges etc. Besides, the significant difference of Ω(G) from other graph invariant is that it is an index defined over only a given degree sequence. According to [5], omega indices of above indicated well-known graph classes having n vertices are
Ω(Cn)=0,Ω(Pn)=−2=Ω(Sn),Ω(Kn)=n(n−3),Ω(Kr,s)=2[rs−(r+s)]. |
To have a brief look on the different results of omega index, one may read [1,5,6,7].
It is well known that one of the aim to study on graph operations is to produce some new graphs from initial ones. So far, although several studies on different graph operations have been studied (see, for instance, [22,27]), it still takes interest because of the aim indicated just in the previous sentence. We refer to [12] for a recent survey on graph operations. In fact the tensor and cartesian products are well known operations among the others.
The tensor product of two graphs G1 and G2 is the graph G1⊗G2 with the vertex set V(G1⊗G2)=V(G1)×V(G2), and any two vertices (u1,v1) and (u2,v2) are adjacent whenever u1 is adjacent to u2 in G1 and v1 is adjacent to v2 in G2. On the other hand, the cartesian product G1×G2 of two graphs G1 and G2 is the graph with the vertex set V(G1)×V(G2) and any two vertices (u1,u2) and (v1,v2) are adjacent if and only if u1=v1∈V(G1) and u2v2∈E(G2) or u2=v2∈V(G2) and u1v1∈E(G1). These two products have been studied to expose some results on graph colorings, decompositions of graphs, graph embeddings and topological indices; see [17,18,19,23,28].
This paper is structured as follows. In Section 2, we calculate the degree sequence of tensor products of two graphs (Theorem 2.1) and present the general degree sequence formula of G1⊗G2⊗⋯⊗Gn (Theorem 2.2). In the same section, we count the omega invariant of the tensor product of any two graphs (Theorem 2.4) and then state with proofs some consequences (Corollarys 2.6 and 2.7) of this last theorem. The other key point of this section is investigating the algebraic properties (Theorem 2.8) over tensor products via the degree sequence obtained in Theorem 2.1 and Theorem 2.2. In Section 3, by applying same approximation and transferring the similar ideas from the previous section, we obtain important results (Theorems 3.1, 3.3, Corollary 3.5 and Teorem 3.6) over cartesian products of graphs. Finally, in the light of Theorem 3.6, we pay attention to distributive law over tensor and cartesian products (see Theorem 3.7) in which we believe that it would be useful for future studies.
We may remind some other studies mentioned in the first sections over tensor products of graphs as in the following: In [23], the author obtained a characterization and some properties of G⊗K2, and in [29], the author studied the connectedness of the tensor product of two graphs. Furthermore, in [28], it has been obtained the Randic, geometric-arithmetic, first and second Zagreb indices, first and second Zagreb coindices of tensor product of two graphs. Additionally, in [2], the authors have been recently introduced four new tensor products of graphs and studied the first and second Zagreb indices and coindices of the resulting graphs and their complements.
Despite so many studies, the tensor product of graphs over degree sequences has not been studied in the literature. In fact degree sequences on graph operations considered only in the paper [1] in terms of join and corona products of two simple connected graphs. Therefore the studies and their results in this and next sections are quite original and interesting in the literature.
In this section, we focus on how to obtain the degree sequence of the tensor product of two graphs. We firstly start to find the degree sequence on the case G1⊗G2 and then present a general formula for DS(G1⊗G2⊗⋯⊗Gn).
The proof of the following result will be omitted since it is quite clear by considering the definition of tensor products over graphs and then applying the meaning of degree sequence on these graphs obtained by tensor products.
Theorem 2.1. Suppose that the degree sequences of two connected graphs G1 and G2 are defined by DS(G1)={da11,da22,…,dann} and DS(G2)={eb11,eb22,…,ebmm}, respectively. Then
DS(G1⊗G2)={(d1e1)a1b1,(d1e2)a1b2,…,(d1em)a1bm,(d2e1)a2b1,(d2e2)a2b2,…,(d2em)a2bm,…,(dnem)anbm}. |
As an example of the above result, let us consider the degree sequences DS(Pn)={12,2n−2} and DS(Cm)={2m} of Pn and Cm, respectively. Thus the degree sequence of the tensor product (see Figure 2 for a simple numerical plotting) is defined by DS(Pn⊗Cm)={22m,4nm−2m}.
Now, by taking into account the tensor product of n simple connected graphs G1,G2,…,Gn, where n≥2, we can state and prove a generalization of Theorem 2.1 as in the following.
Theorem 2.2. Consider n simple connected graphs G1,G2,…,Gn with the degree sequence of each Gi is DS(Gi)={dai1i1,…,daikik} for i=1,2,…,n and 1≤k≤n. Then the degree sequence DS(G1⊗G2⊗⋯⊗Gn) consists of all terms with the form (dαsαtdβsβt)aαsαtaβsβt, where αs,βs=1,2,…,n and 1≤αt,βt≤n.
Proof. For arbitrary the degree sequences DS(G1)={da11,da22,…,dann} and DS(G2)={eb11,eb22,…,ebmm}, if we apply Theorem 2.1, then we obtain
DS(G1⊗G2)={(d1e1)a1b1,(d1e2)a1b2,…,(d1em)a1bm,(d2e1)a2b1,(d2e2)a2b2,…,(d2em)a2bm,…,(dnem)anbm}. |
Let us take into account an another arbitrary degree sequence DS(G3)={xy11,xy22,…,xytt}.
DS(G1⊗G2⊗G3)={(d1e1)a1b1,(d1e2)a1b2,…,(d1em)a1bm,(d2e1)a2b1,(d2e2)a2b2,…,(d2em)a2bm,…,(dnem)anbm}⊗{xy11,xy22,…,xytt}={(d1e1x1)a1b1y1,…,(d1e1xt)a1b1yt,…,(dnemx1)anbmy1,…,(dnemxt)anbmyt} |
Then, by applying a similar approach n times, the form of the element of degree sequences DS(G1⊗G2⊗⋯⊗Gn) is (dαsαtdβsβt)aαsαtaβsβt, as required.
Example 2.3. Assume that n=3 in Theorem 2.2. Then we obtain the degree sequence
DS(P4⊗C3⊗P3)={12,22}⊗{23}⊗{12,2}={26,46}⊗{12,2}={212,46,412,86} |
for special path and cycle graphs.
The degree sequence of a graph is one of the oldest notions in graph theory. Its applications are legion; they range from computing science to real-world networks such as social contact networks where degree distributions play an important role in the analysis of the network. On the other hand the concept of degree sequence is closely related to computable. It is an open problem to determine that which DSs are realizable and there are several algorithms to determine that. Omega invariant, many properties of its have been obtained [5], directly say whether the given degree sequence is realizable (see [4]). So this invariant is essential. There are several graph operations used in calculating some chemical invariants of graphs. In [1], the authors studied omega invariant of union and corona product of two graphs. This section emphasizes on the omega invariant for the tensor product of two graph.
Firstly we calculate the degree sequence and omega invariant of the tensor product of two special graphs such as path, complete, cycle, star and complete bipartite graphs. (See Table 2).
G1 | G2 | G1⊗G2 | Ω(G1⊗G2) |
Pr | Ps | {14,2(2s−4),2(2r−4), | 2(r−2)(s−2)−4 |
4(r−2)(s−2)} | |||
Pr | Ks | {(s−1)(2s),(2s−2)(rs−2s)} | (s−3)2s+(2s−4)(rs−2s) |
Pr | Cs | {2(2s),4(rs−2s)} | 2(rs−2s) |
Pr | Ss | {1(2s−2),(s−1)2, | (s−3)2+(2s−4)(r−2)−(2s−2) |
2(r−2)(s−1),(2s−2)(r−2)} | |||
Pr | Ks,t | {s(2t),t(2s),(2s)(rt−2t), | (s−2)2t+(t−2)2s+(2s−2) |
(2t)(rs−2s)} | (rt−2t)+(2t−2)(rs−2s) | ||
Kr | Ps | {(r−1)(2r),(2r−2)(rs−2r)} | (r−3)2r+(2r−4)(rs−2r) |
Kr | Ks | {((r−1)(s−1))(rs)} | (rs−r−s−1)rs |
Kr | Cs | {(2r−2)(rs)} | (2r−4)rs |
Kr | Ss | {(r−1)(rs−r),((r−1)(s−1))r} | (r−3)(rs−r)+(rs−r−s−1)r |
Kr | Ks,t | {(rs−s)(rt),(rt−t)(rs)} | (rs−s−2)rt+(rt−t−2)rs |
Cr | Ps | {2(2r),4(rs−2r)} | 2(rs−2r) |
Cr | Ks | {(2s−2)(rs)} | (2s−4)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {2(rs−r),(2s−2)r} | (2s−4)r |
Cr | Ks,t | {(2s)(rt),(2t)(rs)} | (2s−2)rt+(2t−2)rs |
Sr | Ps | {1(2r−2),2(r−1)(s−2),(r−1)2,(2r−2)(s−2)} | (r−3)2+(2r−4)(s−2)−2r+2 |
Sr | Ks | {(s−1)(rs−s),((r−1)(s−1))s} | (s−3)(rs−s)+((r−1)(s−1)−2)s |
Sr | Cs | {2(rs−s),(2r−2)s} | (2r−4)s |
Sr | Ss | {1((r−1)(s−1)),(s−1)(r−1), | (s−3)(r−1)+(r−3)(s−1)+ |
(r−1)(s−1),(r−1)(s−1)} | ((r−1)(s−1)−2)−(r−1)(s−1) | ||
Sr | Ks,t | {s(rt−t),t(rs−s), | (s−2)(rt−t)+(t−2)(rs−s)+ |
(rs−s)t,(rt−t)s} | (rs−s−2)t+(rt−t−2)s | ||
Kr,s | Pt | {r(2s),(2r)(st−2s),s(2r),} | (r−2)2s+(2r−2)(st−2s)+ |
{(2s)(rt−2r)} | (s−2)2r+(2s−2)(rt−2r) | ||
Kr,s | Kt | {(rt−r)(st),(st−s)(rt)} | (rt−r−2)st+(st−s−2)rt |
Kr,s | Ct | {(2r)(st),(2s)(rt)} | (2r−2)st+(2s−2)rt |
Kr,s | St | {r(st−s),(rt−r)s,s(rt−r),(st−s)r} | (r−2)(st−s)+(rt−r−2)s+(s−2)(rt−r)+(st−s−2)r |
Kr,s | Kt,m | {(rt)(sm),(rm)(st),(st)(rm), | (rt−2)sm+(rm−2)st+ |
(sm)(rt)} | +(st−2)rm+(sm−2)rt |
Now, we give the omega invariant of the tensor product of any two graphs in general.
Theorem 2.4. For any two connected graphs G1 and G2 having n1 vertices, m1 edges and n2 vertices, m2 edges, respectively, the omega index of their tensor product is
Ω(G1⊗G2)=4m1m2−2n1n2. |
Proof. Let us suppose that the degree sequences of these graphs are defined by DS(G1)={da11,da22,…,ΔaΔ11} and DS(G2)={eb11,eb22,…,ΔbΔ22}, respectively. So, by the definition of omega invariant given in Eq. (1.1), we obtain
Ω(G1⊗G2)=(d1e1−2)a1b1+(d1e2−2)a1b2+(d1e3−2)a1b3+⋯+(d1Δ2−2)a1bΔ2+(d2e1−2)a2b1+(d2e2−2)a2b2+⋯+(d2Δ2−2)a2bΔ2+⋯+(Δ1e1−2)aΔ1b1+(Δ1e2−2)aΔ1b2+⋯+(Δ1Δ2−2)aΔ1bΔ2=d1a1(e1b1+e2b2+⋯+Δ2bΔ2)+d2a2(e1b1+e2b2+⋯+Δ2bΔ2)+⋯+Δ1aΔ1(e1b1+e2b2+⋯+Δ2bΔ2)−2(a1b1+⋯+a1bΔ2+a2b1+⋯+a2bΔ2+⋯)=(e1b1+e2b2+⋯+Δ2bΔ2)(d1a1+d2a2+⋯+Δ1aΔ1)−2(b1+⋯+bΔ2)(a1+⋯+aΔ1)=2m22m1−2n2n1=4m1m2−2n1n2, |
as required.
Example 2.5. Note that DS(Sr⊗Ks,t)={s(rt−t),t(rs−s),(rs−s)t,(rt−t)s}. For example, DS(S3⊗K3,4)={38,46,64,83} and Ω(S3⊗K3,4)=1×8+2×6+4×4+6×3=54. On the other hand S3 and K3,4 have 3 vertices, 2 edges and 7 vertices, 12 edges, respectively. Accordingly Theorem 2.4, Ω(S3⊗K3,4)=4×2×12−2×3×7=54 approving the truth of it.
As a consequence of Theorem 2.4, we can restate the omega invariant of the tensor product of two graphs in terms of the omega index of only one of the graphs.
Corollary 2.6. Ω(G1⊗G2)=2m2Ω(G1)+4m2n1−2n1n2.
Proof. We clearly have
Ω(G1⊗G2)=(e1b1+e2b2+⋯+Δ2bΔ2)(d1a1+d2a2+⋯+Δ1aΔ1)−2(b1+⋯+bΔ2)(a1+⋯+aΔ1)=2m2(Ω(G1)+2n1)−2n1n2=2m2Ω(G1)+4m2n1−2n1n2 |
which completes the proof.
With a similar approach as in the proof of Corollary 2.6, one may obtain the following another consequence of Theorem 2.4.
Corollary 2.7.. Ω(G1⊗G2)=2m1Ω(G2)+4m1n2−2n1n2.
Havel in 1955 [14], Erdos and Gallai in 1960 [21], Hakimi in 1962 [11], Knuth in 2008 [16], Tripathi et al. in 2010 [25] proposed a method to decide, whether a sequence of nonnegative integers can be the degree sequence of a simple graph. Sierksma and Hoogeven in 1991 [24] compared seven known methods. These studies are about whether a graph can be drawn over the degree sequence. On the other hand, in [20], the authors studied some algebraic properties of the join and corona product of two graphs. In this section, we obtain new result regarding algebraic structure of the set of graphs accorging to tensor product operation.
Theorem 2.8. Let G be the set of all simple connected graphs. Then G defines an abelian semigroup under the operation of tensor products.
Proof. Let us consider any three graphs G1, G2 and G3 from the set G having degree sequences
DS(G1)={da11,da22,…,dann},DS(G2)={eb11,eb22,…,ebmm} and DS(G3)={xy11,xy22,…,xytt}, |
respectively. Now our aim is to show that G satisfies closure, associativity and commutativity properties under the operation of the tensor product.
First of all, the tensor product of two simple connected graph is another graph, so G is closed. For associativity,
(G1⊗G2)⊗G3={(d1e1)a1b1,…,(d1em)a1bm,…,(dne1)anb1,…,(dnem)anbm}⊗{xy11,xy22,…,xytt}={(d1e1x1)a1b1y1,…,(d1e1xt)a1b1yt,(d1emx1)a1bmy1,…,(d1emxt)a1bmyt,(dne1x1)anb1y1,…,(dnemxt)anbmyt} |
and
G1⊗(G2⊗G3)={da11,da22,…,dann}⊗{(e1x1)b1y1,…,(e1xt)b1yt,…,(emx1)bmy1,…,(emxt)bmyt}={(d1e1x1)a1b1y1,…,(d1e1xt)a1b1yt,(d1emx1)a1bmy1,…,(d1emxt)a1bmyt,(dne1x1)anb1y1,…,(dnemxt)anbmyt}. |
In addition, since the property
G1⊗G2={(d1e1)a1b1,…,(d1em)a1bm,…,(dne1)anb1,…,(dnem)anbm}={(e1d1)b1a1,…,(e1dn)b1an,…,(emd1)bma1,…,(emdn)bman}=G2⊗G1 |
holds, the operation ⊗ is commutative on G.
Clearly, to identify the identity element (if there exists), we need to find a graph I with the property G1⊗I=G1 and I⊗G1=G1. Assume that the degree sequence of the graph I is defined by DS(I)={kt11,kt22,...,ktnn}. Then
G1⊗I={(d1k1)a1t1,(d1k2)a1t2,…,(d1kn)a1tn,(d2k1)a2t1,…,(d2kn)a2tn,…,(dnk1)ant1,…,(dnkn)antn}={da11,da22,…,dann}. |
However to be held of this equality, the degree sequence must the form of DS(I)={11}. But there is no such a graph since the degree sequence {11} is not realizable. This implies that the identity element does not exist.
Hence the result.
Research into the extension of graphs is essential in applied sciences. So, there are many studies on the Cartesian product which is a graph extension. In [3], the authors gave sufficient conditions for the Cartesian product of two graphs to be maximum edge-connected, maximum point-connected, super edge-connected. The researchers in [9,10] estimated the Wiener index of the Cartesian product of graphs and in [15] the authors calculated the Szeged index of the Cartesian product of graphs. Very recently, in [26], the author computed Sombor index over the tensor and Cartesian products of a monogenic semigroup graph. In this section we scrutinize the cartesian products of graphs via its degree sequence.
Now, we consider degree sequence of the cartesian product of two graphs. Firstly we give the degree sequence of cartesian product of two graphs G1,G2, then we obtain general formula for degree sequence of G1×G2×⋯×Gn.
With completely the same reason as mentioned for Theorem 2.1, proof of the following result will be omitted.
Theorem 3.1. Suppose that two connected graphs G1 and G2 have the degree sequences DS(G1)={da11,da22,…,dann} and DS(G2)={eb11,eb22,…,ebmm}, respectively. Then
DS(G1×G2)={(d1+e1)a1b1,(d1+e2)a1b2,…,(d1+em)a1bm,(d2+e1)a2b1,(d2+e2)a2b2,…,(d2+em)a2bm,…,(dn+em)anbm}. |
A simple example for Theorem 3.1 can be presented by considering the cartesian product of C3 and P4 (see Figure 3). In fact, since DS(P4)={12,22} and DS(C3)={23}, we obtain DS(P4×C3)={(2+1)2×3,(2+2)2×3}.
In the following, as a generalization of Theorem 3.1, we take into account the cartesian product of n simple connected graphs G1,G2,⋯,Gn, where n≥2.
Theorem 3.2. Let G1,G2,⋯,Gn be n simple connected graphs, and let the degree sequence of each Gi be DS(Gi)={dai1i1,…,daikik} for i=1,2,…,n and 1≤k≤n. Then DS(G1×G2×⋯×Gn) consists of all terms with the form
(dα1α2+dβ1β2)aα1α2aβ1β2, |
where α1,β1=1,2,…,n and 1≤α2,β2≤n.
Proof. We will follow a similar way as in the proof of Theorem 2.2. For the degree sequences
DS(G1)={da11,da22,…,dann},DS(G2)={eb11,eb22,…,ebmm} and DS(G3)={xy11,xy22,…,xytt}, |
if we apply Theorem 3.1, then we obtain
DS(G1×G2×G3)={(d1+e1)a1b1,(d1+e2)a1b2,…,(d1+em)a1bm,(d2+e1)a2b1,(d2+e2)a2b2,…,(d2+em)a2bm,…,(dn+em)anbm}×{xy11,xy22,…,xytt}={(d1+e1+x1)a1b1y1,…,(d1+e1+xt)a1b1yt,…,(dn+em+x1)anbmy1,…,(dn+em+xt)anbmyt}. |
To achieve the truthfulness of Theorem, it is enough to process n times. Thus, it is clear that the form of the element of degree sequences DS(G1×G2×⋯×Gn) is (dα1α2+dβ1β2)aα1α2aβ1β2.
With a similar manner and using the same graphs as in Example 2.3, by considering Theorem 3.2, the degree sequence of the cartesian product is
DS(P4×C3×P3)={12,22}×{23}×{12,2}={36,46}×{12,2}={412,56,512,66}={412,518,66}. |
In this section we give the degree sequence and omega invariant of the cartesian product of two special graphs such as path, complete, cycle, star and complete bipartite graphs (See Table 3).
G1 | G2 | G1×G2 | Ω(G1×G2) |
Pr | Ps | {24,3(2s−4),3(2r−4), | (2s−8+2r)+2((r−2)(s−2)) |
4(r−2)(s−2)} | |||
Pr | Ks | {s(2s),(s+1)(rs−2s)} | (s−2)2s+(s−1)(rs−2s) |
Pr | Cs | {3(2s),4(rs−2s)} | 2s+2(rs−2s) |
Pr | Ss | {2(2s−2),s2,3(r−2)(s−1), | (s−2)2+(s−1)(r−2)− |
(s+1)(r−2)} | (s−1)(r−2) | ||
Pr | Ks,t | {(1+s)(2t),(1+t)(2s),(2+s)(rt−2t),(2+t)(rs−2s)} | (s−1)2t+(t−1)2s+s(rt−2t)+t(rs−2s) |
Kr | Ps | {(r)(2r),(r+1)(rs−2r)} | (r−2)2r+(r−1)(rs−2r) |
Kr | Ks | {(r+s−2)(rs)} | (r+s−4)rs |
Kr | Cs | {(r+1)(rs)} | (r−1)rs |
Kr | Ss | {(r)(rs−r),(r+s−2)r} | (r−2)(rs−r)+(r+s−4)r |
Kr | Ks,t | {(r+s−1)(rt),(r+t−1)(rs)} | (r+s−3)(rt)+(r+t−3)(rs) |
Cr | Ps | {3(2r),4(rs−2r)} | 2r+2(rs−2r) |
Cr | Ks | {(s+1)(rs)} | (s−1)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {3(rs−r),(s+1)r} | (rs−r)+(s−1)r |
Cr | Ks,t | {(2+s)(rt),(2+t)(rs)} | 2srt |
Sr | Ps | {2(2r−2),3(r−1)(s−2),r2, | (r−1)(s−2)+(r−2)2+ |
(r+1)(s−2)} | (r−1)(s−2) | ||
Sr | Ks | {s(rs−s),(r+s−2)s} | (s−2)(rs−s)+(r+s−4)s |
Sr | Cs | {3(rs−s),(r+1)s} | (rs−s)+(r−1)s |
Sr | Ss | {2((r−1)(s−1)),s(r−1), | (s−2)(r−1)+(r−2)(s−1)+ |
r(s−1),(r+s−2)} | (r+s−4) | ||
Sr | Ks,t | {(1+s)(rt−t),(1+t)(rs−s),(r+s−1)t,(r+t−1)s} | (s−1)(rt−t)+(t−1)(rs−s)+(r+s−3)t+(r+t−3)s |
Kr,s | Pt | {(r+1)(2s),(2+r)(st−2s),(s+1)(2r),(2+s)(rt−2r)} | (r−1)(2s)+r(st−2s)+(s−1)(2r)+s(rt−2r) |
Kr,s | Kt | {(r+t−1)(st),(s+t−1)(rt)} | (r+t−3)(st)+(s+t−3)(rt) |
Kr,s | Ct | {(2+r)(st),(2+s)(rt)} | 2rst |
Kr,s | St | {(r+1)(st−s),(r+t−1)s,(s+1)(rt−r),(s+t−1)r} | (r−1)(st−s)+(r+t−3)s+(s−1)(rt−r)+(s+t−3)r |
Kr,s | Kt,m | {(r+t)(sm),(r+m)(st),(s+t)(rm),(s+m)(rt)} | (r+t−2)(sm)+(r+m−2)(st)+(s+t−2)(rm)+(s+m−2)(rt) |
Now, we give the omega invariant of the cartesian product of any two graphs in general.
Theorem 3.3. Let G1 and G2 be a connected graphs with n1 vertices, m1 edges, and n2 vertices, m2 edges, respectively. Then
Ω(G1×G2)=2(m1n2+m2n1−n1n2). |
Proof. Assume DS(G1)={da11,da22,…,dann} and DS(G2)={eb11,eb22,…,ebmm}. By Eq. (1.1), we have
Ω(G1×G2)=(d1+e1−2)a1b1+(d1+e2−2)a1b2+(d1+e3−2)a1b3+…+(d1+em−2)a1bm+(d2+e1−2)a2b1+(d2+e2−2)a2b2+…+(d2+em−2)a2bm+…+(dn+e1−2)anb1+(dn+e2−2)anb2+…+(dn+em−2)anbm=d1a1(b1+b2+…+bm)+d2a2(b1+b2+…+bm)+…+dnan(b1+b2+…+bm)+a1(e1b1+e2b2+…+embm)+a2(e1b1+e2b2+…+embm)+…+an(e1b1+e2b2+…+embm)−2(a1b1+…+a1bm+a2b1+…+a2bm+…)=(b1+b2+…+bm)(d1a1+d2a2+…+dnan)+(a1+a2+…+an)(e1b1+…+embm)−2(b1+…+bm)(a1+…+an)=n22m1+n12m2−2n1n2=2(m1n2+m2n1−n1n2), |
as required.
Example 3.4. Let us consider DS(Cr×Ss)={3(rs−r),(s+1)r}. In particular, we choose C3 and S4. We have DS(C3×S4)={39,53} and Ω(C3×S4)=(3−2)×9+(5−2)×3=18. Indeed, C3 and S4 have 3 vertices, 3 edges and 4 vertices, 3 edges, respectively. Accordingly Theorem 3.3, Ω(C3×S4)=2(3×4+3×3−3×4)=18 approving the truth of it.
As a result of Theorem 3.3, we can present the omega invariant of the cartesian product of two graphs by the omega index of graphs.
Corollary 3.5. Ω(G1×G2)=n2Ω(G1)+n1Ω(G2)+2n1n2.
Proof. Suppose that G1 and G2 have the same degree sequences as in the proof of Theorem 2.8. In this case, we get
Ω(G1×G2)=(b1+b2+…+bΔ2)(d1a1+d2a2+…+Δ1aΔ1)+(a1+a2+…+aΔ1)(e1b1+…+Δ2bΔ2)−2(b1+…+bΔ2)(a1+…+aΔ1)=n2(Ω(G1)+2n1)+n1(Ω(G2)+2n2)−2n1n2=n2Ω(G1)+n1Ω(G2)+2n1n2, |
as required.
With a different manner from above topics (Sections 3.1 and 3.2), in this section, we will state and prove some theoretical results. Firstly we consider algebraic structure of set of connected graphs by using cartesian product operation.
Theorem 3.6. Let G be the set of all simple connected graphs. Thus G is an abelian monoid under the cartesian product.
Proof. Consider three graphs from the family G having degree sequences DS(G1)={da11,da22,…,dann}, DS(G2)={eb11,eb22,…,ebmm} and DS(G3)={xy11,xy22,…,xytt}. Aim is to show that G is closed, associative, commutative and having an identity element under the cartesian product.
By the definition, since the cartesian product of any two simple connected graphs is another simple connected graph in G, we achieve that G is closed.
For associativity,
(G1×G2)×G3={(d1+e1)a1b1,…,(d1+em)a1bm,…,(dn+e1)anb1,…,(dn+em)anbm}×{xy11,xy22,…,xytt}={(d1+e1+x1)a1b1y1,…,(d1+e1+xt)a1b1yt,(d1+em+x1)a1bmy1,…,(d1+em+xt)a1bmyt,(dn+e1+x1)anb1y1,…,(dn+em+xt)anbmyt} |
and
G1×(G2×G3)={da11,da22,…,dann}×{(e1+x1)b1y1,…,(e1+xt)b1yt,…,(em+x1)bmy1,…,(em+xt)bmyt}={(d1+e1+x1)a1b1y1,…,(d1+e1+xt)a1b1yt,(d1+em+x1)a1bmy1,…,(d1+em+xt)a1bmyt,(dn+e1+x1)anb1y1,…,(dn+em+xt)anbmyt}. |
So G is associative. Moreover, for any two graphs G1,G2∈G, a simple calculation shows that G1×G2=G2×G1 which implies the commutativity of G.
To the identity element, we need to find a suitable graph I∈G such that the equality G×I=G=I×G holds for every G∈G. Let us reconsider G1∈G and assume that DS(I)={kt11,kt22,…,ktnn}.
G1×I={(d1+k1)a1t1,(d1+k2)a1t2,...,(d1+kn)a1tn,(d2+k1)a2t1,…,(d2+kn)a2tn,…,(dn+k1)ant1,…,(dn+kn)antn}={da11,da22,…,dann} |
To have this equality, we must have DS(I)={01}. This implies that k1=k2=⋯=kn=0 and t1=t2=⋯=tn=1 and so this graph is order-zero graph, and the unique graph having no vertices (hence its order is zero). Since we have identity element, the cartesian product operation is monoid. Eventually, we consider the inverse element of the graph DS(G1)={da11,da22,…,dann}. Let us denote the inverse element with {cx11,cx22,…,cxnn}. Then we have
{da11,da22,…,dann}×{cx11,cx22,…,cxnn}={01}{(d1+c1)a1x1,…,(d1+cn)a1xn,…,(d2+cn)a2xn,…,(dn+c1)anx1,…,(dn+cn)anxn}={01}. |
In this case, this equation cannot be hold and so there is no inverse element of G. Therefore G is abelian monoid with the cartesian product operation.
Now, we consider distributive law related to tensor and cartesian product operation.
Theorem 3.7. Tensor and cartesian products do not provide the distributive law over each other. In other words,
G1⊗(G2×G3)≠(G1⊗G2)×(G1⊗G3)andG1×(G2⊗G3)≠(G1×G2)⊗(G1×G3). |
Proof. Let us take DS(G1)={da11,da22,…,dann},DS(G2)={eb11,eb22,…,ebmm},DS(G3)={xy11,xy22,…,xytt}. Now, we handle the first case.
G1⊗(G2×G3)={da11,…,dann}⊗{(e1+x1)b1y1,…,(e1+xt)b1yt,…,(em+x1)bmy1,…,(em+xt)bmyt}={(d1(e1+x1))a1b1y1,…,(d1(e1+xt))a1b1yt,…,(d1(em+x1))a1bmy1,…,(d1(em+xt))a1bmyt,…,(dn(e1+x1))anb1y1,…,(dn(e1+xt))anb1yt,…,(dn(em+x1))anbmy1,…,(dn(em+xt))anbmyt}. |
On the other hand, the mixed product (G1⊗G2)×(G1⊗G3) is equal to
{(d1e1)a1b1,…,(d1em)a1bm,…,(dne1)anb1,…,(dnem)anbm}×{(d1x1)a1y1,…,(d1xt)a1yt,…,(dnx1)any1,…,(dnxt)anyt}={((d1e1)+(d1x1))(a1)2b1y1,…,((d1e1)+(dnxt))a1b1anyt,…,((dnem)+(d1x1))anbma1y1,…,((dnem)+(dnxt))(an)2bmyt}. |
So this result is required. Second claim follow after following calculations:
G1×(G2⊗G3)={da11,…,dann}×{(e1x1)b1y1,…,(e1xt)b1yt,…,(emx1)bmy1,…,(emxt)bmyt}={(d1+(e1x1))a1b1y1,…,(d1+(e1xt))a1b1yt,…,(d1+(emx1))a1bmy1,…,(d1+(emxt))a1bmyt,…,(dn+(e1x1))anb1y1,…,(dn+(e1xt))anb1yt,…,(dn+(emx1))anbmy1,…,(dn+(emxt))anbmyt} |
and the mixed product (G1×G2)⊗(G1×G3) is equal to
{(d1+e1)a1b1,…,(d1+em)a1bm,…,(dn+e1)anb1,…,(dn+em)anbm}⊗{(d1+x1)a1y1,…,(d1+xt)a1yt,…,(dn+x1)any1,…,(dn+xt)anyt}={((d1+e1)(d1+x1))(a1)2b1y1,…,((d1+e1)(dn+xt))a1b1anyt,…,((dn+em)(d1+x1))anbma1y1,…,((dn+em)(dn+xt))(an)2bmyt}. |
This paper is supported by the Natural Science Foundation of Anhui Provincial Department of Education (KJ2021A0650), Graduate offline course graph theory (2021aqnuxskc02).
The authors declare that there is no conflict of interest in this paper.
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G | Vertices | Edges | Degree sequence |
Pn | n | (n−1) | {12,2n−2} |
Kn | n | n(n−1)/2 | {(n−1)n} |
Cn | n | n | {2n} |
Sn | n | (n−1) | {1n−1,(n−1)1} |
Km,n | m+n | mn | {mn,nm} |
G1 | G2 | G1⊗G2 | Ω(G1⊗G2) |
Pr | Ps | {14,2(2s−4),2(2r−4), | 2(r−2)(s−2)−4 |
4(r−2)(s−2)} | |||
Pr | Ks | {(s−1)(2s),(2s−2)(rs−2s)} | (s−3)2s+(2s−4)(rs−2s) |
Pr | Cs | {2(2s),4(rs−2s)} | 2(rs−2s) |
Pr | Ss | {1(2s−2),(s−1)2, | (s−3)2+(2s−4)(r−2)−(2s−2) |
2(r−2)(s−1),(2s−2)(r−2)} | |||
Pr | Ks,t | {s(2t),t(2s),(2s)(rt−2t), | (s−2)2t+(t−2)2s+(2s−2) |
(2t)(rs−2s)} | (rt−2t)+(2t−2)(rs−2s) | ||
Kr | Ps | {(r−1)(2r),(2r−2)(rs−2r)} | (r−3)2r+(2r−4)(rs−2r) |
Kr | Ks | {((r−1)(s−1))(rs)} | (rs−r−s−1)rs |
Kr | Cs | {(2r−2)(rs)} | (2r−4)rs |
Kr | Ss | {(r−1)(rs−r),((r−1)(s−1))r} | (r−3)(rs−r)+(rs−r−s−1)r |
Kr | Ks,t | {(rs−s)(rt),(rt−t)(rs)} | (rs−s−2)rt+(rt−t−2)rs |
Cr | Ps | {2(2r),4(rs−2r)} | 2(rs−2r) |
Cr | Ks | {(2s−2)(rs)} | (2s−4)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {2(rs−r),(2s−2)r} | (2s−4)r |
Cr | Ks,t | {(2s)(rt),(2t)(rs)} | (2s−2)rt+(2t−2)rs |
Sr | Ps | {1(2r−2),2(r−1)(s−2),(r−1)2,(2r−2)(s−2)} | (r−3)2+(2r−4)(s−2)−2r+2 |
Sr | Ks | {(s−1)(rs−s),((r−1)(s−1))s} | (s−3)(rs−s)+((r−1)(s−1)−2)s |
Sr | Cs | {2(rs−s),(2r−2)s} | (2r−4)s |
Sr | Ss | {1((r−1)(s−1)),(s−1)(r−1), | (s−3)(r−1)+(r−3)(s−1)+ |
(r−1)(s−1),(r−1)(s−1)} | ((r−1)(s−1)−2)−(r−1)(s−1) | ||
Sr | Ks,t | {s(rt−t),t(rs−s), | (s−2)(rt−t)+(t−2)(rs−s)+ |
(rs−s)t,(rt−t)s} | (rs−s−2)t+(rt−t−2)s | ||
Kr,s | Pt | {r(2s),(2r)(st−2s),s(2r),} | (r−2)2s+(2r−2)(st−2s)+ |
{(2s)(rt−2r)} | (s−2)2r+(2s−2)(rt−2r) | ||
Kr,s | Kt | {(rt−r)(st),(st−s)(rt)} | (rt−r−2)st+(st−s−2)rt |
Kr,s | Ct | {(2r)(st),(2s)(rt)} | (2r−2)st+(2s−2)rt |
Kr,s | St | {r(st−s),(rt−r)s,s(rt−r),(st−s)r} | (r−2)(st−s)+(rt−r−2)s+(s−2)(rt−r)+(st−s−2)r |
Kr,s | Kt,m | {(rt)(sm),(rm)(st),(st)(rm), | (rt−2)sm+(rm−2)st+ |
(sm)(rt)} | +(st−2)rm+(sm−2)rt |
G1 | G2 | G1×G2 | Ω(G1×G2) |
Pr | Ps | {24,3(2s−4),3(2r−4), | (2s−8+2r)+2((r−2)(s−2)) |
4(r−2)(s−2)} | |||
Pr | Ks | {s(2s),(s+1)(rs−2s)} | (s−2)2s+(s−1)(rs−2s) |
Pr | Cs | {3(2s),4(rs−2s)} | 2s+2(rs−2s) |
Pr | Ss | {2(2s−2),s2,3(r−2)(s−1), | (s−2)2+(s−1)(r−2)− |
(s+1)(r−2)} | (s−1)(r−2) | ||
Pr | Ks,t | {(1+s)(2t),(1+t)(2s),(2+s)(rt−2t),(2+t)(rs−2s)} | (s−1)2t+(t−1)2s+s(rt−2t)+t(rs−2s) |
Kr | Ps | {(r)(2r),(r+1)(rs−2r)} | (r−2)2r+(r−1)(rs−2r) |
Kr | Ks | {(r+s−2)(rs)} | (r+s−4)rs |
Kr | Cs | {(r+1)(rs)} | (r−1)rs |
Kr | Ss | {(r)(rs−r),(r+s−2)r} | (r−2)(rs−r)+(r+s−4)r |
Kr | Ks,t | {(r+s−1)(rt),(r+t−1)(rs)} | (r+s−3)(rt)+(r+t−3)(rs) |
Cr | Ps | {3(2r),4(rs−2r)} | 2r+2(rs−2r) |
Cr | Ks | {(s+1)(rs)} | (s−1)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {3(rs−r),(s+1)r} | (rs−r)+(s−1)r |
Cr | Ks,t | {(2+s)(rt),(2+t)(rs)} | 2srt |
Sr | Ps | {2(2r−2),3(r−1)(s−2),r2, | (r−1)(s−2)+(r−2)2+ |
(r+1)(s−2)} | (r−1)(s−2) | ||
Sr | Ks | {s(rs−s),(r+s−2)s} | (s−2)(rs−s)+(r+s−4)s |
Sr | Cs | {3(rs−s),(r+1)s} | (rs−s)+(r−1)s |
Sr | Ss | {2((r−1)(s−1)),s(r−1), | (s−2)(r−1)+(r−2)(s−1)+ |
r(s−1),(r+s−2)} | (r+s−4) | ||
Sr | Ks,t | {(1+s)(rt−t),(1+t)(rs−s),(r+s−1)t,(r+t−1)s} | (s−1)(rt−t)+(t−1)(rs−s)+(r+s−3)t+(r+t−3)s |
Kr,s | Pt | {(r+1)(2s),(2+r)(st−2s),(s+1)(2r),(2+s)(rt−2r)} | (r−1)(2s)+r(st−2s)+(s−1)(2r)+s(rt−2r) |
Kr,s | Kt | {(r+t−1)(st),(s+t−1)(rt)} | (r+t−3)(st)+(s+t−3)(rt) |
Kr,s | Ct | {(2+r)(st),(2+s)(rt)} | 2rst |
Kr,s | St | {(r+1)(st−s),(r+t−1)s,(s+1)(rt−r),(s+t−1)r} | (r−1)(st−s)+(r+t−3)s+(s−1)(rt−r)+(s+t−3)r |
Kr,s | Kt,m | {(r+t)(sm),(r+m)(st),(s+t)(rm),(s+m)(rt)} | (r+t−2)(sm)+(r+m−2)(st)+(s+t−2)(rm)+(s+m−2)(rt) |
G | Vertices | Edges | Degree sequence |
Pn | n | (n−1) | {12,2n−2} |
Kn | n | n(n−1)/2 | {(n−1)n} |
Cn | n | n | {2n} |
Sn | n | (n−1) | {1n−1,(n−1)1} |
Km,n | m+n | mn | {mn,nm} |
G1 | G2 | G1⊗G2 | Ω(G1⊗G2) |
Pr | Ps | {14,2(2s−4),2(2r−4), | 2(r−2)(s−2)−4 |
4(r−2)(s−2)} | |||
Pr | Ks | {(s−1)(2s),(2s−2)(rs−2s)} | (s−3)2s+(2s−4)(rs−2s) |
Pr | Cs | {2(2s),4(rs−2s)} | 2(rs−2s) |
Pr | Ss | {1(2s−2),(s−1)2, | (s−3)2+(2s−4)(r−2)−(2s−2) |
2(r−2)(s−1),(2s−2)(r−2)} | |||
Pr | Ks,t | {s(2t),t(2s),(2s)(rt−2t), | (s−2)2t+(t−2)2s+(2s−2) |
(2t)(rs−2s)} | (rt−2t)+(2t−2)(rs−2s) | ||
Kr | Ps | {(r−1)(2r),(2r−2)(rs−2r)} | (r−3)2r+(2r−4)(rs−2r) |
Kr | Ks | {((r−1)(s−1))(rs)} | (rs−r−s−1)rs |
Kr | Cs | {(2r−2)(rs)} | (2r−4)rs |
Kr | Ss | {(r−1)(rs−r),((r−1)(s−1))r} | (r−3)(rs−r)+(rs−r−s−1)r |
Kr | Ks,t | {(rs−s)(rt),(rt−t)(rs)} | (rs−s−2)rt+(rt−t−2)rs |
Cr | Ps | {2(2r),4(rs−2r)} | 2(rs−2r) |
Cr | Ks | {(2s−2)(rs)} | (2s−4)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {2(rs−r),(2s−2)r} | (2s−4)r |
Cr | Ks,t | {(2s)(rt),(2t)(rs)} | (2s−2)rt+(2t−2)rs |
Sr | Ps | {1(2r−2),2(r−1)(s−2),(r−1)2,(2r−2)(s−2)} | (r−3)2+(2r−4)(s−2)−2r+2 |
Sr | Ks | {(s−1)(rs−s),((r−1)(s−1))s} | (s−3)(rs−s)+((r−1)(s−1)−2)s |
Sr | Cs | {2(rs−s),(2r−2)s} | (2r−4)s |
Sr | Ss | {1((r−1)(s−1)),(s−1)(r−1), | (s−3)(r−1)+(r−3)(s−1)+ |
(r−1)(s−1),(r−1)(s−1)} | ((r−1)(s−1)−2)−(r−1)(s−1) | ||
Sr | Ks,t | {s(rt−t),t(rs−s), | (s−2)(rt−t)+(t−2)(rs−s)+ |
(rs−s)t,(rt−t)s} | (rs−s−2)t+(rt−t−2)s | ||
Kr,s | Pt | {r(2s),(2r)(st−2s),s(2r),} | (r−2)2s+(2r−2)(st−2s)+ |
{(2s)(rt−2r)} | (s−2)2r+(2s−2)(rt−2r) | ||
Kr,s | Kt | {(rt−r)(st),(st−s)(rt)} | (rt−r−2)st+(st−s−2)rt |
Kr,s | Ct | {(2r)(st),(2s)(rt)} | (2r−2)st+(2s−2)rt |
Kr,s | St | {r(st−s),(rt−r)s,s(rt−r),(st−s)r} | (r−2)(st−s)+(rt−r−2)s+(s−2)(rt−r)+(st−s−2)r |
Kr,s | Kt,m | {(rt)(sm),(rm)(st),(st)(rm), | (rt−2)sm+(rm−2)st+ |
(sm)(rt)} | +(st−2)rm+(sm−2)rt |
G1 | G2 | G1×G2 | Ω(G1×G2) |
Pr | Ps | {24,3(2s−4),3(2r−4), | (2s−8+2r)+2((r−2)(s−2)) |
4(r−2)(s−2)} | |||
Pr | Ks | {s(2s),(s+1)(rs−2s)} | (s−2)2s+(s−1)(rs−2s) |
Pr | Cs | {3(2s),4(rs−2s)} | 2s+2(rs−2s) |
Pr | Ss | {2(2s−2),s2,3(r−2)(s−1), | (s−2)2+(s−1)(r−2)− |
(s+1)(r−2)} | (s−1)(r−2) | ||
Pr | Ks,t | {(1+s)(2t),(1+t)(2s),(2+s)(rt−2t),(2+t)(rs−2s)} | (s−1)2t+(t−1)2s+s(rt−2t)+t(rs−2s) |
Kr | Ps | {(r)(2r),(r+1)(rs−2r)} | (r−2)2r+(r−1)(rs−2r) |
Kr | Ks | {(r+s−2)(rs)} | (r+s−4)rs |
Kr | Cs | {(r+1)(rs)} | (r−1)rs |
Kr | Ss | {(r)(rs−r),(r+s−2)r} | (r−2)(rs−r)+(r+s−4)r |
Kr | Ks,t | {(r+s−1)(rt),(r+t−1)(rs)} | (r+s−3)(rt)+(r+t−3)(rs) |
Cr | Ps | {3(2r),4(rs−2r)} | 2r+2(rs−2r) |
Cr | Ks | {(s+1)(rs)} | (s−1)rs |
Cr | Cs | {4(rs)} | 2rs |
Cr | Ss | {3(rs−r),(s+1)r} | (rs−r)+(s−1)r |
Cr | Ks,t | {(2+s)(rt),(2+t)(rs)} | 2srt |
Sr | Ps | {2(2r−2),3(r−1)(s−2),r2, | (r−1)(s−2)+(r−2)2+ |
(r+1)(s−2)} | (r−1)(s−2) | ||
Sr | Ks | {s(rs−s),(r+s−2)s} | (s−2)(rs−s)+(r+s−4)s |
Sr | Cs | {3(rs−s),(r+1)s} | (rs−s)+(r−1)s |
Sr | Ss | {2((r−1)(s−1)),s(r−1), | (s−2)(r−1)+(r−2)(s−1)+ |
r(s−1),(r+s−2)} | (r+s−4) | ||
Sr | Ks,t | {(1+s)(rt−t),(1+t)(rs−s),(r+s−1)t,(r+t−1)s} | (s−1)(rt−t)+(t−1)(rs−s)+(r+s−3)t+(r+t−3)s |
Kr,s | Pt | {(r+1)(2s),(2+r)(st−2s),(s+1)(2r),(2+s)(rt−2r)} | (r−1)(2s)+r(st−2s)+(s−1)(2r)+s(rt−2r) |
Kr,s | Kt | {(r+t−1)(st),(s+t−1)(rt)} | (r+t−3)(st)+(s+t−3)(rt) |
Kr,s | Ct | {(2+r)(st),(2+s)(rt)} | 2rst |
Kr,s | St | {(r+1)(st−s),(r+t−1)s,(s+1)(rt−r),(s+t−1)r} | (r−1)(st−s)+(r+t−3)s+(s−1)(rt−r)+(s+t−3)r |
Kr,s | Kt,m | {(r+t)(sm),(r+m)(st),(s+t)(rm),(s+m)(rt)} | (r+t−2)(sm)+(r+m−2)(st)+(s+t−2)(rm)+(s+m−2)(rt) |