| Literature DB >> 36235303 |
Xuewu Zuo1, Bilal Ahmad Rather2, Muhammad Imran2, Akbar Ali3.
Abstract
Let G be a simple graph with the vertex set V={v1,…,vn} and denote by dvi the degree of the vertex vi. The modified Sombor index of G is the addition of the numbers (dvi2+dvj2)-1/2 over all of the edges vivj of G. The modified Sombor matrix AMS(G) of G is the n by n matrix such that its (i,j)-entry is equal to (dvi2+dvj2)-1/2 when vi and vj are adjacent and 0 otherwise. The modified Sombor spectral radius of G is the largest number among all of the eigenvalues of AMS(G). The sum of the absolute eigenvalues of AMS(G) is known as the modified Sombor energy of G. Two graphs with the same modified Sombor energy are referred to as modified Sombor equienergetic graphs. In this article, several bounds for the modified Sombor index, the modified Sombor spectral radius, and the modified Sombor energy are found, and the corresponding extremal graphs are characterized. By using computer programs (Mathematica and AutographiX), it is found that there exists only one pair of the modified Sombor equienergetic chemical graphs of an order of at most seven. It is proven that the modified Sombor energy of every regular, complete multipartite graph is 2; this result gives a large class of the modified Sombor equienergetic graphs. The (linear, logarithmic, and quadratic) regression analyses of the modified Sombor index and the modified Sombor energy together with their classical versions are also performed for the boiling points of the chemical graphs of an order of at most seven.Entities:
Keywords: Sombor index; adjacency matrix; correlation; modified Sombor energy; modified Sombor matrix
Year: 2022 PMID: 36235303 PMCID: PMC9572862 DOI: 10.3390/molecules27196772
Source DB: PubMed Journal: Molecules ISSN: 1420-3049 Impact factor: 4.927
Figure 1Double star-type graph on 16 vertices and the chain graph on 10 vertices.
Table showing value of modified Sombor index for some graphs, numerical values of the bounds obtained in Propositions 1 and 3, and the different results of Huang and Liu [16].
| Graph |
| Propositions 1 | Propositions 3 | Theorem 2.1 | Corollary 2.3 | Corollary 2.4 |
|---|---|---|---|---|---|---|
|
| 4.78351 | 4.89003 | 4.80364 | 4.88908 | 6.05761 | 4.94975 |
|
| 2.75387 | 2.78203 | 2.76018 | 2.80299 | 4.49642 | 2.82843 |
|
| 4.70027 | 5.01065 | 5.06802 | 5.30254 | 6.78914 | 5.65685 |
|
| 1.31329 | 1.66039 | 1.36239 | 2.18222 | 2.12132 | 2.12132 |
|
| 2.82008 | 3.22145 | 2.84684 | 3.22319 | 4.66404 | 3.53553 |
| Graph |
| Theorem 2.7 | Cor. 2.8 | Theorem 2.16 | Corollary 2.18 | Corollary 2.21 |
|
| 4.78351 | 9.19239 | 9.89949 | 8.13909 | 9.1115 | 5.0104 |
|
| 2.75387 | 3.53553 | 3.9598 | 7.38738 | 3.50586 | 2.782 |
|
| 4.70027 | 10.6060 | 28.28443 | 9.01171 | 9.92488 | 5.14324 |
|
| 1.31329 | 4.24264 | 10.6066 | 3.44814 | 3.566 | 1.85567 |
|
| 2.82008 | 10.6066 | 17.6777 | 6.82982 | 9.96694 | 3.71687 |
Modified Sombor energy and the approximate values of the upper bounds obtained in this article.
|
|
| Theorem 2 (i) | Theorem 2 (ii) | Theorem 3 | Corollary 2 |
|---|---|---|---|---|---|
|
| 6.38433 | 7.01418 | 7.04982 | 7.04982 | NA |
|
| 1.39101 | 1.66237 | 2.20814 | 2.56084 | 1.50819 |
|
| 1.40331 | 2.39582 | 3.00054 | 3.14352 | 1.69421 |
|
| 5.29907 | 5.81504 | 5.8599 | 5.86874 | NA |
|
| 1.60161 | 2.03389 | 2.098059 | 2.19134 | NA |
|
| 1.41422 | 1.41422 | 2.55841 | 3.33034 | 1.44457 |
Modified Sombor energy and the approximate values of the lower bounds obtained in the present paper and Theorem 3.6 of [16].
|
|
| Theorem 1 (i) | Theorem 1 (ii) | Theorem 4 | Theorem 5 | Theorem 3.6 [ |
|---|---|---|---|---|---|---|
|
| 6.38433 | 1.36672 | 1.00712 | 2.66458 | 3.0726 | 5.80258 |
|
| 1.39101 | 1.37694 | 0.552036 | 1.10407 | 1.27336 | 0.967999 |
|
| 1.40331 | 1.39786 | 0.50009 | 1.22496 | 1.40331 | 1.22496 |
|
| 5.29907 | 1.36923 | 0.976651 | 2.3923 | 2.76237 | 4.77683 |
|
| 1.60161 | 0.94144 | 0.599442 | 1.12145 | 1.29488 | 1.25262 |
|
| 1.41422 | 1.41421 | 0.426402 | 1.04447 | 1.1028 | 0.805388 |
Figure 2Three pairs of equienergetic chemical graphs of the order of at most 7, namely , , and . Among these three pairs, and are neither Sombor equienergetic graphs nor modified Sombor equienergetic graphs.
Approximate values of the energy, Sombor energy, and modified Sombor energy of the graphs depicted in Figure 2.
| Energy |
|
|
|
|
|
|
|---|---|---|---|---|---|---|
|
| 4 | 4 | 9.62721 | 9.62721 | 7.72741 | 7.72741 |
|
| 11.3137 | 16.4924 | 32.3713 | 32.3713 | 22.3639 | 27.5959 |
|
| 1.41421 | 0.970143 | 2.90798 | 2.90798 | 2.74436 | 2.34164 |
Correlation of the boiling points (Bp) with each of the following topological indices for the case of all chemical graphs of the order of at most 7: Sombor index, Sombor energy, modified Sombor index, and modified Sombor energy.
|
|
|
|
|
|---|---|---|---|
| 0.720862158 | 0.809447751 | 0.943525603 | 0.842522597 |
Figure 3The scattering of (boiling points) with each of the topological indices and for the linear, logarithmic, and quadratic regressions along with the regression equations and (coefficient of determination).
The coefficient of determination of the boiling points with the topological indices , , and for the linear, logarithmic, and quadratic regressions.
| Topological Index | Linear | Logarithmic | Quadratic |
|---|---|---|---|
|
| 0.5196 | 0.3069 | 0.7136 |
|
| 0.6552 | 0.4624 | 0.8119 |
|
| 0.8902 | 0.8433 | 0.933 |
|
| 0.7098 | 0.6742 | 0.7746 |