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Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 707954, 5 pages http://dx.doi.org/10.1155/2013/707954

Research Article The Distance Matrices of Some Graphs Related to Wheel Graphs

Xiaoling Zhang and Chengyuan Song

School of Mathematics and Information Science, Yantai University, Yantai, Shandong 264005, China

Correspondence should be addressed to Xiaoling Zhang; [email protected]

Received 25 November 2012; Revised 29 May 2013; Accepted 30 May 2013

Academic Editor: Maurizio Porfiri

Copyright Β© 2013 X. Zhang and C. Song. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Let π· denote the distance matrix of a connected graph πΊ. The inertia of π· is the triple of integers (π + (π·), π

0 (π·), π

β (π·)), where

π + (π·), π

0 (π·), and π

β (π·) denote the number of positive, 0, and negative eigenvalues of π·, respectively. In this paper, we mainly

study the inertia of distance matrices of some graphs related to wheel graphs and give a construction for graphs whose distance matrices have exactly one positive eigenvalue.

1. Introduction

A simple graph πΊ = (π, πΈ) consists of π, a nonempty set of vertices, and πΈ, a set of unordered pairs of distinct elements of π called edges. All graphs considered here are simple and connected. LetπΊ be a simple connected graph with vertex set π(πΊ) and edge set πΈ(πΊ).The distance between two vertices π’, V β π(πΊ) is denoted by π

π’V and is defined as the length of the shortest path between π’ and V inπΊ.The distancematrix ofπΊ is denoted byπ·(πΊ) and is defined byπ·(πΊ) = (π

π’V)π’,Vβπ(πΊ). Since π·(πΊ) is a symmetric matrix, its inertia is the triple of integers (π + (π·(πΊ)), π

0 (π·(πΊ)), π

β (π·(πΊ))), where π

+ (π·(πΊ)), π

0 (π·(πΊ)),

and π β (π·(πΊ)) denote the number of positive, 0, and negative

eigenvalues ofπ·(πΊ), respectively. The distancematrix of a graph has numerous applications

to chemistry [1]. It contains information on various walks and self-avoiding walks of chemical graphs. Moreover, the distance matrix is not only immensely useful in the compu- tation of topological indices such as the Wiener index [1] but also useful in the computation of thermodynamic properties such as pressure and temperature virial coefficients [2]. The distance matrix of a graph contains more structural informa- tion compared to a simple adjacency matrix. Consequently, it seems to be a more powerful structure discriminator than the adjacency matrix. In some cases, it can differentiate isospectral graphs although there are nonisomorphic trees with the same distance polynomials [3]. In addition to such applications in chemical sciences, distance matrices

find applications in music theory, ornithology [4], molecular biology [5], psychology [4], archeology [6], sociology [7], and so forth. For more information, we can see [1] which is an excellent recent review on the topic and various uses of distance matrices.

Since the distance matrix of a general graph is a compli- cated matrix, it is very difficult to compute its eigenvalues. People focus on studying the inertia of the distance matrices of some graphs. Unfortunately, up to now, only few graphs are known to have exactly one positive π·-eigenvalue, such as trees [8], connected unicyclic graphs [9], the polyacenes, honeycomb and square lattices [10], complete bipartite graphs [11], πΎ

π , and iterated line graphs of some regular graphs [12],

and cacti [13]. This inspires us to find more graphs whose distance matrices have exactly one positive eigenvalue.

Thewheel graph of π verticesπ π is a graph that contains a

cycle of length πβ1 plus a vertex V (sometimes called the hub) not in the cycle such that V is connected to every other vertex. In this paper, we first study the inertia of the distancematrices in wheel graphs if one or more edges are removed from the graph, and then, with the help of the structural characteristics of wheel graphs, we give a construction for graphs whose distance matrices have exactly one positive eigenvalue.

2. Preliminaries

We first give some lemmas that will be used in the main results.

2 Journal of Applied Mathematics

Lemma 1 (see [14]). Let π΄ be a Hermitian matrix with eigenvalues π

1 β©Ύ β β β β©Ύ π

π and π΅ one of its principal

submatrices. Let π΅ have eigenvalues π 1 β©Ύ β β β β©Ύ π

π . Then the

inequalities π πβπ+π

β©½ π π β©½ π π (π = 1, . . . , π) hold.

For a square matrix, let cof (π΄) denote the sum of cofactors of π΄. Form the matrix π΄ by subtracting the first row from all other rows then the first column from all other columns and letπ΄

11 denote the principle submatrix obtained

from π΄ by deleting the first row and first column.

Lemma 2 (see [15]). πππ(π΄) = detπ΄ 11 .

A cut vertex is a vertex the removal of which would disconnect the remaining graph; a block of a graph is defined to be a maximal subgraph having no cut vertices.

Lemma3 (see [15]). If πΊ is a strongly connected directed graph with blocks πΊ

1 , πΊ 2 , . . . , πΊ

π , then

ππππ· (πΊ) =

π

β

π=1

ππππ· (πΊ π ) ,

detπ· (πΊ) = π

β

π=1

det π·(πΊ π )β

π ΜΈ= π

ππππ· (πΊ π ) .

(1)

Lemma 4. Let

πΆ =

[ [ [ [ [ [ [ [ [ [

[

1 1 1 1 β β β 1 1

β1 β2 β1 0 β β β 0 0

0 β1 β2 β1 β β β 0 0

0 0 β1 β2 β β β 0 0

... ...

... ... d

... ...

0 0 0 0 β β β β2 β1

0 0 0 0 β β β β1 β2

] ] ] ] ] ] ] ] ] ]

]πΓπ

. (2)

Then

det πΆ = {{{

{{{

{

β π

2 , ππ π ππ πVππ,

π + 1

2 , ππ π ππ πππ.

(3)

Proof. Let

πΆ π =

σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨

1 1 1 1 β β β 1 1

β1 β2 β1 0 β β β 0 0

0 β1 β2 β1 β β β 0 0

0 0 β1 β2 β β β 0 0

... ...

... ... d

... ...

0 0 0 0 β β β β2 β1

0 0 0 0 β β β β1 β2

σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨ πΓπ

,

π· π =

σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨

1

2 β1 0 0 β β β 0 0

1 β2 β1 0 β β β 0 0

1 β1 β2 β1 β β β 0 0

1 0 β1 β2 β β β 0 0

... ...

... ... d

... ...

1 0 0 0 β β β β2 β1

1 0 0 0 β β β β1 β2

σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨πΓπ

.

(4)

Comparing πΆ π toπ· π , we get the following:

πΆ π = π· π + π

2 Γ (β1)

πβ1

. (5)

Expanding the determinant π· π according to the last column

and then the last line, we get the following incursion:

π· π = β2π·

πβ1 β π· πβ2

+ 1; (6)

that is,

π· π + π· πβ1

= β (π· πβ1

+ π· πβ2 ) + 1. (7)

Since π· 1 = 1/2, π·

2 = 0, and π·

3 = 1/2, from the above

incursion, we get the following:

π· π =

{{

{{

{

0, if π is even,

1

2 , if π is odd.

(8)

So, we have the following:

πΆ π =

{{{

{{{

{

β π

2 , if π is even,

π + 1

2 , if π is odd.

(9)

This completes the proof.

3. Main Results

In the following, we always assume that π(π π ) = {V

0 , V 1 , . . . ,

V πβ1 }, where V

0 is the hub ofπ

π .

Theorem 5. Let π = V π V π+1 mod (πβ1) (1 β©½ π β©½ π β 1). Then

det π·(π π β π) =

{{{{

{{{{

{

β π 2

4 , ππ π ππ πVππ,

π 2 β 1

4 , ππ π ππ πππ,

(10)

where π β©Ύ 3.

Proof. Without loss of generality, we may assume that π = V 1 V πβ1

. Let

π΄ π = detπ·(π

π β π) =

σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨σ΅¨

0 1 1 1 β β β 1 1

1 0 1 2 β β β 2 2

1 1 0 1 β β β 2 2

1 2 1 0 β β β 2 2

... ...

... ... d

... ...

1 2 2 2 β β β 0