Research article

Numerous graph energies of regular subdivision graph and complete graph

  • Received: 27 April 2021 Accepted: 19 May 2021 Published: 02 June 2021
  • MSC : 14H50, 14H20, 32S15

  • The graph energy E(G) of a simple graph G is sum of its absolute eigenvalues where eigenvalues of adjacency matrix A(G) are referred as eigenvalues of graph G. Depends upon eigenvalues of different graph matrices, several graph energies has been observed recently such as maximum degree energy, Randiˊc energy, sum-connectivity energy etc. Depending on the definition of a graph matrix, the graph energy can be easily determined. This article contains upper bounds of several graph energies of s-regular subdivision graph S(G). Also various graph energies of complete graph are mentioned in this article.

    Citation: Imrana Kousar, Saima Nazeer, Abid Mahboob, Sana Shahid, Yu-Pei Lv. Numerous graph energies of regular subdivision graph and complete graph[J]. AIMS Mathematics, 2021, 6(8): 8466-8476. doi: 10.3934/math.2021491

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  • The graph energy E(G) of a simple graph G is sum of its absolute eigenvalues where eigenvalues of adjacency matrix A(G) are referred as eigenvalues of graph G. Depends upon eigenvalues of different graph matrices, several graph energies has been observed recently such as maximum degree energy, Randiˊc energy, sum-connectivity energy etc. Depending on the definition of a graph matrix, the graph energy can be easily determined. This article contains upper bounds of several graph energies of s-regular subdivision graph S(G). Also various graph energies of complete graph are mentioned in this article.



    Consider a simple connected graph G=(V(G),E(G)) having |V(G)|=p vertices and E(G)=q edges. Number of edges in the neighborhood of a vertex x in a graph G is named as degree of that vertex and is denoted by dx or d(x). If the number of edges in the neighborhood of each vertex in a graph are same say s then graph is said to be a s-regular graph.

    Adjacency matrix is a p×p matrix having entries axy such that

    axy={1,ifuxuyE(G)0,otherwise

    The eigenvalues of a graph are actually eigenvalues of its A(G). The set which is constructed from eigenvalues of G with their multiplicities is known as spectrum of G.

    In Mathematics, the graph energy was firstly introduced by Ivan Gutman in 1978. Graph energy is built upon eigenvalues of A(G). It is sum of absolute values of elements of spectrum of G. For a p-vertex graph G with eigenvalues βk in non-increasing order for k=1,2,3,...,p,

    E(G)=pk=1|βk|. (1.1)

    The impression which is stated in Eq (1.1) is associated with computational chemistry. If, in a conjugated hydrocarbon system, the eigenvalues of a molecular graph are α1,α2,α3,...,αp and are in non-increasing order. Then Hückel molecular orbital approximation calculated the total Π-electron energy EΠ as

    EΠ=pγ+δ[2p2k=1αk]

    for p is even and

    EΠ=pγ+δ[αk+12+2p12k=1αk]

    for p is odd with γ and δ are constants.

    A large number of research papers have been published on graph energy. The thesis of Siraj [1] contains some elementary determinations of graph energy.

    This paper include upper bounds of different graph energies of subdivision graph S(G) of s-regular graph G containing p vertices and q edges. Also various graph energies of complete graph are explored in this paper.

    Based on eigenvalues of different graph matrices, several energies of a graph have been such as maximum degree energy, seidel energy, sum-connectivity energy etc. These energies depends upon eigenvalues of their corresponding energy matrices, see [2,3,4].

    First we define subdivision graph.

    Definition 2.1 (Subdivision graph). The subdivision graph S(G) of a graph G is acquire by dividing each edge of G into two edges with the help of a vertex of degree 2 on every edge. Thus |V(S(G))|=|V(G)|+|E(G)| and |E(S(G))|=2|E(G)|. The graph of subdivision of cycle C4 is shown in Figure 1.

    Figure 1.  Subdivision of cycle C4.

    In this section, we present bounds of maximum degree energy, minimum degree energy, Randić energy, sum-connectivity energy and first and second Zagreb energies. Firstly, we define these energies.

    Definition 2.2 (Maximum degree energy). [5] The maximum degree energy EM of a simple graph G is define as the sum of the absolute eigenvalues of its maximum degree matrix M(G) where M(G) has (i,j)th entry max(dj,dj) if vivjE(G) and 0 elsewhere.

    Definition 2.3 (Minimum degree energy). [6] The minimum degree energy Em of a simple connected graph G is define as the sum of the absolute eigenvalues of minimum degree matrix m(G) of a graph G where (i,j)th entry of m(G) is min(di,dj) if vivjE(G) and 0 otherwise.

    Definition 2.4 (Randiˊc energy). [7] The randiˊc energy ER of a simple connected graph G is the sum of the absolute eigenvalues of the randiˊc matrix R(G) where if vivjE(G) then (i,j)th entry of R(G) is 1didj and 0 elsewhere.

    Definition 2.5 (Sum-connectivity energy). [8] The sum-connectivity energy ESC of a simple connected graph G is define as the sum of the absolute eigenvalues of the sum-connectivity matrix SC(G) where (i,j)th entry of SC(G) is 1di+dj if vivjE(G) and 0 otherwise.

    Definition 2.6 (First Zagreb energy). [9] The first Zagreb energy ZE1 of a simple connected graph G is define as the sum of the absolute eigenvalues of first Zagreb matrix Z(1)(G) of G where Z(1)(G) has (i,j)th entry di+dj if vivjE(G) and 0 otherwise.

    Definition 2.7 (Second Zagreb energy). [9] The second Zagreb energy ZE2 of a simple connected graph G is define as the sum of the absolute eigenvalues of second Zagreb matrix Z(2)(G) of G where Z(2)(G) has (i,j)th entry di.dj if vivjE(G) and 0 otherwise.

    In the following theorem, we give bounds of all above defined degree energies;

    Theorem 2.8. Let p and q be vertices and edges of a regular graph G. Then

    1. for maximum degree energy, we have EM(S(G))2s2pq;

    2. for minimum degree energy, we have Em(S(G))42pq,

    3. for Randiˊc energy, we have ER(S(G))4pqs,

    4. for sum-connectivity energy, we have ESC(S(G))22pq2+s,

    5. for first Zagreb energy, we have ZE1(S(G))2(s+2)2pq,

    6. for second Zagreb energy, we have ZE2(S(G))4s2pq.

    Proof. Let the incidence matrix of G is C(G). Note that the degree matrix of the subdivision graph S(G) can be stated as:

    M(S(G))=[0IptC(G)tCT(G)0Iq]. (2.1)

    1. By taking t=s in Eq (2.1), we have following computations for the maximum degree energy of the subdivision graph S(G);

    EM(S(G))=p+qj=1|αi[0IpsC(G)sCT(G)0Iq]|=s(p+qj=1αj[0IpC(G)CT(G)0Iq]).

    As in [12] CCT=L+(G), we have

    p+qj=1νj[0IpC(G)CT(G)0Iq]=2pj=1ν+j(G).

    where L+(G) is signless Laplacian matrix and ν+j are eigenvalues of L+(G). Thus by Cauchy Schawaz inequality

    pj=1ν+j(G)ppj=1ν+j(G)=2pq.

    Hence,

    EM(S(G))2s2pq.

    2. By taking t=2 in Eq (2.1), we have following computations for the minimum degree energy of the subdivision graph S(G);

    Em(S(G))=p+qj=1|νj[0Ip2C(G)2CT(G)0Iq]|.

    Since,

    p+qj=1|νj[0Ip2C(G)2CT(G)0Iq]|42pq.

    Therefore,

    Em(S(G))42pq.

    3. By taking t=12s in Eq (2.1), we have following computations for the Randić energy of the subdivision graph S(G);

    ER(S(G))=p+qj=1|ρj(0Ip12s[C(G)]12s[CT(G)]0Iq)|=12sp+qj=1|ρj(0Ip[C(G)][CT(G)]0Iq)|.

    As

    p+qj=1|ρj[0IpC(G)[CT(G)]0Iq]|22pq.

    Therefore,

    ER(S(G))12s.22pq=4pqs.

    4. By taking t=12+s in Eq (2.1), we have following computations for the sum-connectivity energy of the subdivision graph S(G);

    ESC(S(G))=12+sp+qj=1|ηj[0IpC(G)CT(G)0Iq]|.

    As

    p+qj=1|ηj[0IpC(G)CT(G)0Iq]|22pq.

    Hence,

    ESC(S(G))12+s22pq=22pq2+s.

    5. By taking t=s+2 in Eq (2.1), we have following computations for the first Zagreb energy of the subdivision graph S(G);

    ZE1(S(G))=(s+2)p+qj=1|νj[0IpC(G)CT(G)0Iq]|(s+2).22pq.

    as

    p+qj=1|νj[0IpC(G)CT(G)0Iq]|22pq.

    Hence,

    ZE1(S(G))2(s+2)2pq.

    6. By taking t=2s in Eq (2.1), we have following computations for the second Zagreb energy energy of the subdivision graph S(G);

    ZE2(S(G))=2sp+qj=1|zj[0IpC(G)CT(G)0Iq]|2s[22pq].

    where

    p+qj=1|zj[0IpC(G)CT(G)0Iq]|[22pq]

    Hence,

    ZE2(S(G))4s2pq.

    Definition 2.9 (Seidel energy). [10] The Seidel energy ESE of a simple connected graph G as the sum of the absolute eigenvalues of the seidel matrix SE(G) of G. Here SE(G)=[sij] where

    sij={1,ifviandvjareadjacentandij1,ifviandvjarenonadjacentandij0,ifi=j

    Theorem 2.10. For an s-regular (p,q) graph G,

    ESE(S(G))2(p+q)+2spq4.

    Proof. Let u1,u2,u3,...,up be vertices of an s-regular graph G and let uj for 1jq be vertices that are added at all edges of G to gain S(G). Note that SE(S(G)) is given as:

    SE(S(G))=[JpIpEp×qEq×pJqIq].

    where Ep×q=[epq] such that

    epq={1,ifvpandvqareadjacent1,Otherwise

    Therefore

    ESE(S(G))pj=1|νj[JpIq]|+p+qj=1|νj[0IpEp×qEq×p0Iq]|+qj=1|νj[JqIq]|.

    As

    pj=1|νj[JpIp]|2(p1),
    qj=1|νj[JqIq]|2(q1),

    and

    p+qj=1|νj[0IpEp×qEq×p0Iq]|2spq.

    Hence,

    ESE(S(G))2(p1)+2spq+2(q1),=2(p+q)+2spq4.

    Definition 2.11 (Degree sum energy). [11] The degree sum energy EDS of a simple connected graph G is define as the sum of the absolute eigenvalues of the degree sum matrix DS(G) of G where DS(G) has (i,j)th entry di+dj if ij and 0 otherwise.

    Theorem 2.12. For a s-regular graph G having p and q as order and size respectively,

    EDS(S(G))4s(p1)+2(s+2)pq+8(q1).

    Proof. Let G has vertices w1,w2,w3,...,wp and wj for 1jq be the vertices that are added at every edge of G to acquire S(G). Then

    DS(S(G))=w1w2w3wpw1w2w3wqw1w2w3wpw1w2w3wq(02s2s2ss+2s+2s+2s+22s02s2ss+2s+2s+2s+22s2s02ss+2s+2s+2s+22s2s2s0s+2s+2s+2s+2s+2s+2s+2s+20444s+2s+2s+2s+24044s+2s+2s+2s+24404+2s+2s+2s+24440).

    Or

    DS(S(G))=[2s[JpIp](s+2)[Jp×q](s+2)[Jq×p]4[JqIq]].

    Therefore

    EDS(S(G))pj=1|μj[2s[JpIp]0Jp×q0Jq×p0[JqIq]]|+p+qj=1|μj[0Ip(s+2)Jp×q(s+2)Jq×p0[JqIq]]|+qj=1|μj[0Ip0Jp×q0Jq×p4[JqIq]]|
    EDS(S(G))2spj=1|μj[[JpIp]0Jp×q0Jq×p0[JqIq]]|+(s+2)p+qj=1|μj[0IpJp×qJq×p0[JqIq]]|+4qj=1|μj[0Ip0Jp×q0Jq×p[JqIq]]|

    Hence,

    EDS(S(G))2s[2(n1)]+(s+2)[2pq]+4[2(q1)],=4s(p1)+2(s+2)pq+8(q1).

    Definition 2.13 (Degree square sum energy). [12] The degree square sum energy EDSS of a simple connected graph G is define as the sum of the absolute eigenvalues of the degree square sum matrix DSS(G) of G where DSS(G) has (i,j)th entry d2i+d2j if ij and 0 otherwise.

    Theorem 2.14. For an s-regular graph G

    EDSS(S(G))4s2(p1)+2(s2+4)pq+16(q1).

    Proof. Let for 1jp, uj be vertices of G and uk for 1kq be the vertices that are added in G to get S(G). Note that the degree square sum matrix of S(G) is denoted by DSS(S(G)) and is given as:

    u1u2u3upu1u2u3uqu1u2u3upu1u2u3uq(02s22s22s2s2+4s2+4s2+4s2+42s202s22s2s2+4s2+4s2+4s2+42s22s202s2s2+4s2+4s2+4s2+42s22s22s20s2+4s2+4s2+4s2+4s2+4s2+4s2+4s2+40888s2+4s2+4s2+4s2+48088s2+4s2+4s2+4s2+48808s2+4s2+4s2+4s2+48880).

    Or

    DSS(S(G))=[2s2[JpIp](s2+4)[Jp×q](s2+4)[Jq×p]8[JqIq]].

    Therefore

    EDSS(S(G))pj=1|μj[2s2[JpIp]0Jp×q0Jq×p0[JqIq]]|+p+qj=1|μj[0Ip(s2+4)Jp×q(s2+4)Jq×p0[JqIq]]|+qj=1|μj[0Ip0Jp×q0Jq×p8[JqIq]]|

    Or

    EDSS(S(G))2s2pj=1|μj[[JpIp]0Jp×q0Jq×p0[JqIq]]|+(s2+4)p+qj=1|μj[0IpJp×qJq×p0[JqIq]]|+8qj=1|μj[0Ip0Jp×q0Jq×p[JqIq]]|

    Hence,

    EDSS(S(G))2s2[2(p1)]+(s2+4)[2pq]+8[2(q1)],=4s2(p1)+2(s2+4)pq+16(q1).

    A complete graph denoted by Kp is a simple undirected graph in which every pair of distinct vertices is connected by a unique edge. K5 is shown in Figure 2.

    Figure 2.  K5.

    We have following trivial results about energies of complete graphs.

    Theorem 3.1. For the complete graph Kp, the maximum degree energy is

    EM(Kp)=2(p1)2.

    Theorem 3.2. For the complete graph Kp, the minimum degree energy is

    Em(Kp)=2(p1)2.

    Theorem 3.3. For the complete graph Kp, the Randić energy is

    ER(Kp)=2.

    Theorem 3.4. For the complete graph Kp, the Seidel energy is

    ESE(Kp)=2(p1)=2(p1)).

    Theorem 3.5. For the complete graph Kp, the sum-connectivity energy is

    ESC(Kp)=2(p1).

    Theorem 3.6. For the complete graph Kp, the degree sum energy is

    EDS(Kp)=4(p1)2.

    Theorem 3.7. For the complete graph Kp, the degree square sum energy is

    EDSS(Kp)=4(p1)3.

    Theorem 3.8. For the complete graph Kp, the first Zagreb energy is

    ZE1(Kp)=4(p1)2.

    Theorem 3.9. For the complete graph Kp, the second Zagreb energy is

    ZE2(Kp)=2(p1)3.

    In this paper we gave bounds of maximum degree energy, Randiˊc energy, sum-connectivity energy etc of s-regular subdivision graph S(G). Also various graph energies of complete graph are mentioned in this article. In future, we aim to study graph energies for the other families of graphs.

    Authors do not have any competing interests.



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