A note on (local) energy of a graph

B. R. Rakshith, Kinkar Chandra Das
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Abstract

Let G be a simple graph with vertex set \(V(G)\,(|V(G)|=n)\) and let \(S\subseteq V(G)\). We denote by \(d_{i}\), the degree of the vertex \(v_{i}\). The graph \(G^{S}\) is obtained from G by removing all the vertices belonging to S (If \(S=\{v_j\}\), then \(G^S\) is denoted by \(G^{(j)}\)). The energy of G is the sum of all absolute values of the eigenvalues of the adjacency matrix A(G) and is denoted by \({\mathcal {E}}(G)\). Recently, Espinal and Rada (MATCH Commun Math Comput Chem 92(1):89–103, 2024) introduced the concept of local energy of a graph e(G). It is defined as \(e(G)=\sum ^n_{j=1}\,\mathcal {E}_{G}(v _j)\), where \(\mathcal {E}_{G}(v_j)=\mathcal {E}(G)-\mathcal {E}(G^{(j)})\) is called the local energy of a graph G at vertex \(v_j\). In this paper, we prove that if \(v_{1}\in S\) and S is a vertex independent set of size k such that every vertex in S share the same open neighborhood set \(N_{G}(v_{1})\), then \(\mathcal {E}(G)-\mathcal {E}(G^{S})\le 2\,\sqrt{k\,d_{1}}\). We also characterize graphs that satisfy the equality case. If \(S=\{v_{1}\}\), we get \(\mathcal {E}(G)-\mathcal {E}(G^{(1)})\le 2\,\sqrt{d_{1}}\) Espinal and Rada (MATCH Commun Math Comput Chem 92(1):89–103, 2024). One of the open problems in the study of local energy of a graph is to characterize graphs with \(e(G)=2\mathcal {E}(G)\). Motivated by this problem, we present an infinite class of graphs for which \(e(G)<2\mathcal {E}(G)\). As a result, we show that for a complete multipartite graph G, \(e(G)=2\mathcal {E}(G)\) if and only if \(G\cong K_{2}\). We also prove that the local energy of a complete multipartite graph G is constant at each vertex of the graph if and only if G is regular. Finally, we give an upper bound on e(G) in terms of n and chromatic number k.

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关于图形(局部)能量的说明
让 G 是一个简单图,它的顶点集是 \(V(G)\,(|V(G)|=n)\) 并且让 \(S\subseteq V(G)\).我们用 \(d_{i}\)表示顶点 \(v_{i}\)的度数。图 \(G^{S}\) 是通过删除所有属于 S 的顶点从 G 得到的(如果 \(S=\{v_j\}\), 那么 \(G^S\) 表示为 \(G^{(j)}\))。G 的能量是邻接矩阵 A(G) 所有特征值的绝对值之和,用 \({\mathcal {E}}(G)\) 表示。最近,Espinal 和 Rada(MATCH Commun Math Comput Chem 92(1):89-103, 2024)引入了图 e(G) 的局部能量概念。它的定义是 \(e(G)=\sum ^n_{j=1}\,\mathcal {E}_{G}(v _j)\), 其中 \(\mathcal {E}_{G}(v_j)=\mathcal {E}(G)-\mathcal {E}(G^{(j)})\) 被称为图 G 在顶点 \(v_j\) 处的局部能量。在本文中,我们证明如果 \(v_{1}\in S\) 和 S 是大小为 k 的顶点独立集合,使得 S 中的每个顶点共享同一个开放邻域集合 \(N_{G}(v_{1})\),那么 \(\mathcal {E}(G)-\mathcal {E}(G^{S})\le 2\,\sqrt{k\,d_{1}}\).我们还描述了满足相等情况的图的特征。如果 \(S=\{v_{1}\}), 我们得到 \(\mathcal {E}(G)-\mathcal {E}(G^{(1)})\le 2\,\sqrt{d_{1}}\})Espinal 和 Rada (MATCH Commun Math Comput Chem 92(1):89-103, 2024).图的局部能量研究中的一个未决问题是描述具有 \(e(G)=2\mathcal {E}(G)\) 的图的特征。受这个问题的启发,我们提出了一类无限图,对于这类图,\(e(G)<2\mathcal {E}(G)\).因此,我们证明了对于一个完整的多方图 G,当且仅当 \(G\cong K_{2}\) 时,\(e(G)=2\mathcal {E}(G)\) 。我们还证明,当且仅当 G 是正则图时,完整多方图 G 的每个顶点的局部能量是常数。最后,我们用 n 和色度数 k 给出了 e(G) 的上界。
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来源期刊
自引率
11.50%
发文量
352
期刊介绍: Computational & Applied Mathematics began to be published in 1981. This journal was conceived as the main scientific publication of SBMAC (Brazilian Society of Computational and Applied Mathematics). The objective of the journal is the publication of original research in Applied and Computational Mathematics, with interfaces in Physics, Engineering, Chemistry, Biology, Operations Research, Statistics, Social Sciences and Economy. The journal has the usual quality standards of scientific international journals and we aim high level of contributions in terms of originality, depth and relevance.
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