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; zhangxling04@yahoo.cn Received 25 November 2012; Revised 29 May 2013; Accepted 30 May 2013 Academic Editor: Maurizio Porfiri Copyright © 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·), π0 (π·), π− (π·)), where π+ (π·), π0 (π·), and π− (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. Let πΊ be a simple connected graph with vertex set π(πΊ) and edge set πΈ(πΊ). The distance between two vertices π’, V ∈ π(πΊ) is denoted by ππ’V and is defined as the length of the shortest path between π’ and V in πΊ. The distance matrix of πΊ is denoted by π·(πΊ) and is defined by π·(πΊ) = (ππ’V )π’,V∈π(πΊ) . Since π·(πΊ) is a symmetric matrix, its inertia is the triple of integers (π+ (π·(πΊ)), π0 (π·(πΊ)), π− (π·(πΊ))), where π+ (π·(πΊ)), π0 (π·(πΊ)), and π− (π·(πΊ)) denote the number of positive, 0, and negative eigenvalues of π·(πΊ), respectively. The distance matrix 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 computation 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 information 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 complicated 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], πΎπ , 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. The wheel graph of π vertices ππ is a graph that contains a cycle of length π−1 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 distance matrices 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©Ύ π π and π΅ one of its principal submatrices. Let π΅ have eigenvalues π1 β©Ύ ⋅ ⋅ ⋅ β©Ύ ππ . Then the inequalities π π−π+π β©½ ππ β©½ π π (π = 1, . . . , π) hold. Comparing πΆπ to π·π , we get the following: For a square matrix, let cof (π΄) denote the sum of Μ by subtracting the first cofactors of π΄. Form the matrix π΄ row from all other rows then the first column from all other Μ11 denote the principle submatrix obtained columns and let π΄ Μ from π΄ by deleting the first row and first column. Expanding the determinant π·π according to the last column and then the last line, we get the following incursion: Μ11 . Lemma 2 (see [15]). πππ(π΄) = det π΄ 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. that is, Lemma 3 (see [15]). If πΊ is a strongly connected directed graph with blocks πΊ1 , πΊ2 , . . . , πΊπ , then πΆπ = π·π + (1) det π· (πΊ) = ∑ det π· (πΊπ ) ∏πππ π· (πΊπ ) . π=1 Then 1 −2 −1 0 .. . 0 0 1 −1 −2 −1 .. . 0 0 1 0 −1 −2 .. . ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ 1 0 0 0 . d .. 0 ⋅ ⋅ ⋅ −2 0 ⋅ ⋅ ⋅ −1 1 0] ] 0] ] 0] ] . .. ] . ] ] −1] −2]π×π π ππ π ππ πVππ, − , { { { 2 det πΆ = { { { π + 1 , ππ π ππ πππ. { 2 (6) π·π + π·π−1 = − (π·π−1 + π·π−2 ) + 1. (7) if π is even, (8) if π is odd. So, we have the following: π =ΜΈ π Lemma 4. Let 1 [−1 [ [0 [ [ πΆ=[0 [ .. [ . [ [0 [0 π·π = −2π·π−1 − π·π−2 + 1; 0, { { π·π = { {1 , {2 π π (5) Since π·1 = 1/2, π·2 = 0, and π·3 = 1/2, from the above incursion, we get the following: πππ π· (πΊ) = ∏πππ π· (πΊπ ) , π=1 π × (−1)π−1 . 2 π − , { { { 2 πΆπ = { { {π + 1, { 2 (2) if π is even, (9) if π is odd. This completes the proof. 3. Main Results (3) Proof. Let In the following, we always assume that π(ππ ) = {V0 , V1 , . . . , Vπ−1 }, where V0 is the hub of ππ . Theorem 5. Let π = Vπ Vπ+1 mod (π−1) (1 β©½ π β©½ π − 1). Then 2 σ΅¨σ΅¨ 1 σ΅¨σ΅¨ σ΅¨σ΅¨−1 σ΅¨σ΅¨ σ΅¨σ΅¨ 0 σ΅¨σ΅¨ σ΅¨σ΅¨ πΆπ = σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨ .. σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨σ΅¨ 0 σ΅¨σ΅¨ σ΅¨σ΅¨ 0 σ΅¨ 1 −2 −1 0 .. . 0 0 1 −1 −2 −1 .. . 0 0 1 0 −1 −2 .. . ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ 1 0 0 0 . d .. 0 ⋅ ⋅ ⋅ −2 0 ⋅ ⋅ ⋅ −1 σ΅¨σ΅¨ 1 σ΅¨σ΅¨ −1 0 0 ⋅ ⋅ ⋅ σ΅¨σ΅¨ 2 σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −2 −1 0 ⋅ ⋅ ⋅ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −1 −2 −1 ⋅ ⋅ ⋅ σ΅¨ π·π = σ΅¨σ΅¨σ΅¨ 1 0 −1 −2 ⋅ ⋅ ⋅ σ΅¨σ΅¨ σ΅¨σ΅¨ . . . . σ΅¨σ΅¨ . . . . σ΅¨σ΅¨ . . . . d σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ 1 0 0 0 ⋅ ⋅ ⋅ σ΅¨σ΅¨ 1 0 0 0 ⋅ ⋅ ⋅ σ΅¨ 0 0 0 0 .. . −2 −1 π { { ππ π ππ πVππ, { {− 4 , det π· (ππ − π) = { { π2 − 1 { { , ππ π ππ πππ, { 4 1 σ΅¨σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ , .. σ΅¨σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨ −1σ΅¨σ΅¨σ΅¨σ΅¨ −2σ΅¨σ΅¨σ΅¨π×π σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨ . σ΅¨ .. σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨σ΅¨ σ΅¨ −1σ΅¨σ΅¨σ΅¨ σ΅¨ −2σ΅¨σ΅¨σ΅¨π×π (10) where π β©Ύ 3. (4) Proof. Without loss of generality, we may assume that π = V1 Vπ−1 . Let σ΅¨σ΅¨0 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨ π΄ π = det π· (ππ − π) = σ΅¨σ΅¨σ΅¨1 σ΅¨σ΅¨ .. σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨ 1 0 1 2 .. . 1 1 0 1 .. . 1 2 1 0 .. . ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ 1 2 2 2 . d .. 2 2 2 ⋅⋅⋅ 0 2 2 2 ⋅⋅⋅ 1 1σ΅¨σ΅¨σ΅¨ σ΅¨ 2σ΅¨σ΅¨σ΅¨σ΅¨ 2σ΅¨σ΅¨σ΅¨σ΅¨ 2σ΅¨σ΅¨σ΅¨σ΅¨ . .. σ΅¨σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨ 1σ΅¨σ΅¨σ΅¨σ΅¨ 0σ΅¨σ΅¨σ΅¨π×π (11) Journal of Applied Mathematics 3 Then Proof. Consider the following σ΅¨σ΅¨ 1 σ΅¨σ΅¨ 0 1 1− 1 ⋅⋅⋅ σ΅¨σ΅¨ 2 σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −2 0 0 ⋅⋅⋅ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 1 σ΅¨1 − 0 −2 + −1 ⋅ ⋅ ⋅ π΄ π = σ΅¨σ΅¨σ΅¨σ΅¨ 2 2 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 −1 −2 ⋅ ⋅ ⋅ σ΅¨σ΅¨ .. .. .. σ΅¨σ΅¨ .. σ΅¨σ΅¨ . . . . d σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 0 0 ⋅⋅⋅ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 0 0 ⋅⋅⋅ σ΅¨ 1 0 0 0 .. . −2 −1 σ΅¨σ΅¨ 1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ . σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ .. σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨σ΅¨ σ΅¨ −1σ΅¨σ΅¨σ΅¨ σ΅¨ −2σ΅¨σ΅¨σ΅¨π×π (12) Expanding the determinant π΄ π according to the second line, we get the following incursion: π΄ π = (−1) π−1 π 2 − 2π΄ π−1 − πΆπ−2 − π·π−2 − π΄ π−2 , (13) where πΆπ and π·π are defined as in Lemma 4. By Lemma 4, we get the following: π΄π = { −1 − 2π΄ π−1 − π΄ π−2 , if π is even, −2π΄ π−1 − π΄ π−2 , if π is odd. (14) Since π΄ 3 = 2, π΄ 4 = −4, π΄ 5 = 6, and π΄ 6 = −9, according to the above incursion, we get the following: 2 π { { if π is even, { {− 4 , π΄π = { 2 { { { π − 1 , if π is odd, { 4 (15) where π β©Ύ 3. This completes the proof. Corollary 6. Let π = Vπ Vπ+1 mod π+ (π· (ππ − π)) = 1, (π−1) σ΅¨σ΅¨0 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨ = σ΅¨σ΅¨σ΅¨1 σ΅¨σ΅¨ .. σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨ 1 0 1 2 .. . 1 2 2 2 . d .. 2 2 2 ⋅⋅⋅ 0 1 2 2 ⋅⋅⋅ 1 1 −2 −1 0 .. . 1 1 0 1 .. . 1 2 1 0 .. . ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ 1 −1 −2 −1 .. . 1 0 −1 −2 .. . 0 0 −1 0 1σ΅¨σ΅¨σ΅¨ σ΅¨ 1σ΅¨σ΅¨σ΅¨σ΅¨ 2σ΅¨σ΅¨σ΅¨σ΅¨ 2σ΅¨σ΅¨σ΅¨σ΅¨ .. σ΅¨σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨ 1σ΅¨σ΅¨σ΅¨σ΅¨ 0σ΅¨σ΅¨σ΅¨π×π 1 1 σ΅¨σ΅¨σ΅¨ σ΅¨ 0 −1σ΅¨σ΅¨σ΅¨σ΅¨ 0 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 0 σ΅¨σ΅¨σ΅¨σ΅¨ . . σ΅¨σ΅¨σ΅¨ d .. .. σ΅¨σ΅¨σ΅¨ σ΅¨ 0 ⋅ ⋅ ⋅ −2 −1σ΅¨σ΅¨σ΅¨σ΅¨ 0 ⋅ ⋅ ⋅ −1 −2σ΅¨σ΅¨σ΅¨π×π ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ σ΅¨σ΅¨ 0 π−1 σ΅¨σ΅¨ σ΅¨σ΅¨π − 1 −4 (π − 1) σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −4 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −4 σ΅¨ = σ΅¨σ΅¨ σ΅¨σ΅¨ .. .. σ΅¨σ΅¨ . . σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −4 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 −4 σ΅¨ σ΅¨σ΅¨ 0 π−1 σ΅¨σ΅¨ σ΅¨σ΅¨π − 1 4 (π − 1) σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 σ΅¨ = σ΅¨σ΅¨ σ΅¨σ΅¨ .. .. σ΅¨σ΅¨ . . σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 0 σ΅¨ 1 −4 −2 −1 .. . 0 0 1 0 −2 −1 .. . 0 0 1 −4 −1 −2 .. . π0 (π· (ππ − π)) = 0, 1 −4 0 0 . d .. 0 ⋅ ⋅ ⋅ −2 0 ⋅ ⋅ ⋅ −1 1 0 −1 −2 .. . ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ 1 0 0 0 . d .. 0 ⋅ ⋅ ⋅ −2 0 ⋅ ⋅ ⋅ −1 1 σ΅¨σ΅¨σ΅¨ σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ . .. σ΅¨σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨ −1σ΅¨σ΅¨σ΅¨σ΅¨ −2σ΅¨σ΅¨σ΅¨π×π (18) Expanding the above determinant according to the second line, we get the following: (16) Proof. We will prove the result by induction on π. If π = 3, π3 − π ≅ π3 is obviously true. Suppose that the result is true for π−1; that is, π+ (π·(ππ−1 − π)) = 1, π0 (π·(ππ−1 − π)) = 0, π− (π·(ππ−1 − π)) = π − 2. Since π·(ππ−1 − π) is a principle submatrix of π·(ππ − π), by Lemma 1, the eigenvalues of π·(ππ−1 − π) interlace the eigenvalues of π·(ππ − π). By Theorem 5, det π·(ππ−1 − π) det π·(ππ − π) < 0. So, π·(ππ − π) has one negative eigenvalue more than π·(ππ−1 −π). According to the induction hypothesis, we get π+ (π·(ππ − π)) = 1, π0 (π·(ππ − π)) = 0, and π− (π·(ππ − π)) = π − 1. This completes the proof. Theorem 7. One has 1 − π, ππ π ππ πVππ, det π· (ππ ) = { 0, ππ π ππ πππ, 1 σ΅¨σ΅¨σ΅¨ σ΅¨ −4σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ 0 σ΅¨σ΅¨σ΅¨σ΅¨ .. σ΅¨σ΅¨σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨ −1σ΅¨σ΅¨σ΅¨σ΅¨ −2σ΅¨σ΅¨σ΅¨π×π ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ ⋅⋅⋅ (1 β©½ π β©½ π − 1). Then π− (π· (ππ − π)) = π − 1. where π β©Ύ 3. σ΅¨σ΅¨0 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨ det π· (ππ ) = σ΅¨σ΅¨σ΅¨1 σ΅¨σ΅¨ .. σ΅¨σ΅¨ . σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨σ΅¨ σ΅¨σ΅¨1 σ΅¨ (17) det π· (ππ ) = (−1)π−1 (π − 1)3 + 4 (π − 1) π΄ π−1 , (19) where π΄ π is defined as in Theorem 5. By Theorem 5, when π β©Ύ 3, we get the following: 1 − π, if π is even, det π· (ππ ) = { 0, if π is odd. (20) This completes the proof. Similar to Corollary 6, we can get the following corollary. Corollary 8. (i) If π is even, π+ (π·(ππ )) = 1, π0 (π·(ππ )) = 0, π− (π·(ππ )) = π − 1. (ii) If π is odd, π+ (π·(ππ )) = 1, π0 (π·(ππ )) = 1, π− (π·(ππ )) = π − 2. Denote by ππ − V0 the graph obtained from ππ by deleting the vertex V0 and all the edges adjacent to V0 ; that is, ππ − V0 ≅ πΆπ−1 . Let πΈπ (1 β©½ π β©½ π) be any subset of πΈ(ππ − V0 ) with |πΈπ | = π. In the following, we always denote by ππ − πΈπ the graph obtained from ππ by deleting all the edges in πΈπ . 4 Journal of Applied Mathematics Theorem 9. One has π+ (π·(ππ − πΈπ )) = 1, π0 (π·(ππ − πΈπ )) = 0, π− (π·(ππ − πΈπ )) = π − 1. Proof. Denote the components of ππ − πΈπ − V0 by πΆ1 , . . . , πΆπ . Let πΊπ denote the graph that contains πΆπ plus the vertex V0 such that V0 is connected to every other vertex, 1 β©½ π β©½ π . Then each πΊπ (1 β©½ π β©½ π ) is isomorphism to π|π(πΊπ )| − ππ or πΎ2 , where ππ is an edge of π|π(πΊπ )| − V0 . By Lemma 2 and some direct calculations, we get the following: Μ σ΅¨ σ΅¨ cof (πΊπ ) = det π·(π|π(πΊπ )| − ππ )11 = (−1)|π(πΊπ )|−1 σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨ . (21) It is easy to check that cof (πΊπ ) = (−1)|π(πΊπ )|−1 |π(πΊπ )| is also true when πΊπ is isomorphism to πΎ2 . In the following, we will prove the theorem by introduction on π . For π = 1, πΊ ≅ ππ − π, where π is an edge of ππ − V0 , by Corollary 6, we get the result. Suppose the result is true for π − 1. For π , let πΊσΈ = πΊ1 ∪ πΊ2 ∪ ⋅ ⋅ ⋅ ∪ πΊπ −1 . Then by the induction hypothesis, π+ (π·(πΊσΈ )) = 1, π0 (π·(πΊσΈ )) = 0, and π− (π·(πΊσΈ )) = |π(πΊσΈ )| − 1, which implies that σΈ det π· (πΊσΈ ) = (−1)|π(πΊ )|−1 π, (22) where π is a positive integer. Since σ΅¨ σ΅¨ cof (πΊπ ) = (−1)|π(πΊπ )|−1 σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨ , 1 β©½ π β©½ π , (23) by Lemma 3, π −1 π −1 σΈ σ΅¨ σ΅¨ cof π· (πΊσΈ ) = ∏cofπ· (πΊπ ) = (−1)|π(πΊ )|−1 ∏ σ΅¨σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨σ΅¨ . π=1 π=1 (24) Then Lemma 10 (see [13]). Let πΊ × π» denote the Cartesian product of connected graphs πΊ and π», where π(πΊ) = {π’1 , . . . , π’π } and π(π») = {V1 , . . . , Vπ }. Then we have (i) π+ (πΊ × π») = π+ (πΊπ’π ⋅ Vπ π»); (ii) π0 (πΊ × π») = (π − 1)(π − 1) + π0 (πΊπ’π ⋅ Vπ π»); (iii) π− (πΊ × π») = π− (πΊπ’π ⋅ Vπ π»). Theorem 11. Let π’0 and V0 be the hubs of ππ and ππ , respectively. Suppose πΈπ (0 β©½ π β©½ π−1) and πΈπ (0 β©½ π β©½ π−1) are any subsets of πΈ(ππ − π’0 ) and πΈ(ππ − V0 ) with |πΈπ | = π, |πΈπ | = π, respectively. Then, the distance matrix of the graph (ππ − πΈπ ) × (ππ − πΈπ ) has exactly one positive eigenvalue. Proof. Since π’0 and V0 are the hubs of ππ and ππ , respectively, (ππ −πΈπ )π’0 ⋅V0 (ππ −πΈπ ) must be isomorphism to some ππ+π−1 − πΈπ+π , where π€0 is the hub of ππ+π−1 and πΈπ+π is any subset of πΈ(ππ+π−1 − π€0 ) with |πΈπ+π | = π + π. By Theorem 9 and Lemma 10, we get the result. Given an arbitrary integer π, for 1 β©½ π β©½ π, let Vπ0 be the hub of πππ and πΈππ any subset of πΈ(πππ − Vπ0 ). Suppose π(πππ ) = {Vπ0 , Vπ1 , . . . , Vπ(ππ −1) }. Theorem 12. For an arbitrary integer π, the distance matrix of the graph πΊ = (ππ1 − πΈπ1 )V1π ⋅ V2π (ππ2 − πΈπ2 )V2β ⋅ ⋅ ⋅ V(π−1)π (πππ−1 − πΈππ−1 )V(π−1)π‘ ⋅ Vππ (πππ − πΈππ ) has exactly one positive eigenvalue. Proof. We will prove the conclusion by induction on π. If π = 1, by Theorem 9, the conclusion is true. Suppose the conclusion is true for π−1. For convenience, let π» = (ππ1 − πΈπ1 )V1π ⋅ V2π (ππ2 − πΈπ2 )V2β ⋅ ⋅ ⋅ V(π−2)π (πππ−2 − πΈππ−2 ). Then πΊ = π»V(π−2)π ⋅ V(π−1)π (πππ−1 − πΈππ−1 )V(π−1)π‘ ⋅ Vππ (πππ − πΈππ ). By Lemma 10, we have the following: π+ (πΊ) = π+ (π» (πππ−1 − πΈππ−1 ) V(π−1)π‘ ⋅ Vππ (πππ − πΈππ )) det π· (ππ − πΈπ ) = π+ (π» (πππ−1 − πΈππ−1 ) V(π−1)0 ⋅ Vπ0 (πππ − πΈππ )) . (26) = det π· (πΊσΈ ) cof π· (πΊπ ) + det π· (πΊπ ) cof π· (πΊσΈ ) σ΅¨ σ΅¨ = (−1)|π(πΊ )|−1 π × (−1)|π(πΊπ )|−1 σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨ σΈ π −1 σΈ σ΅¨ σ΅¨ + (−1)|π(πΊπ )|−1 π × (−1)|π(πΊ )|−1 ∏ σ΅¨σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨σ΅¨ (25) π=1 π −1 σ΅¨ σ΅¨ σ΅¨ σ΅¨ = (−1)π−1 (π σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨ + π∏ σ΅¨σ΅¨σ΅¨σ΅¨π (πΊπ )σ΅¨σ΅¨σ΅¨σ΅¨) , π=1 where π = π2 /4, if π is even and π = (π2 − 1)/4, if π is odd. In this case, similar to Corollary 6, we can easily get π+ (π·(ππ − πΈπ )) = 1, π0 (π·(ππ − πΈπ )) = 0, and π− (π·(ππ − πΈπ )) = π − 1. Up to now, we have proved the result. Let πΊπ’π ⋅Vπ π» denote the graph formed by only identifying the vertex π’π of πΊ with the vertex Vπ of π», where π’π and Vπ are arbitrary vertices of πΊ and π», respectively. Since (πππ−1 − πΈππ−1 )V(π−1)0 ⋅ Vπ0 (πππ − πΈππ ) = πππ−1 +ππ −1 − πΈππ−1 −πΈππ , we get π+ (πΊ) = π+ (π»V(π−2)π ⋅V(π−1)π (πππ−1 +ππ −1 − πΈππ−1 − πΈππ )). By the induction hypothesis, we get π+ (πΊ) = 1. This completes the proof. Remark 13. Let πΊ1 and πΊ2 be any two graphs with the same form as πΊ in Theorem 12. Making Cartesian product of graphs πΊ1 and πΊ2 , by Lemma 10 and Theorem 12, we get a series of graphs whose distance matrices have exactly one positive eigenvalue. Acknowledgments The authors would like to thank the anonymous referees for their valuable comments and suggestions. This work was supported by NSFC (11126256) and NSF of Shandong Province of China (ZR2012AQ022). Journal of Applied Mathematics References [1] D. H. 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