Bounds on the $\alpha$-distance spectrum of graphs
Yang Yang, Lizhu Sun, Changjiang Bu

TL;DR
This paper introduces bounds on the spectral radius, energy, and Estrada index related to the $ ext{alpha}$-distance matrix of graphs, expanding spectral graph theory with new spectral bounds and indices.
Contribution
It defines the $ ext{alpha}$-distance Estrada index and provides bounds on its spectral radius, energy, and Estrada index, advancing the understanding of spectral properties of $ ext{alpha}$-distance matrices.
Findings
Bounds on the spectral radius of $D_{\alpha}(G)$
Bounds on the $\alpha$-distance energy of $G$
Bounds on the $\alpha$-distance Estrada index
Abstract
For a simple, undirected and connected graph , is called the -distance matrix of , where , is the distance matrix of , and is the vertex transmission diagonal matrix of . Recently, the -distance energy of was defined based on the spectra of . In this paper, we define the -distance Estrada index of in terms of the eigenvalues of . And we give some bounds on the spectral radius of , -distance energy and -distance Estrada index of .
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Taxonomy
TopicsGraph theory and applications · Matrix Theory and Algorithms · Synthesis and Properties of Aromatic Compounds
Bounds on the -distance spectrum of graphs
Yang Yang11footnotemark: 1
Lizhu Sun22footnotemark: 2
Changjiang Bua,b
College of Automation,, Harbin Engineering University, Harbin 150001, PR China
College of Mathematical Sciences, Harbin Engineering University, Harbin 150001, PR China
Abstract
For a simple, undirected and connected graph , is called the -distance matrix of , where , is the distance matrix of , and is the vertex transmission diagonal matrix of . Recently, the -distance energy of was defined based on the spectra of . In this paper, we define the -distance Estrada index of in terms of the eigenvalues of . And we give some bounds on the spectral radius of , -distance energy and -distance Estrada index of .
keywords:
Distance matrix, Energy of graph, Estrada index, -distance spectra
MSC:
[2010] 05C50
1 Introduction
1.1 Distance spectrum of graphs
In this paper, we consider the simple, undirected and connected graphs. Let , be a graph with the vertex set and edge set . The distance between two vertices is the length of the shortest path between and , denoted by . The Wiener index of the graph is the sum of the distances between all pairs of vertices in , i.e., The matrix with entries is called the distance matrix of , where . The spectra of is called the distance spectra of .
The study of the distance spectra arises from the work of R. Graham and H.O. Pollack in 1971 (see [11]). In [11], the determinant of the distance matrix of a tree was given as , where . And Graham and Pollack proved has positive eigenvalue and negative eigenvalues. In 1978, Graham and Lovász established the representation for the inverse of (see [10]). The distance spectrum of graphs has attracted much attention [27].
1.2 -spectrum of graphs
The adjacency matrix of the graph is , where if , and otherwise. The Laplacian matrix and signless Laplacian matrix of are
[TABLE]
respectively, where and is the degree of , .
It is well-known that the spectrum of the adjacency matrix, Laplacian matrix and signless Laplacian matrix of a graph were widely investigated [5]. In 2013, the study of the spectrum of Laplacian matrix and signless Laplacian matrix was extended to distance Laplacian matrices and distance signless Laplacian matrices defined as in Equation (1) (see [1]). In 2016, the study of the spectrum of Laplacian matrix and signless Laplacian matrix was generalized to a convex combination of and defined as (see [24]). Recently, the above study was further extended to the -distance matrices defined as in Equation (2) (see [3]).
For a vertex , the sum of the distances between and all the other vertices in is called the transimission of , denoted by , that is
[TABLE]
A graph is said to be transmission regular if the transimissions of all the vertices in are equal. In 2013, Aouchiche and Hansen [1] defined the distance Laplacian matrix and distance signless Laplacian matrix of the graph ,
[TABLE]
where .
For a transmission regular graph , the characteristic polynomials of and were calculated in [1]. In [21,28,29], the bounds on the spectral radii for the distance signless Laplacian matrix of trees, unicyclic graphs and bicyclic graphs were characterized, respectively.
In [3], the -distance matrix of a graph
[TABLE]
was defined. Clearly, , and . The spectra of is called the -distance spectra of . Since is a real symmetric matrix, the eigenvalues of are real. Let be the eigenvalues of . And let be the spectral radius of . We know that is a nonnegative weakly irreducible matrix. From the Perron-Frobenius Theorem, we have . And is positive semidefiniteness for .
In [3], upper and lower bounds for the spectral radius of the -distance matrix were established. In [4], authors characterized the unique graph with minimum spectral radius of the -distance matrix among the connected graphs with fixed chromatic number. In [20], a lower bound on the -th smallest eigenvalue of the -distance matrix was given. In [14], the bounds on the spectral radius of the -distance matrix were established.
1.3 -distance energy of graphs
Let , and be the eigenvalues of , and respectively, where and . The energy of is (see [12,13]). The sum is called the distance energy of (see [17]), and is called the distance signless Laplacian energy [6].
Graph energy has important applications in the fields of mathematics and chemistry. There are many researches on the above kinds of graph energy. Scholars gave the bounds on the energy of graphs, for example the McClelland bounds [23], Koolen-Moulton bounds [18] and so on [2]. In [17], the distance energy of some graphs were calculated.
Recently, Zhou extended the concept of graph energy to a more general form called -distance energy
[TABLE]
where is the eigenvalue of , , (see [14]). Clearly, and .
1.4 Main work
In this paper, we give some bounds on the -distance energy of graphs and stars in terms of the parameter and the vertex number. And we establish some bounds for the spectral radius of the -distance matrix by using the transimission of vertices and Wiener index. Further, we define the -distance Estrada index of a graph, and obtain some bounds on the -distance Estrada index.
2 Some bounds for the -distance energy of graphs
To begin with this section, we introduce some notations. The average transmission of the graph , denoted by , is defined by
[TABLE]
where . Clearly, Let (see [3]).
Lemma 2.1**.**
[3]* Let be a graph with vertices. Then*
[TABLE]
the equality holds if and only if is a transmission regular graph.
For a graph and , let .
Lemma 2.2**.**
[3]* Let be a graph with vertices. Let be a subset of such that for any .
(1) If is an independent set, then is a constant for each , and has as an eigenvalue with multiplicity at least .
(2) If is a clique, then is a constant for each , and has as an eigenvalue with multiplicity at least .*
From Lemma 2.2, we have the following result.
Proposition 2.3**.**
For a graph , () has two distinct eigenvalues if and only if is a complete graph.
Let be a star with vertices.
Lemma 2.4**.**
[4,14,20]* Let be a tree with vertices. Then*
[TABLE]
the equality holds if and only if .
Proposition 2.5**.**
*The -distance spectra of consists of
(1) with multiplicity ;
(2) .*
Proof.
Since satisfies the statement (1) of Lemma 2.2, and the number of the vertices in the independent set is and the transimission of each vertex in the independent set is , we have is an eigenvalue of with multiplicity at least . From Lemma 2.4, the statement (2) holds. ∎
Let be a complete graph with vertices.
Lemma 2.6**.**
[9]* Let be a graph with vertices. Then*
[TABLE]
the equality holds if and only if .
Next, we give some bounds for the -distance energy of a graph and characterize the -distance energy of by using the parameter and the vertex number.
Theorem 2.7**.**
Let be a connected graph with vertices. Then
[TABLE]
the equality holds if and only if .
Proof.
Let be the eigenvalues of . It is easy to see that
[TABLE]
Lemma 2.1 gives . Suppose that is the largest number such that . And it follows from Equation (3) that
[TABLE]
From Lemmas 2.1 and 2.6, we have
[TABLE]
and if and only if . ∎
Theorem 2.8**.**
The -distance energy of is
[TABLE]
Proof.
We know that And from Proposition 2.5, we obtain
[TABLE]
∎
Let denote the Frobenius norm of a matrix , that is
[TABLE]
We know that , where are the eigenvalues of . For a graph with vertices,
[TABLE]
where are the eigenvalues of (see [7,8]). Similarly to the above equation, we have
[TABLE]
where are the eigenvalues of .
Lemma 2.9**.**
[8]* Let be a graph with vertices. Then*
[TABLE]
From Lemma 2.9, the following result can be obtained directly.
Proposition 2.10**.**
Let be a connected graph with vertices. Then
[TABLE]
In the following, we establish some bounds for the -distance energy of a graph by using the Frobenius norm of , transmissions of vertices and .
Theorem 2.11**.**
Let be a graph with vertices. Then
[TABLE]
where .
Proof.
Let , where . Clearly, From Equation (4), we have
[TABLE]
Let By Cauchy-Schwars inequality, we have
[TABLE]
∎
Lemma 2.12**.**
[3]* Let be a graph with vertices. Then*
[TABLE]
where are the eigenvalues of .
Theorem 2.13**.**
Let be a graph with vertices. Then
[TABLE]
Proof.
From Cauchy-Schwars inequality we have
[TABLE]
It follows from Lemma 2.12 that
[TABLE]
∎
3 Bounds for the -distance spectrum of graphs
Lemma 3.14**.**
[8]* Let be real numbers. Then*
[TABLE]
where .
It follows from the above lemma the following result holds directly.
Proposition 3.15**.**
For a graph with vertices, let be the largest eigenvalue of . For ,
[TABLE]
For a matrix , let be the -th row sum of , .
Lemma 3.16**.**
[7,19]* Let be a nonnegative matrix. Let be the spectral radius of . Then*
[TABLE]
Further, if is an irreducible matrix, then the above two equalities hold if and only if .
From the above Lemma, it is easy to see the following result holds.
Proposition 3.17**.**
Let be a graph with vertices. Let be the spectral radius of . Then
[TABLE]
the equality holds if and only if is a transmission regular graph.
Lemma 3.18**.**
[22]* For a graph with vertices, let be the largest eigenvalue of the signless Laplacian matrix . Let be a polynomial on . Then*
[TABLE]
Moreover, if the row sums of are not all equal, then both inequalities are strict.
Inspired by the above result, we give the following bounds on the largest eigenvalue of .
Proposition 3.19**.**
For a graph with vertices, let be the largest eigenvalue of . Let be a polynomial on . For ,
[TABLE]
If the row sums of are not all equal, then both inequalities are strict.
Proof.
Perron-Frobenius Theorem gives that there exists a positive vector such that . Then
[TABLE]
Let . Then
[TABLE]
Hence,
[TABLE]
∎
Lemma 3.20**.**
For a graph with vertices, let and . Then for each vertex ,
[TABLE]
Proof.
By calculation, we have
[TABLE]
Similarly,
[TABLE]
∎
Theorem 3.21**.**
For a graph with vertices, let and . Let be the largest eigenvalue of , where . Then for ,
[TABLE]
Proof.
Let be an unity vector whose -component is . And let be a vector whose components are all . Then
[TABLE]
From Lemma 3.7, we have
[TABLE]
and
[TABLE]
Let . Then the sum of the entries in the -th row of is
[TABLE]
Clearly,
[TABLE]
By Proposition 3.6, we obtain
[TABLE]
that is
[TABLE]
Similarly, let . Then
[TABLE]
∎
Lemma 3.22**.**
[26]* let be real numbers such that . Then*
[TABLE]
the equality holds if and only if .
Theorem 3.23**.**
Let be a graph with vertices. Then
[TABLE]
the equality holds if and only if .
Proof.
Obviously,
[TABLE]
It follows from Lemma 3.9 that
[TABLE]
and the equality holds if and only if
[TABLE]
By calculation, we know
[TABLE]
Then
[TABLE]
and the equality holds if and only if . And it follows from Proposition 2.3 that the equality holds if and only if . ∎
For an matrix and order partition of the ordered set , can be denoted as a partition matrix
[TABLE]
where has as the set of its row indices and as the set of its column indices, Let be the quotient matrix of the partitioned matrix , which is defined to be an matrix with the -entry , where (see [5] ).
Lemma 3.24**.**
[16]* Suppose is a quotient matrix of a symmetric partitioned matrix . Let and be the eigenvalue sets of and , respectively. Then for ,*
[TABLE]
Proposition 3.25**.**
Let be a graph with vertices. Let and be the largest and the smallest eigenvalue of , respectively. Then for each ,
[TABLE]
Proof.
Let and be a partition of . Then the following is the corresponding quotient matrix of ,
[TABLE]
Let and be the eigenvalue sets of and , respectively. It follows from Lemma 3.11 that
[TABLE]
where . Hence,
and .
Then
[TABLE]
Since , we obtain
[TABLE]
[TABLE]
[TABLE]
∎
Let be a graph with vertices. Let be the eigenvalue set of . And is called the Estrada index of . It is well-known that Estrada index plays an important role in the problem of characterizing the molecular structure [30]. In [15], the study was extended to distance matrices, and the distance Estrada index of was defined by , where is the eigenvalue set of .
In this paper, we consider a more general Estrada index. Let
[TABLE]
be the -distance Estrada index of , where is the eigenvalue set of . Clearly, . Next, we establish some bounds on the -distance Estrada index.
Lemma 3.26**.**
[25]* Let be nonnegative real numbers. Then for ,*
[TABLE]
Theorem 3.27**.**
Let be a graph with vertices. Then
[TABLE]
where .
Proof.
Let be the eigenvalues of . From Lemmas 2.12 and 3.13, we have
[TABLE]
[TABLE]
where . ∎
Theorem 3.28**.**
Let be a graph with vertices. Then
[TABLE]
Proof.
Let be the eigenvalues of . Then
[TABLE]
From Arithmetic-Geometric inequality, we obtain
[TABLE]
By Taylor expansion theorem, we have
[TABLE]
Let . Then
[TABLE]
Hence,
[TABLE]
It is elementary to show for , let the function
[TABLE]
where , then is monotonically decreasing in the interval . Hence, is a largest lower bound of . ∎
Theorem 3.29**.**
Let be a graph with vertices. Then
[TABLE]
Proof.
Let , where Obviously, is a decreasing function when , and is increasing when . Then , that is
[TABLE]
and the equality holds if and only if . So by this function, we have
[TABLE]
where are the eigenvalues of .
Let , where . Clearly, is an increasing function when . From Lemma LABEL:lem1, we have
[TABLE]
then,
[TABLE]
Hence,
[TABLE]
∎
From Theorem 2.1, we have the following result.
Corollary 3.30**.**
Let be a transmission regular graph with vertices. Let for each . Then
[TABLE]
Next, a new upper bound for the -distance Estrada index is established.
Theorem 3.31**.**
Let be a graph with vertices. Then
[TABLE]
Proof.
By the definition of -distance energy, we have
[TABLE]
∎
4 Acknowledgments
Supported by by the National Natural Science Foundation of China (No. 11801115 and No.11601102), the Natural Science Foundation of the Heilongjiang Province (No.QC2018002) and the Fundamental Research Funds for the Central Universities.
References
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