542
Views
0
CrossRef citations to date
0
Altmetric
Articles

On the distance spectra of m-generation n-prism graph

, &
Pages 276-281 | Received 19 Oct 2021, Accepted 06 Oct 2022, Published online: 27 Oct 2022

Abstract

The distance matrix of a simple connected graph G is D(G)=(dij), where dij is the length of a shortest path between the ith and jth vertices of G. Eigenvalues of D(G) are called the distance eigenvalues of G. The m-generation n-prism graph or (m, n)-prism graph can be defined in an iterative way where (1,n)-prism graph is an n-vertex cycle. In this paper, we first find the number of zero eigenvalues of the distance matrix of a (m, n)-prism graph. Next, we find some quotient matrix that contains m nonzero distance eigenvalues of a (m, n)-prism graph. Our next result gives the rest of the nonzero distance eigenvalues of a (m, n)-prism graph in terms of distance eigenvalues of a cycle. Finally, we find the characteristic polynomial of the distance matrix of a (m, n)-prism graph. Applying this result, we provide the explicit distance eigenvalues of a (3,n)-prism graph.

2000 Mathematics Subject Classification::

1. Introduction

Consider an n-vertex undirected, connected and simple graph G=(V,E), where V={1,2,3,,n} is the vertex set and E is the edge set. The distance matrix of G, is denoted by D(G), is an n × n matrix (dij), where dij is the distance between the ith and jth vertices in G. The matrix D(G) is symmetric, non-negative and irreducible. A cycle graph of n vertices is denoted by Cn, and a path graph of n vertices is denoted by Pn. The m-generation n-prism graph or (m, n)-prism graph can be defined in an iterative way. Let (1,n)-prism graph be an n-vertex cycle. Then, (m, n)-prism graph can be obtained from (m1,n)-prism graph as follows: Every outermost vertex in (m1,n)-prism graph gives birth to a new vertex, and all the n new vertex form a new cycle, then connect each new vertex with its corresponding mother vertex by an edge. We denote the (m, n)-prism graph by Umn. For construction of Umn, reader may see . Clearly, the number of vertices of Umn is mn. By Jn, we denote the n × n matrix with all entries one and by jn we denote the n×1 column vector with all entries one. The Kronecker product of two matrices A=(aij) of size m × n and B of size p×q, denoted by AB, is defined to be the mp × nq partition matrix (aijB). For matrices M, N, P and Q of suitable sizes, MNPQ=(MP)(NQ). Suppose a real symmetric matrix A can be partitioned as (A11A12A1mAm1Am2Amm), where each Aij is a block of A. The matrix Q=(qij) of order m × m is called a quotient matrix of A, where qij is the average row sum of the block Aij. If the row sum of each block Aij is a constant, then the partition is called equitable.

Figure 1. Construction of Umn.

Figure 1. Construction of Umn.

The distance matrix of a graph was introduced in [Citation1] to the study of problem involves finding appropriate addresses so that a message can efficiently transfer through a series of loops from its origin to its destination. Balaban et al. [Citation2] proposed the use of distance spectral radius, which is the largest eigenvalue of the distance matrix, as a molecular descriptor, while Gutman and Medeleanu [Citation3] successfully used it to infer the extent of branching and model boiling points of alkanes. The distance spectral radius is a useful molecular descriptor in QSPR modeling as demonstrated by Consonni and Todeschini [Citation4,Citation5]. In [Citation6], Graham and Lovász discussed the characteristic polynomial of distance matrix of a tree. Ruzieh and Powers [Citation7] found all the eigenvalues and eigenvectors of the distance matrix of the path Pn. In [Citation8], Fowler et al. found all the distance eigenvalues of the cycle Cn. Lin et al. [Citation9] characterized connected graphs whose distance eigenvalues satisfies some properties. In [Citation10], Atik and Panigrahi found the distance spectrum of some distance regular graphs, including the well-known Johnson graphs. In [Citation11], authors found the bounds of the distance and distance signless Laplacian eigenvalues for any general graph. Aalipour et al. [Citation12] determined the distance spectra of some graphs, including distance regular graphs, double odd graphs, Doob graphs and characterized strongly regular graphs as having more positive than negative distance eigenvalues. Alazemi et al. [Citation13] characterized some distance-regular graphs in terms of number of distinct distance eigenvalues. In [Citation14], Lu and Huang obtained the distance spectrum of B(n, k) which is a subgraph of the Boolean lattice. Pirzada et al. [Citation15] worked on spectral spread of generalized distance matrix of a graph. A few more recent works related to spectra of distance matrix researchers may follow [Citation16–18]. For extensive research, work on distance spectra can be found in the survey [Citation19] and in the most recent survey [Citation20]. In this paper, we first find the lower bound of the number of zero eigenvalues of the distance matrix of m-generation n-prism graph Umn and later we prove that this bound is exact. Next, we find some quotient matrix of D(Umn) corresponding to an equitable partition. We prove that this quotient matrix will contain m nonzero eigenvalues D(Umn). Our next result gives the rest of the nonzero eigenvalues of D(Umn). Applying these results, we find the characteristic polynomial of distance matrix of Umn. As an immediate application of these results, we provide the explicit distance eigenvalues of U3n.

Next, we state some of the earlier useful results. The following is a well-known result on equitable partition of matrices.

Theorem 1.1.

[Citation21] Let Q be a quotient matrix of a square matrix A corresponding to an equitable partition. Then the spectrum of A contains the spectrum of Q.

Explicit eigenvalues of Pn and Cn can be found from the following results.

Theorem 1.2.

[Citation7] The distance eigenvalues λi, i=1,2,,n, of the path Pn with n > 2 are as follows:

  1. 1. λ1=1/(coshθ1), where θ is the positive solution of tanh(θ/2)tanh(nθ/2)=1/n.

  2. λi=1/(cosθ1), where (a) θ is the one of the [(n1)/2] solutions of tanh(θ/2)tanh(nθ/2)=1/n in the interval (0,π), or (b) θ=(2m1)π/n for m=1,2,,[n/2].

Theorem 1.3.

[Citation8] The characteristic polynomial of D(Cn), the distance matrix of an n-vertex cycle Cn, is given by p(t)=tp1(tn24)j=1p(t+csc2(π(2j1)n)),  if n=2p.p(t)=(tn214)j=1p(t+14sec2(πjn))j=1p(t+14csc2(π(2j1)2n)), if n=2p+1.

Theorem 1.4.

[Citation22] Let T be a weighted tree on n vertices with edge weights α1,α2,,αn1. Let D be the distance matrix of T. Then, for any real number x, det(D+xJ)=(1)n12n2(i=1n1αi)(2x+i=1n1αi)

Theorem 1.5.

[Citation23] Suppose that A and B are square matrices of order n and m, respectively. Let λ1,λ2,,λn be the eigenvalues of A and μ1,μ2,,μm be the eigenvalues of B. Then, the eigenvalues of AB are λiμj;  i=1,2,,n;  j=1,2,,m.

Theorem 1.6.

[Citation24] If A,BMm,n(F), then Rank(A+B)Rank(A)+Rank(B)

Equality holds if and only if range(A)range(B)={0} and range(AT)range(BT)={0}.

2. Full D-spectrum of some graphs

We first discuss the number of zero eigenvalues of D(Umn).

Theorem 2.1.

The distance matrix of Umn is having zero as an eigenvalue with multiplicity at least mnmn+1 and mnmn2 according as n is odd and even, respectively.

Proof.

By a suitable ordering of vertices (as shown in ) we get the distance matrix of Umn as (1) D(Umn)=[D(Cn)D(Cn)+JnD(Cn)+2JnD(Cn)+(m1)JnD(Cn)+JnD(Cn)D(Cn)+JnD(Cn)+(m2)JnD(Cn)+2JnD(Cn)+JnD(Cn)D(Cn)+(m3)JnD(Cn)+(m1)JnD(Cn)+(m2)JnD(Cn)+(m3)JnD(Cn)](1) (2) =[D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)D(Cn)]+[0Jn2Jn(m1)JnJn0Jn(m2)Jn2JnJn0(m3)Jn(m1)Jn(m2)Jn(m3)Jn0]=JmD(Cn)+D(Pm)Jn.(2)

Figure 2. U35.

Figure 2. U35.

We have from Theorem 1.3, the number of zero eigenvalues of D(Cn) is 0 and n21 according as n is odd and even, respectively. Also, for a symmetric matrix, the number of zero eigenvalues is equal to nullity. So, the rank of D(Cn)=n if n is odd and the rank of D(Cn)=n2+1 if n is even. Again by Theorem 1.2, we get the rank of D(Pm) is m. Now by applying Theorem 1.5, we get the rank of JmD(Cn) is n and n2+1 if n is odd and even, respectively, and the rank of D(Pm)Jn is m. Thus, from EquationEquation (2), we get Rank(D(Umn))Rank(JmD(Cn))+Rank(D(Pm)Jn)={n+m,     when n is oddn2+m+1,     when nis even.

Now, we consider the matrix Jm+D(Pm). Then, by considering all edge weight 1 of Pm and applying Theorem 1.4, we get the determinant of Jm+D(Pm) is nonzero. So, the rank of Jm+D(Pm) is m. Then, we have (3) Rank(Jm+D(Pm))Rank(Jm)+Rank(D(Pm))m1+m(3)

Thus, the rank additivity does not hold in (Citation16). So, by applying Theorem 1.6, we get there is some nonzero vector y such that y(range(Jm)range(D(Pm)). Then, there exist some vectors x1 and x2 such that y=Jmx1=D(Pm)x2. Let k be the constant row sum of D(Cn). We consider the nonzero vectors X1=1kx1jn and X2=1nx2jn. Then, (JmD(Cn))X1=1k(JmD(Cn))(x1jn)=1k((Jmx1)(D(Cn)jn)=1k(y(kjn))=(yjn)

Similarly, we have (D(Pm)Jn)X2=(yjn)

Thus, we get a nonzero vector yjn such that (yjn)(range(JmD(Cn))range(D(Pm)Jn). So, the rank additivity does not hold in (Citation13). Then, we have Rank(D(Umn))<Rank(JmD(Cn))+Rank(D(Pm)Jn)={n+m,     when n is oddn2+m+1,     when nis even.

Hence, the number of zero eigenvalues which is the nullity of D(Umn) is at least mnmn+1 and mnmn2 according as n is odd and even, respectively. □

Our next result shows some quotient matrix of D(Umn) corresponding to an equitable partition. From this quotient matrix, we find m nonzero eigenvalues of D(Umn).

Theorem 2.2.

The eigenvalues of nD(Pm)+n24Jm and the eigenvalues of nD(Pm)+n214Jm are also some nonzero eigenvalues of the distance matrix of Umn according as n is even and odd, respectively.

Proof.

We consider the partition of D(Umn) as in EquationEquation (1). We note that each row sum of D(Cn) is constant and is equal to n24 and n214 according as n is even and odd, respectively. Then, the considered partition of D(Umn) is equitable. Now if n is even, then the corresponding quotient matrix is Q1=[n24n24+nn24+2nn24+(m1)nn24+nn24n24+nn24+(m2)nn24+2nn24+nn24n24+(m3)nn24+(m1)nn24+(m2)nn24+(m3)nn24]=[n24n24n24n24n24n24n24n24n24n24n24n24n24n24n24n24]+[0n2n(m1)nn0n(m2)n2nn0(m3)n(m1)n(m2)n(m3)n0]=n24Jm+nD(Pm)

Similarly, we get if n is odd, then the quotient matrix of D(Umn) corresponding to the equitable partition of (1) is given by Q2=n214Jm+nD(Pm).

Then, by Theorem 1.1, we get the eigenvalues of nD(Pm)+n24Jm and the eigenvalues of nD(Pm)+n214Jm are also some eigenvalues of the distance matrix of Umn according as n is even and odd, respectively. Finally, considering all edge weights 1 for the tree Pm in Theorem 1.4, we conclude that the determinants of both the matrices Q1 and Q2 are nonzero. Hence, eigenvalues of Q1 and Q2 are nonzero eigenvalues of D(Umn) according as n is even and odd, respectively. □

Some of the nonzero eigenvalues of D(Umn) are still remaining. The following result provides these nonzero eigenvalues.

Theorem 2.3.

Let λ be a nonzero eigenvalue of D(Cn) other than the constant row sum. Then mλ is an eigenvalue of D(Umn).

Proof.

We note that if k is a constant row sum of D(Cn) then jn is an eigenvector of D(Cn) corresponding to the eigenvalue k. Let x be an eigenvector of D(Cn) corresponding to the nonzero eigenvalue λ. Then as D(Cn) is symmetric, all of its independent eigenvectors are orthogonal. Then, jnTx=0, so that Jnx = 0. Then, from EquationEquation (2), we get D(Umn)(jmx)=(JmD(Cn)+D(Pm)Jn)(jmx)=(Jmjm)(D(Cn)x)+(D(Pm)jm)(Jnx)=(mjm)(λx)+(D(Pm)jm)(0)=mλ(jmx).

Hence, we get mλ is an eigenvalue of D(Umn) corresponding to the eigenvector jmx.

Remark 2.1.

We claim that the nonzero eigenvalues of D(Umn) obtained from Theorem 2.2 and Theorem 2.3 are different. Assume that μ is an eigenvalue of nD(Pm)+kJm corresponding to the eigenvector y, where k=n24 or k=n214 according as n is even and odd, respectively. We note that this k is the constant row sum of D(Cn) according as n is even and odd, respectively. Let λ be an nonzero eigenvalue of D(Cn) other than k corresponding to the eigenvector x. Now we have (JmD(Cn)+D(Pm)Jn)(yjn)=JmyD(Cn)jn+D(Pm)yJnjn=Jmykjn+D(Pm)ynjn=kJmyjn+nD(Pm)yjn=(kJm+nD(Pm))yjn=μ(yjn).

This shows that yjn is an eigenvector of D(Umn) corresponding to the eigenvalue μ. Also, from the proof of Theorem 2.3, we get mλ is an eigenvalue of D(Umn) corresponding to the eigenvector jmx.

If possible let μ=mλ, then for some scalar c we have yjn=c(jmx). Then, this gives all components of x are equal which is impossible as jnTx=0. Hence, the nonzero eigenvalues of D(Umn) obtained from Theorem 2.2 and Theorem 2.3 are different.

Theorem 2.4.

The characteristic polynomial of the distance matrix of Umn is given by P(t)=tmnmn2det(tImn24JmnD(Pm))j=1n2(t+mcsc2(π(2j1)n)), if nis even.               p(t)=tmnmn+1det(tImn214JmnD(Pm))j=1n12(t+m14sec2(πjn))j=1n12(t+m14csc2(π(2j1)2n)), if nis odd.

Proof.

From the Theorems 2.2, 2.3, 1.3 and from Remark 2.1, the number of nonzero eigenvalues of D(Umn) is at least equal to {n+m1,     when n is oddn2+m,     when nis even.

Thus, the number of zero eigenvalues is at most mnmn+1 and mnmn2 according as n is odd and even, respectively. Then, from Theorem 2.1, we get the number of zero eigenvalues of D(Umn) is exactly mnmn+1 and mnmn2 according as n is odd and even, respectively. Hence, the characteristic polynomial of D(Umn) is P(t)=tmnmn2det(tImn24JmnD(Pm))j=1n2(t+mcsc2(π(2j1)n)), if nis even.               p(t)=tmnmn+1det(tImn214JmnD(Pm))j=1n12(t+m14sec2(πjn))j=1n12(t+m14csc2(π(2j1)2n)), if nis odd.

Now, by applying Theorem 2.4, one can find the explicit eigenvalues of D(Umn). As an example, we provide the explicit distance eigenvalues of U3n.

Theorem 2.5.

Distance eigenvalues of U3n are as follows:

When n is even:

2n,n8(3n+8±9n2+80n+192),3csc2(π(2j1)n) for j=1,2,,n2 together with zero with multiplicity 5n62.

When n is odd:

2n,18(3n2+8n3±9n4+80n3+174n280n+9),34sec2(πjn),34csc2(π(2j1)2n) for j=1,2,,n12 together with zero with multiplicity 2n2.

Proof.

We have eigenvalues of n24J3nD(P3)=[n24n24+nn24+2nn24+nn24n24+nn24+2nn24+nn24] are 2n and n8(3n+8±9n2+80n+192).

Also, the eigenvalues of n214J3nD(P3)=[n214n214+nn214+2nn214+nn214n214+nn214+2nn214+nn214] are 2n and

18(3n2+8n3±9n4+80n3+174n280n+9). Hence, applying Theorem 2.4, we get the desired result. □

Acknowledgement

The authors are thankful to the anonymous referees for various comments and suggestions.

Additional information

Funding

The authors would like to thank the Department of Science and Technology, India, for the financial support (start-up research grant (SRG/2019/000839)).

References

  • Graham, R. L, Pollak, H. O. (1971). On the addressing problem for loop switching. Bell Syst. Tech. J. 50(8): 2495–2519.
  • Balaban, A. T., Ciubotariu, D, Medeleanu, M. (1991). Topological indices and real number vertex invariants based on graph eigenvalues or eigenvectors. J. Chem. Inf. Model. 31(4): 517–523.
  • Gutman, I, Medeleanu, M. (1998). On the structure-dependence of the largest eigenvalue of the distance matrix of an alkane. Indian J. Chem. 37A: 569–573.
  • Consonni, V, Todeschini, R. (2008). New spectral indices for molecule description. MATCH Commun. Math. Comput. Chem. 60: 3–14.
  • Todeschini, R, Consonni, V. (2000). Handbook of Molecular Descriptors. Weinheim: Wiley-VCH.
  • Graham, R. L, Lovasz, L. (1978). Distance matrix polynomials of trees. Adv. Math. 29(1): 60–88.
  • Ruzieh, S. N, Powers, D. L. (1990). The distance spectrum of the path Pn and the first distance eigenvector of connected graphs. Linear Multilinear Algebra 28(1–2): 75–81.
  • Fowler, P. W., Caporossi, G, Hansen, P. (2001). Distance matrices, wiener indices, and related invariants of fullerenes. J. Phys. Chem. A. 105(25): 6232–6242.
  • Lin, H. Q., Hong, Y., Wang, J. F, Shu, J. L. (2013). On the distance spectrum of graphs. Linear Algebra Appl. 439(6): 1662–1669.
  • Atik, F, Panigrahi, P. (2015). On the distance spectrum of distance regular graphs. Linear Algebra Appl. 478: 256–273.
  • Atik, F, Panigrahi, P. (2018). On the distance and distance signlesslaplacian eigenvalues of graphs and the smallest ger sˇ gorin disc. Electron. J. Linear Algebra 34: 191–204.
  • Aalipour, G., Abiad, A., Berikkyzy, Z., Cummings, J., De Silva, J., Gao, W., Heysse, K., Hogben, L., Kenter, F. H., Lin, J. C. H., et al. (2016). On the distance spectra of graphs. Linear Algebra Appl. 497: 66–87.
  • Alazemi, A., Anđelić, M., Koledin, T, Stanić, Z. (2017). Distance-regular graphs with small number of distinct distance eigenvalues. Linear Algebra Appl. 531: 83–97.
  • Lu, L, Huang, Q. (2021). Distance eigenvalues of B(n, k). Linear Multilinear Algebra 69(11): 2078–2092.
  • Pirzada, S., Ganie, H. A., Rather, B. A, Ul Shaban, R. (2020). On spectral spread of generalized distance matrix of a graph. Linear Multilinear Algebra 603: 1–19.
  • Alhevaz, A., Baghipur, M., Ganie, H. A, Shang, Y. (2019). On the generalized distance energy of graphs. Mathematics 8(1): 17.
  • DeVille, L. (2022). The generalized distance spectrum of a graph and applications. Linear Multilinear Algebra 70(13): 2425–2458.
  • Guo, H, Zhou, B. (2020). On the distance α-spectral radius of a connected graph. J. Inequal. Appl. 2020(1): 1–21.
  • Aouchiche, M, Hansen, P. (2014). Distance spectra of graphs: A survey. Linear Algebra Appl. 458: 301–386.
  • Hogben, L, Reinhart, C. (2022). Spectra of variants of distance matrices of graphs and digraphs: a survey. La Mathematica. 1(1): 186–224.
  • Brouwer, A. E, Haemers, W. H. (2011). Spectra of Graphs. Springer: Springer Science & Business Media.
  • Bapat, R. B., Kirkland, S. J, Neumann, M. (2005). On distance matrices and Laplacians. Linear Algebra Appl. 401: 193–209.
  • Laub, A. J. (2004). Matrix Analysis for Scientists and Engineers. Philadelphia: Society for Industrial and Applied Mathematics.
  • Horn, R. A, Johnson, C. R. (2012). Matrix Analysis. Cambridge: Cambridge University Press.