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Introduction

In: Graph Energy

Author

Listed:
  • Xueliang Li

    (Nankai University, Center for Combinatorics)

  • Yongtang Shi

    (Nankai University, Center for Combinatorics)

  • Ivan Gutman

    (University of Kragujevac, Faculty of Science)

Abstract

Let G be a finite and undirected simple graph, with vertex set V (G) and edge set E(G). The number of vertices of G is n, and its vertices are labeled by v 1,v 2,…,v n . The adjacency matrix A(G) of the graph G is a square matrix of order n, whose (i,j)-entry is equal to 1 if the vertices v i and v j are adjacent and is equal to zero otherwise. The characteristic polynomial of the adjacency matrix, i.e., det(x I n −A(G)), where I n is the unit matrix of order n, is said to be the characteristic polynomial of the graph G and will be denoted by ϕ(G,x). The eigenvalues of a graph G are defined as the eigenvalues of its adjacency matrix A(G), and so they are just the roots of the equation ϕ(G,x)=0. Since A(G) is symmetric, its eigenvalues are all real. Denote them by λ1,λ2,…,λ n , and as a whole, they are called the spectrum of G and denoted by Spec(G).

Suggested Citation

  • Xueliang Li & Yongtang Shi & Ivan Gutman, 2012. "Introduction," Springer Books, in: Graph Energy, edition 127, chapter 0, pages 1-9, Springer.
  • Handle: RePEc:spr:sprchp:978-1-4614-4220-2_1
    DOI: 10.1007/978-1-4614-4220-2_1
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