DOCSLIB.ORG

On the Eigenvalues of Euclidean Distance Matrices

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
On the Eigenvalues of Euclidean Distance Matrices “main” — 2008/10/13 — 23:12 — page 237 — #1 Volume 27, N. 3, pp. 237–250, 2008 Copyright © 2008 SBMAC ISSN 0101-8205 www.scielo.br/cam On the eigenvalues of Euclidean distance matrices A.Y. ALFAKIH∗ Department of Mathematics and Statistics University of Windsor, Windsor, Ontario N9B 3P4, Canada E-mail: [email protected] Abstract. In this paper, the notion of equitable partitions (EP) is used to study the eigenvalues of Euclidean distance matrices (EDMs). In particular, EP is used to obtain the characteristic poly- nomials of regular EDMs and non-spherical centrally symmetric EDMs. The paper also presents methods for constructing cospectral EDMs and EDMs with exactly three distinct eigenvalues. Mathematical subject classification: 51K05, 15A18, 05C50. Key words: Euclidean distance matrices, eigenvalues, equitable partitions, characteristic poly- nomial. 1 Introduction ( ) An n ×n nonzero matrix D = di j is called a Euclidean distance matrix (EDM) 1, 2,..., n r if there exist points p p p in some Euclidean space < such that i j 2 , ,..., , di j = ||p − p || for all i j = 1 n where || || denotes the Euclidean norm. i , ,..., Let p , i ∈ N = {1 2 n}, be the set of points that generate an EDM π π ( , ,..., ) D. An m-partition of D is an ordered sequence = N1 N2 Nm of ,..., nonempty disjoint subsets of N whose union is N. The subsets N1 Nm are called the cells of the partition. The n-partition of D where each cell consists #760/08. Received: 07/IV/08. Accepted: 17/VI/08. ∗Research supported by the Natural Sciences and Engineering Research Council of Canada and MITACS. “main” — 2008/10/13 — 23:12 — page 238 — #2 238 ON THE EIGENVALUES OF EUCLIDEAN DISTANCE MATRICES of a single point is called the discrete partition, while the 1-partition of D with only one cell is called the single-cell partition. π ( , ,..., ) An m-partition = N1 N2 Nm of an EDM D is said to be equitable , ,..., if for all i j = 1 m (case i = j included), there exist non-negative scalars α i j such that for each k ∈ Ni , the sum of the squared Euclidean distances from k l α p to all points p , l in N j , is equal to i j . i.e., , α , , ,..., . ∀ k ∈ Ni dkl = i j for all i j = 1 m (1) lX∈N j The notion of equitable partitions for graphs, which was introduced by Sachs [13], is related to, among others, automorphism groups of graphs and distance- regular graphs [4]. Schwenk [15] used equitable partitions to find the eigenvalues of the adjacency matrix of a graph. Hayden et al. [7] also used equitable parti- tions, albeit under the name block structure, to investigate EDMs generated by points lying on a collection of concentric spheres. In particular, they devised an algorithm for finding the least number of concentric spheres containing the points that generate a given EDM. Their investigation was based on the block structure of EDMs and the corresponding eigenvectors. Many of the results on the spectra of graphs obtained using equitable parti- tions have analogous counterparts in the case of EDMs. In particular, we show (see Theorem 3.1) that the characteristic polynomial of an EDM can be written as the product of the characteristic polynomials of two matrices associated with partitions. Theorem 3.1 is then used to determine the characteristic polynomials of regular EDMs and non-spherical centrally symmetric EDMs. We also present methods for constructing cospectral EDMs and non-regular EDMs with exactly three distinct eigenvalues. Recently, EDMs have received a great deal of attention for their many impor- tant applications. These applications include, among others, molecular confor- mation problems in chemistry [2], multidimensional scaling in statistics [9], and wireless sensor network localization problems [16]. We denote the identity matrix of order n by In and the n-vector of all 1’s , T T by en. En m = enem denotes the n × m matrix of all 1’s, and En = enen denotes the square matrix of order n of all 1’s. The subscripts of I , e and E will be deleted if the order is clear from the context. For a matrix A, diag A Comp. Appl. Math., Vol. 27, N. 3, 2008 “main” — 2008/10/13 — 23:12 — page 239 — #3 A.Y. ALFAKIH 239 denotes the vector consisting of the diagonal entries of A. Finally, the spec- trum of a matrix A, denoted by σ (A), is the multiset of the eigenvalues of A. λ , . , λ ,..., If A has eigenvalues 1 k with multiplicities m1 mk respectively, σ( ) λm1 , . , λmk then D = { 1 k }. 2 Preliminaries 1,..., n Let D be an n×n EDM, the dimension of the affine span of the points p p T / that generate D is called the embedding dimension of D. Let Jn := In − enen n denote the orthogonal projection on subspace ⊥ n T . M := e = x ∈ < : e x = 0 (2) It is well known [14, 18] that a symmetric matrix D with zero diagonal is an EDM if and only if D is negative semidefinite on M. Hence, EDMs have exactly one positive eigenvalue. Let SH denote the subset of n × n symmetric matrices with zero diagonal; and let SC denote the subset of n × n symmetric matrices A satisfying Ae = 0. Following [3], let T : SH → SC and K : SC → SH be the two linear maps defined by 1 (D) JDJ, (3) T := −2 and ( ) ( ) T ( ( ))T . K B := diag B e + e diag B − 2B (4) It, then, immediately follows [3] that T and K are mutually inverse, and that ( ) D in SH is an EDM of embedding dimension r if and only if T D is positive semidefinite of rank r. Let D be an n × n EDM of embedding dimension r generated by the points 1,..., n r p p in < . Then the n × r matrix T p1 . . P = n T p is called a realization of D. Given an EDM D, a realization P of D can be ob- ( ) ( ) T tained by factorizing T D into T D = PP . Note that if P is a realization Comp. Appl. Math., Vol. 27, N. 3, 2008 “main” — 2008/10/13 — 23:12 — page 240 — #4 240 ON THE EIGENVALUES OF EUCLIDEAN DISTANCE MATRICES 0 of D, then P = PQ is also a realization of D for any r × r orthogonal matrix Q. Obviously, P and P0 in this case are obtained from each other by a rigid motion such as a rotation or a translation. An EDM D is said to be spherical if the points that generate D lie on a hyper- sphere, otherwise, it is said to be non-spherical. It is well known [6, 17] that an EDM D of embedding dimension r is spherical if and only if rank D = r + 1, and that D is non-spherical if and only if rank D = r + 2. A spherical EDM D is said to be regular if the points p1,..., pn that generate D lie on a hyper-sphere whose center coincides with the centroid of p1,..., pn. It is not difficult to show that [12, 8] an EDM D is regular if and only if e is an eigenvector of D 1 T corresponding to the eigenvalue n e De. 3 Equitable partition for EDMs It immediately follows from (1) that the discrete partition of D is always equi- α table with i j = di j ; while the single-cell partition of D is equitable if and only α 1 T if D is regular. In the latter case, 11 = n e De. It also follows from (1) that m ,..., ( ) α . ∀ i = 1 m and ∀ k ∈ Ni we have De k = i j (5) Xj=1 π ( , ,..., ) Let = N1 N2 Nm be an m-partition of an n × n EDM D where ,..., π ( ) |Ni | = ni for i = 1 m. Define the n × m matrix P = pi j such that / −1 2 n j if i ∈ N j pi j = (6) ( 0 otherwise. Pπ is called the normalized characteristic matrix [5] of π since its jth column 1/2 − T π is equal to n j times the characteristic vector of N j , and since Pπ P = Im. Next we present a lemma whose graph adjacency matrix counterpart was proved by Godsil and McKay [5]. Lemma 3.1. Let π be an m-partition of an EDM D. Then π is equitable if and ( ) only if there exists an m × m symmetric matrix S = si j such that π π . DP = P S (7) π ( / )1/2 α Furthermore, if is an equitable partition then si j = ni n j i j . Comp. Appl. Math., Vol. 27, N. 3, 2008 “main” — 2008/10/13 — 23:12 — page 241 — #5 A.Y. ALFAKIH 241 π ,..., Proof. Assume that is equitable then for all k ∈ Ni and for all j = 1 m we have 1/2 1/2 1/2 / ni ( π ) − − α ( )−1 2 α ( π ) , DP kj = n j dkl = n j i j = ni i j = P S kj n j lX∈N j ( / )1/2α where si j = ni n j i j . On the other hand, assume that (7) holds for some partition π. Then for all ,..., k ∈ Ni and all j = 1 m, we have 1/2 / ( π ) − ( π ) ( )−1 2 . DP kj = n j dkl = P S kj = ni si j lX∈N j ( / )1/2 π kl j i i j Therefore, l∈N j d = n n s , which is independent of k.
Load more

Recommended publications
  • Math 221: LINEAR ALGEBRA
    Math 221: LINEAR ALGEBRA Chapter 8. Orthogonality §8-3. Positive Definite Matrices Le Chen1 Emory University, 2020 Fall (last updated on 11/10/2020) Creative Commons License (CC BY-NC-SA) 1 Slides are adapted from those by Karen Seyffarth from University of Calgary. Positive Definite Matrices Cholesky factorization – Square Root of a Matrix Positive Definite Matrices Definition An n × n matrix A is positive definite if it is symmetric and has positive eigenvalues, i.e., if λ is a eigenvalue of A, then λ > 0. Theorem If A is a positive definite matrix, then det(A) > 0 and A is invertible. Proof. Let λ1; λ2; : : : ; λn denote the (not necessarily distinct) eigenvalues of A. Since A is symmetric, A is orthogonally diagonalizable. In particular, A ∼ D, where D = diag(λ1; λ2; : : : ; λn). Similar matrices have the same determinant, so det(A) = det(D) = λ1λ2 ··· λn: Since A is positive definite, λi > 0 for all i, 1 ≤ i ≤ n; it follows that det(A) > 0, and therefore A is invertible. Theorem A symmetric matrix A is positive definite if and only if ~xTA~x > 0 for all n ~x 2 R , ~x 6= ~0. Proof. Since A is symmetric, there exists an orthogonal matrix P so that T P AP = diag(λ1; λ2; : : : ; λn) = D; where λ1; λ2; : : : ; λn are the (not necessarily distinct) eigenvalues of A. Let n T ~x 2 R , ~x 6= ~0, and define ~y = P ~x. Then ~xTA~x = ~xT(PDPT)~x = (~xTP)D(PT~x) = (PT~x)TD(PT~x) = ~yTD~y: T Writing ~y = y1 y2 ··· yn , 2 y1 3 6 y2 7 ~xTA~x = y y ··· y diag(λ ; λ ; : : : ; λ ) 6 7 1 2 n 1 2 n 6 .
    [Show full text]
  • Parametrizations of K-Nonnegative Matrices
    Parametrizations of k-Nonnegative Matrices Anna Brosowsky, Neeraja Kulkarni, Alex Mason, Joe Suk, Ewin Tang∗ October 2, 2017 Abstract Totally nonnegative (positive) matrices are matrices whose minors are all nonnegative (positive). We generalize the notion of total nonnegativity, as follows. A k-nonnegative (resp. k-positive) matrix has all minors of size k or less nonnegative (resp. positive). We give a generating set for the semigroup of k-nonnegative matrices, as well as relations for certain special cases, i.e. the k = n − 1 and k = n − 2 unitriangular cases. In the above two cases, we find that the set of k-nonnegative matrices can be partitioned into cells, analogous to the Bruhat cells of totally nonnegative matrices, based on their factorizations into generators. We will show that these cells, like the Bruhat cells, are homeomorphic to open balls, and we prove some results about the topological structure of the closure of these cells, and in fact, in the latter case, the cells form a Bruhat-like CW complex. We also give a family of minimal k-positivity tests which form sub-cluster algebras of the total positivity test cluster algebra. We describe ways to jump between these tests, and give an alternate description of some tests as double wiring diagrams. 1 Introduction A totally nonnegative (respectively totally positive) matrix is a matrix whose minors are all nonnegative (respectively positive). Total positivity and nonnegativity are well-studied phenomena and arise in areas such as planar networks, combinatorics, dynamics, statistics and probability. The study of total positivity and total nonnegativity admit many varied applications, some of which are explored in “Totally Nonnegative Matrices” by Fallat and Johnson [5].
    [Show full text]
  • Eigenvalues of Euclidean Distance Matrices and Rs-Majorization on R2
    Archive of SID 46th Annual Iranian Mathematics Conference 25-28 August 2015 Yazd University 2 Talk Eigenvalues of Euclidean distance matrices and rs-majorization on R pp.: 1{4 Eigenvalues of Euclidean Distance Matrices and rs-majorization on R2 Asma Ilkhanizadeh Manesh∗ Department of Pure Mathematics, Vali-e-Asr University of Rafsanjan Alemeh Sheikh Hoseini Department of Pure Mathematics, Shahid Bahonar University of Kerman Abstract Let D1 and D2 be two Euclidean distance matrices (EDMs) with correspond- ing positive semidefinite matrices B1 and B2 respectively. Suppose that λ(A) = ((λ(A)) )n is the vector of eigenvalues of a matrix A such that (λ(A)) ... i i=1 1 ≥ ≥ (λ(A))n. In this paper, the relation between the eigenvalues of EDMs and those of the 2 corresponding positive semidefinite matrices respect to rs, on R will be investigated. ≺ Keywords: Euclidean distance matrices, Rs-majorization. Mathematics Subject Classification [2010]: 34B15, 76A10 1 Introduction An n n nonnegative and symmetric matrix D = (d2 ) with zero diagonal elements is × ij called a predistance matrix. A predistance matrix D is called Euclidean or a Euclidean distance matrix (EDM) if there exist a positive integer r and a set of n points p1, . , pn r 2 2 { } such that p1, . , pn R and d = pi pj (i, j = 1, . , n), where . denotes the ∈ ij k − k k k usual Euclidean norm. The smallest value of r that satisfies the above condition is called the embedding dimension. As is well known, a predistance matrix D is Euclidean if and 1 1 t only if the matrix B = − P DP with P = I ee , where I is the n n identity matrix, 2 n − n n × and e is the vector of all ones, is positive semidefinite matrix.
    [Show full text]
  • Polynomial Approximation Algorithms for Belief Matrix Maintenance in Identity Management
    Polynomial Approximation Algorithms for Belief Matrix Maintenance in Identity Management Hamsa Balakrishnan, Inseok Hwang, Claire J. Tomlin Dept. of Aeronautics and Astronautics, Stanford University, CA 94305 hamsa,ishwang,[email protected] Abstract— Updating probabilistic belief matrices as new might be constrained to some prespecified (but not doubly- observations arrive, in the presence of noise, is a critical part stochastic) row and column sums. This paper addresses the of many algorithms for target tracking in sensor networks. problem of updating belief matrices by scaling in the face These updates have to be carried out while preserving sum constraints, arising for example, from probabilities. This paper of uncertainty in the system and the observations. addresses the problem of updating belief matrices to satisfy For example, consider the case of the belief matrix for a sum constraints using scaling algorithms. We show that the system with three objects (labelled 1, 2 and 3). Suppose convergence behavior of the Sinkhorn scaling process, used that, at some instant, we are unsure about their identities for scaling belief matrices, can vary dramatically depending (tagged X, Y and Z) completely, and our belief matrix is on whether the prior unscaled matrix is exactly scalable or only almost scalable. We give an efficient polynomial-time algo- a 3 × 3 matrix with every element equal to 1/3. Let us rithm based on the maximum-flow algorithm that determines suppose the we receive additional information that object whether a given matrix is exactly scalable, thus determining 3 is definitely Z. Then our prior, but constraint violating the convergence properties of the Sinkhorn scaling process.
    [Show full text]
  • Orthogonal Reduction 1 the Row Echelon Form -.: Mathematical
    MATH 5330: Computational Methods of Linear Algebra Lecture 9: Orthogonal Reduction Xianyi Zeng Department of Mathematical Sciences, UTEP 1 The Row Echelon Form Our target is to solve the normal equation: AtAx = Atb ; (1.1) m×n where A 2 R is arbitrary; we have shown previously that this is equivalent to the least squares problem: min jjAx−bjj : (1.2) x2Rn t n×n As A A2R is symmetric positive semi-definite, we can try to compute the Cholesky decom- t t n×n position such that A A = L L for some lower-triangular matrix L 2 R . One problem with this approach is that we're not fully exploring our information, particularly in Cholesky decomposition we treat AtA as a single entity in ignorance of the information about A itself. t m×m In particular, the structure A A motivates us to study a factorization A=QE, where Q2R m×n is orthogonal and E 2 R is to be determined. Then we may transform the normal equation to: EtEx = EtQtb ; (1.3) t m×m where the identity Q Q = Im (the identity matrix in R ) is used. This normal equation is equivalent to the least squares problem with E: t min Ex−Q b : (1.4) x2Rn Because orthogonal transformation preserves the L2-norm, (1.2) and (1.4) are equivalent to each n other. Indeed, for any x 2 R : jjAx−bjj2 = (b−Ax)t(b−Ax) = (b−QEx)t(b−QEx) = [Q(Qtb−Ex)]t[Q(Qtb−Ex)] t t t t t t t t 2 = (Q b−Ex) Q Q(Q b−Ex) = (Q b−Ex) (Q b−Ex) = Ex−Q b : Hence the target is to find an E such that (1.3) is easier to solve.
    [Show full text]
  • Chapter Four Determinants
    Chapter Four Determinants In the first chapter of this book we considered linear systems and we picked out the special case of systems with the same number of equations as unknowns, those of the form T~x = ~b where T is a square matrix. We noted a distinction between two classes of T ’s. While such systems may have a unique solution or no solutions or infinitely many solutions, if a particular T is associated with a unique solution in any system, such as the homogeneous system ~b = ~0, then T is associated with a unique solution for every ~b. We call such a matrix of coefficients ‘nonsingular’. The other kind of T , where every linear system for which it is the matrix of coefficients has either no solution or infinitely many solutions, we call ‘singular’. Through the second and third chapters the value of this distinction has been a theme. For instance, we now know that nonsingularity of an n£n matrix T is equivalent to each of these: ² a system T~x = ~b has a solution, and that solution is unique; ² Gauss-Jordan reduction of T yields an identity matrix; ² the rows of T form a linearly independent set; ² the columns of T form a basis for Rn; ² any map that T represents is an isomorphism; ² an inverse matrix T ¡1 exists. So when we look at a particular square matrix, the question of whether it is nonsingular is one of the first things that we ask. This chapter develops a formula to determine this. (Since we will restrict the discussion to square matrices, in this chapter we will usually simply say ‘matrix’ in place of ‘square matrix’.) More precisely, we will develop infinitely many formulas, one for 1£1 ma- trices, one for 2£2 matrices, etc.
    [Show full text]
  • Handout 9 More Matrix Properties; the Transpose
    Handout 9 More matrix properties; the transpose Square matrix properties These properties only apply to a square matrix, i.e. n £ n. ² The leading diagonal is the diagonal line consisting of the entries a11, a22, a33, . ann. ² A diagonal matrix has zeros everywhere except the leading diagonal. ² The identity matrix I has zeros o® the leading diagonal, and 1 for each entry on the diagonal. It is a special case of a diagonal matrix, and A I = I A = A for any n £ n matrix A. ² An upper triangular matrix has all its non-zero entries on or above the leading diagonal. ² A lower triangular matrix has all its non-zero entries on or below the leading diagonal. ² A symmetric matrix has the same entries below and above the diagonal: aij = aji for any values of i and j between 1 and n. ² An antisymmetric or skew-symmetric matrix has the opposite entries below and above the diagonal: aij = ¡aji for any values of i and j between 1 and n. This automatically means the digaonal entries must all be zero. Transpose To transpose a matrix, we reect it across the line given by the leading diagonal a11, a22 etc. In general the result is a di®erent shape to the original matrix: a11 a21 a11 a12 a13 > > A = A = 0 a12 a22 1 [A ]ij = A : µ a21 a22 a23 ¶ ji a13 a23 @ A > ² If A is m £ n then A is n £ m. > ² The transpose of a symmetric matrix is itself: A = A (recalling that only square matrices can be symmetric).
    [Show full text]
  • Smith Normal Formal of Distance Matrix of Block Graphs∗†
    Ann. of Appl. Math. 32:1(2016); 20-29 SMITH NORMAL FORMAL OF DISTANCE MATRIX OF BLOCK GRAPHS∗y Jing Chen1;2,z Yaoping Hou2 (1. The Center of Discrete Math., Fuzhou University, Fujian 350003, PR China; 2. School of Math., Hunan First Normal University, Hunan 410205, PR China) Abstract A connected graph, whose blocks are all cliques (of possibly varying sizes), is called a block graph. Let D(G) be its distance matrix. In this note, we prove that the Smith normal form of D(G) is independent of the interconnection way of blocks and give an explicit expression for the Smith normal form in the case that all cliques have the same size, which generalize the results on determinants. Keywords block graph; distance matrix; Smith normal form 2000 Mathematics Subject Classification 05C50 1 Introduction Let G be a connected graph (or strong connected digraph) with vertex set f1; 2; ··· ; ng. The distance matrix D(G) is an n × n matrix in which di;j = d(i; j) denotes the distance from vertex i to vertex j: Like the adjacency matrix and Lapla- cian matrix of a graph, D(G) is also an integer matrix and there are many results on distance matrices and their applications. For distance matrices, Graham and Pollack [10] proved a remarkable result that gives a formula of the determinant of the distance matrix of a tree depend- ing only on the number n of vertices of the tree. The determinant is given by det D = (−1)n−1(n − 1)2n−2: This result has attracted much interest in algebraic graph theory.
    [Show full text]
  • Arxiv:1803.06211V1 [Math.NA] 16 Mar 2018
    A NUMERICAL MODEL FOR THE CONSTRUCTION OF FINITE BLASCHKE PRODUCTS WITH PREASSIGNED DISTINCT CRITICAL POINTS CHRISTER GLADER AND RAY PORN¨ Abstract. We present a numerical model for determining a finite Blaschke product of degree n + 1 having n preassigned distinct critical points z1; : : : ; zn in the complex (open) unit disk D. The Blaschke product is uniquely determined up to postcomposition with conformal automor- phisms of D. The proposed method is based on the construction of a sparse nonlinear system where the data dependency is isolated to two vectors and on a certain transformation of the critical points. The effi- ciency and accuracy of the method is illustrated in several examples. 1. Introduction A finite Blaschke product of degree n is a rational function of the form n Y z − αj (1.1) B(z) = c ; c; α 2 ; jcj = 1; jα j < 1 ; 1 − α z j C j j=1 j which thereby has all its zeros in the open unit disc D, all poles outside the closed unit disc D and constant modulus jB(z)j = 1 on the unit circle T. The overbar in (1.1) and in the sequel stands for complex conjugation. The finite Blaschke products of degree n form a subset of the rational functions of degree n which are unimodular on T. These functions are given by all fractions n ~ a0 + a1 z + ::: + an z (1.2) B(z) = n ; a0; :::; an 2 C : an + an−1 z + ::: + a0 z An irreducible rational function of form (1.2) is a finite Blaschke product when all its zeros are in D.
    [Show full text]
  • 4.1 RANK of a MATRIX Rank List Given Matrix M, the Following Are Equal
    page 1 of Section 4.1 CHAPTER 4 MATRICES CONTINUED SECTION 4.1 RANK OF A MATRIX rank list Given matrix M, the following are equal: (1) maximal number of ind cols (i.e., dim of the col space of M) (2) maximal number of ind rows (i.e., dim of the row space of M) (3) number of cols with pivots in the echelon form of M (4) number of nonzero rows in the echelon form of M You know that (1) = (3) and (2) = (4) from Section 3.1. To see that (3) = (4) just stare at some echelon forms. This one number (that all four things equal) is called the rank of M. As a special case, a zero matrix is said to have rank 0. how row ops affect rank Row ops don't change the rank because they don't change the max number of ind cols or rows. example 1 12-10 24-20 has rank 1 (maximally one ind col, by inspection) 48-40 000 []000 has rank 0 example 2 2540 0001 LetM= -2 1 -1 0 21170 To find the rank of M, use row ops R3=R1+R3 R4=-R1+R4 R2ØR3 R4=-R2+R4 2540 0630 to get the unreduced echelon form 0001 0000 Cols 1,2,4 have pivots. So the rank of M is 3. how the rank is limited by the size of the matrix IfAis7≈4then its rank is either 0 (if it's the zero matrix), 1, 2, 3 or 4. The rank can't be 5 or larger because there can't be 5 ind cols when there are only 4 cols to begin with.
    [Show full text]
  • Distance Matrix and Laplacian of a Tree with Attached Graphs R.B
    Linear Algebra and its Applications 411 (2005) 295–308 www.elsevier.com/locate/laa Distance matrix and Laplacian of a tree with attached graphs R.B. Bapat ∗ Indian Statistical Institute, Delhi Centre, 7 S.J.S.S. Marg, New Delhi 110 016, India Received 5 November 2003; accepted 22 June 2004 Available online 7 August 2004 Submitted by S. Hedayat Abstract A tree with attached graphs is a tree, together with graphs defined on its partite sets. We introduce the notion of incidence matrix, Laplacian and distance matrix for a tree with attached graphs. Formulas are obtained for the minors of the incidence matrix and the Laplacian, and for the inverse and the determinant of the distance matrix. The case when the attached graphs themselves are trees is studied more closely. Several known results, including the Matrix Tree theorem, are special cases when the tree is a star. The case when the attached graphs are paths is also of interest since it is related to the transportation problem. © 2004 Elsevier Inc. All rights reserved. AMS classification: 15A09; 15A15 Keywords: Tree; Distance matrix; Resistance distance; Laplacian matrix; Determinant; Transportation problem 1. Introduction Minors of matrices associated with a graph has been an area of considerable inter- est, starting with the celebrated Matrix Tree theorem of Kirchhoff which asserts that any cofactor of the Laplacian matrix equals the number of spanning trees in the ∗ Fax: +91 11 26856779. E-mail address: [email protected] 0024-3795/$ - see front matter 2004 Elsevier Inc. All rights reserved. doi:10.1016/j.laa.2004.06.017 296 R.B.
    [Show full text]
  • Hypercubes Are Determined by Their Distance Spectra 3
    HYPERCUBES ARE DETERMINED BY THEIR DISTANCE SPECTRA JACK H. KOOLEN♦, SAKANDER HAYAT♠, AND QUAID IQBAL♣ Abstract. We show that the d-cube is determined by the spectrum of its distance matrix. 1. Introduction For undefined terms, see next section. For integers n 2 and d 2, the Ham- ming graph H(d, n) has as vertex set, the d-tuples with elements≥ from≥0, 1, 2,...,n 1 , with two d-tuples are adjacent if and only if they differ only in one{ coordinate.− For} a positive integer d, the d-cube is the graph H(d, 2). In this paper, we show that the d-cube is determined by its distance spectrum, see Theorem 5.4. Observe that the d-cube has exactly three distinct distance eigenvalues. Note that the d-cube is not determined by its adjacency spectrum as the Hoffman graph [11] has the same adjacency spectrum as the 4-cube and hence the cartesian product of (d 4)-cube and the Hoffman graph has the same adjacency spectrum − as the d-cube (for d 4, where the 0-cube is just K1). This also implies that the complement of the d-cube≥ is not determined by its distance spectrum, if d 4. ≥ There are quite a few papers on matrices of graphs with a few distinct eigenvalues. An important case is, when the Seidel matrix of a graph has exactly two distinct eigenvalues is very much studied, see, for example [18]. Van Dam and Haemers [20] characterized the graphs whose Laplacian matrix has two distinct nonzero eigenval- ues.
    [Show full text]