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 μ1,μ2,…,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 language | English |
|---|---|
| Pages (from-to) | 827-831 |
| Number of pages | 5 |
| Journal | Materials Today: Proceedings |
| Volume | 54 |
| DOIs | |
| Publication status | Published - 01-2022 |
All Science Journal Classification (ASJC) codes
- General Materials Science
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