Laplacian energy of partial complement of a graph

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Abstract

The energy of the graph had its genesis in 1978. It is the sum of absolute values of its eigenvalues. It originates from the π -electron energy in the Huckel molecular orbital model but has also gained purely mathematical interest. Suppose μ12,…,μn is the Laplacian eigenvalues of G. The Laplacian energy of G has recently been defined as LE(G)=∑i=1nμi-[Formula presented]. In this paper, we define Laplacian energy of partial complements of a graph. Laplacian energy and spectrum of partial complements of the few classes of graphs are established. Some bounds and properties of Laplacian energy are obtained.

Original languageEnglish
Pages (from-to)827-831
Number of pages5
JournalMaterials Today: Proceedings
Volume54
DOIs
Publication statusPublished - 01-2022

All Science Journal Classification (ASJC) codes

  • Materials Science(all)

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