Please use this identifier to cite or link to this item: https://scidar.kg.ac.rs/handle/123456789/11106
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dc.contributor.authordas, kinkar-
dc.contributor.authorGutman, Ivan-
dc.contributor.authorMilovanović I.-
dc.contributor.authorMilovanovíc E.-
dc.contributor.authorFurtula, Boris-
dc.date.accessioned2021-04-20T17:30:50Z-
dc.date.available2021-04-20T17:30:50Z-
dc.date.issued2018-
dc.identifier.issn0024-3795-
dc.identifier.urihttps://scidar.kg.ac.rs/handle/123456789/11106-
dc.description.abstract© 2018 Elsevier Inc. Let G=(V,E) be a simple graph of order n and size m, with vertex set V(G)={v1,v2,…,vn}, without isolated vertices and sequence of vertex degrees Δ=d1≥d2≥⋯≥dn=δ>0, di=dG(vi). If the vertices vi and vj are adjacent, we denote it as vivj∈E(G) or i∼j. With TI we denote a topological index that can be represented as TI=TI(G)=∑i∼jF(di,dj), where F is an appropriately chosen function with the property F(x,y)=F(y,x). A general extended adjacency matrix A=(aij) of G is defined as aij=F(di,dj) if the vertices vi and vj are adjacent, and aij=0 otherwise. Denote by fi, i=1,2,…,n the eigenvalues of A. The “energy” of the general extended adjacency matrix is defined as ETI=ETI(G)=∑i=1n|fi|. Lower and upper bounds on ETI are obtained. By means of the present approach a plethora of earlier established results can be obtained as special cases.-
dc.rightsrestrictedAccess-
dc.sourceLinear Algebra and Its Applications-
dc.titleDegree-based energies of graphs-
dc.typearticle-
dc.identifier.doi10.1016/j.laa.2018.05.027-
dc.identifier.scopus2-s2.0-85048493950-
Appears in Collections:Faculty of Science, Kragujevac

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