Polynomial Sequences Generated by Linear Recurrences
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Triangular Numbers /, 3,6, 10, 15, ", Tn,'" »*"
TRIANGULAR NUMBERS V.E. HOGGATT, JR., and IVIARJORIE BICKWELL San Jose State University, San Jose, California 9111112 1. INTRODUCTION To Fibonacci is attributed the arithmetic triangle of odd numbers, in which the nth row has n entries, the cen- ter element is n* for even /?, and the row sum is n3. (See Stanley Bezuszka [11].) FIBONACCI'S TRIANGLE SUMS / 1 =:1 3 3 5 8 = 2s 7 9 11 27 = 33 13 15 17 19 64 = 4$ 21 23 25 27 29 125 = 5s We wish to derive some results here concerning the triangular numbers /, 3,6, 10, 15, ", Tn,'" »*". If one o b - serves how they are defined geometrically, 1 3 6 10 • - one easily sees that (1.1) Tn - 1+2+3 + .- +n = n(n±M and (1.2) • Tn+1 = Tn+(n+1) . By noticing that two adjacent arrays form a square, such as 3 + 6 = 9 '.'.?. we are led to 2 (1.3) n = Tn + Tn„7 , which can be verified using (1.1). This also provides an identity for triangular numbers in terms of subscripts which are also triangular numbers, T =T + T (1-4) n Tn Tn-1 • Since every odd number is the difference of two consecutive squares, it is informative to rewrite Fibonacci's tri- angle of odd numbers: 221 222 TRIANGULAR NUMBERS [OCT. FIBONACCI'S TRIANGLE SUMS f^-O2) Tf-T* (2* -I2) (32-22) Ti-Tf (42-32) (52-42) (62-52) Ti-Tl•2 (72-62) (82-72) (9*-82) (Kp-92) Tl-Tl Upon comparing with the first array, it would appear that the difference of the squares of two consecutive tri- angular numbers is a perfect cube. -
Graph Equivalence Classes for Spectral Projector-Based Graph Fourier Transforms Joya A
1 Graph Equivalence Classes for Spectral Projector-Based Graph Fourier Transforms Joya A. Deri, Member, IEEE, and José M. F. Moura, Fellow, IEEE Abstract—We define and discuss the utility of two equiv- Consider a graph G = G(A) with adjacency matrix alence graph classes over which a spectral projector-based A 2 CN×N with k ≤ N distinct eigenvalues and Jordan graph Fourier transform is equivalent: isomorphic equiv- decomposition A = VJV −1. The associated Jordan alence classes and Jordan equivalence classes. Isomorphic equivalence classes show that the transform is equivalent subspaces of A are Jij, i = 1; : : : k, j = 1; : : : ; gi, up to a permutation on the node labels. Jordan equivalence where gi is the geometric multiplicity of eigenvalue 휆i, classes permit identical transforms over graphs of noniden- or the dimension of the kernel of A − 휆iI. The signal tical topologies and allow a basis-invariant characterization space S can be uniquely decomposed by the Jordan of total variation orderings of the spectral components. subspaces (see [13], [14] and Section II). For a graph Methods to exploit these classes to reduce computation time of the transform as well as limitations are discussed. signal s 2 S, the graph Fourier transform (GFT) of [12] is defined as Index Terms—Jordan decomposition, generalized k gi eigenspaces, directed graphs, graph equivalence classes, M M graph isomorphism, signal processing on graphs, networks F : S! Jij i=1 j=1 s ! (s ;:::; s ;:::; s ;:::; s ) ; (1) b11 b1g1 bk1 bkgk I. INTRODUCTION where sij is the (oblique) projection of s onto the Jordan subspace Jij parallel to SnJij. -
Odd and Even Lidstone-Type Polynomial Sequences. Part 1: Basic Topics F.A
Costabile et al. Advances in Difference Equations (2018)2018:299 https://doi.org/10.1186/s13662-018-1733-5 R E S E A R C H Open Access Odd and even Lidstone-type polynomial sequences. Part 1: basic topics F.A. Costabile1,M.I.Gualtieri1,A.Napoli1* and M. Altomare1 *Correspondence: [email protected] Abstract 1Department of Mathematics and Computer Science, University of Two new general classes of polynomial sequences called respectively odd and even Calabria, Rende, Italy Lidstone-type polynomials are considered. These classes include classic Lidstone polynomials of first and second kind. Some characterizations of the two classes are given, including matrix form, conjugate sequences, generating function, recurrence relations, and determinant forms. Some examples are presented and some applications are sketched. MSC: 41A58; 11B83 Keywords: Lidstone polynomials; Polynomial sequences; Infinite matrices 1 Introduction “Je m’occupe, dans ce Memoir, de certains polynômes en x formant une suite A0, A1,..., An,... dont le terme An est un polynôme de degré n et dans laquelle deux termes consécutifs dAn sont liés par la relation dx = nAn–1...”.[9] By paraphrasing Appell [9], we will consider a sequence of polynomials L0, L1,...,Lk, Lk+1,... such that two consecutive terms satisfy the differential relation d2 L (x)=c L (x), c ∈ R, k =1,2,.... (1) dx2 k k k–1 k We call this sequence Lidstone-type polynomial sequence (LPS). Really Lidstone [27] extended an Aitken’s theorem on general linear interpolation [8]to EveretttypeIandEveretttypeIIinterpolatoryformulas[32]. As an example, he considered d2 the dx2 operator and expansions of polynomials of odd and even degree involving two points, which are expressed in terms of a basis of polynomials satisfying (1). -
New Bell–Sheffer Polynomial Sets
axioms Article New Bell–Sheffer Polynomial Sets Pierpaolo Natalini 1,* and Paolo Emilio Ricci 2 1 Dipartimento di Matematica e Fisica, Università degli Studi Roma Tre, Largo San Leonardo Murialdo, 1, 00146 Roma, Italy 2 Sezione di Matematica, International Telematic University UniNettuno, Corso Vittorio Emanuele II, 39, 00186 Roma, Italy; [email protected] * Correspondence: [email protected] Received: 20 July 2018; Accepted: 2 October 2018; Published: 8 October 2018 Abstract: In recent papers, new sets of Sheffer and Brenke polynomials based on higher order Bell numbers, and several integer sequences related to them, have been studied. The method used in previous articles, and even in the present one, traces back to preceding results by Dattoli and Ben Cheikh on the monomiality principle, showing the possibility to derive explicitly the main properties of Sheffer polynomial families starting from the basic elements of their generating functions. The introduction of iterated exponential and logarithmic functions allows to construct new sets of Bell–Sheffer polynomials which exhibit an iterative character of the obtained shift operators and differential equations. In this context, it is possible, for every integer r, to define polynomials of higher type, which are linked to the higher order Bell-exponential and logarithmic numbers introduced in preceding papers. Connections with integer sequences appearing in Combinatorial analysis are also mentioned. Naturally, the considered technique can also be used in similar frameworks, where the iteration of exponential and logarithmic functions appear. Keywords: Sheffer polynomials; generating functions; monomiality principle; shift operators; combinatorial analysis 1. Introduction In recent articles [1,2], new sets of Sheffer [3] and Brenke [4] polynomials, based on higher order Bell numbers [2,5–7], have been studied. -
Physics 403, Spring 2011 Problem Set 2 Due Thursday, February 17
Physics 403, Spring 2011 Problem Set 2 due Thursday, February 17 1. A Differential Equation for the Legendre Polynomials (15 pts): In this prob- lem, we will derive a second order linear differential equation satisfied by the Legendre polynomials (−1)n dn P (x) = [(1 − x2)n] : n 2nn! dxn (a) Show that Z 1 2 0 0 Pm(x)[(1 − x )Pn(x)] dx = 0 for m 6= n : (1) −1 Conclude that 2 0 0 [(1 − x )Pn(x)] = λnPn(x) 0 for λn a constant. [ Prime here and in the following questions denotes d=dx.] (b) Perform the integral (1) for m = n to find a relation for λn in terms of the leading n coefficient of the Legendre polynomial Pn(x) = knx + :::. What is kn? 2. A Generating Function for the Legendre Polynomials (20 pts): In this problem, we will derive a generating function for the Legendre polynomials. (a) Verify that the Legendre polynomials satisfy the recurrence relation 0 0 0 Pn − 2xPn−1 + Pn−2 − Pn−1 = 0 : (b) Consider the generating function 1 X n g(x; t) = t Pn(x) : n=0 Use the recurrence relation above to show that the generating function satisfies the first order differential equation d (1 − 2xt + t2) g(x; t) = tg(x; t) : dx Determine the constant of integration by using the fact that Pn(1) = 1. (c) Use the generating function to express the potential for a point particle q jr − r0j in terms of Legendre polynomials. 1 3. The Dirac delta function (15 pts): Dirac delta functions are useful mathematical tools in quantum mechanics. -
Linear Recurrence Relations: the Theory Behind Them
Linear Recurrence Relations: The Theory Behind Them David Soukup October 29, 2019 Linear Recurrence Relations Contents 1 Foreword ii 2 The matrix diagonalization method 1 3 Generating functions 3 4 Analogies to ODEs 6 5 Exercises 8 6 References 10 i Linear Recurrence Relations 1 Foreword This guide is intended mostly for students in Math 61 who are looking for a more theoretical background to the solving of linear recurrence relations. A typical problem encountered is the following: suppose we have a sequence defined by an = 2an−1 + 3an−2 where a0 = 0; a1 = 8: Certainly this recurrence defines the sequence fang unambiguously (at least for positive integers n), and we can compute the first several terms without much problem: a0 = 0 a1 = 8 a2 = 2 · a1 + 3 · a0 = 2 · 8 + 3 · 0 = 16 a3 = 2 · a2 + 3 · a1 = 2 · 16 + 3 · 8 = 56 a4 = 2 · a3 + 3 · a2 = 2 · 56 + 3 · 16 = 160 . While this does allow us to compute the value of an for small n, this is unsatisfying for several reasons. For one, computing the value of a100 by this method would be time-consuming. If we solely use the recurrence, we would have to find the previous 99 values of the sequence first. Moreover, until we compute it we have no good idea of how large a100 will be. We can observe from the table above that an grows quite rapidly as n increases, but we do not know how to extrapolate this rate of growth to all n. Most importantly, we would like to know the order of growth of this function. -
Analysis of Non-Linear Recurrence Relations for the Recurrence Coefficients of Generalized Charlier Polynomials
Journal of Nonlinear Mathematical Physics Volume 10, Supplement 2 (2003), 231–237 SIDE V Analysis of Non-Linear Recurrence Relations for the Recurrence Coefficients of Generalized Charlier Polynomials Walter VAN ASSCHE † and Mama FOUPOUAGNIGNI ‡ † Katholieke Universiteit Leuven, Department of Mathematics, Celestijnenlaan 200 B, B-3001 Leuven, Belgium E-mail: [email protected] ‡ University of Yaounde, Advanced School of Education, Department of Mathematics, P.O. Box 47, Yaounde, Cameroon E-mail: [email protected] This paper is part of the Proceedings of SIDE V; Giens, June 21-26, 2002 Abstract The recurrence coefficients of generalized Charlier polynomials satisfy a system of non- linear recurrence relations. We simplify the recurrence relations, show that they are related to certain discrete Painlev´e equations, and analyze the asymptotic behaviour. 1 Introduction Orthogonal polynomials on the real line always satisfy a three-term recurrence relation. For monic polynomials Pn this is of the form Pn+1(x)=(x − βn)Pn(x) − γnPn−1(x), (1.1) with initial values P0 = 1 and P−1 = 0. For the orthonormal polynomials pn the recurrence relation is xpn(x)=an+1pn+1(x)+bnpn(x)+anpn−1(x), (1.2) 2 where an = γn and bn = βn. The recurrence coefficients are given by the integrals 2 an = xpn(x)pn−1(x) dµ(x),bn = xpn(x) dµ(x) and can also be expressed in terms of determinants containing the moments of the orthog- onality measure µ [11]. For classical orthogonal polynomials one knows these recurrence coefficients explicitly, but when one uses non-classical weights, then often one does not Copyright c 2003 by W Van Assche and M Foupouagnigni 232 W Van Assche and M Foupouagnigni know the recurrence coefficients explicitly. -
General Bivariate Appell Polynomials Via Matrix Calculus and Related Interpolation Hints
mathematics Article General Bivariate Appell Polynomials via Matrix Calculus and Related Interpolation Hints Francesco Aldo Costabile, Maria Italia Gualtieri and Anna Napoli * Department of Mathematics and Computer Science, University of Calabria, 87036 Rende (CS), Italy; [email protected] (F.A.C.); [email protected] (M.I.G.) * Correspondence: [email protected] Abstract: An approach to general bivariate Appell polynomials based on matrix calculus is proposed. Known and new basic results are given, such as recurrence relations, determinant forms, differential equations and other properties. Some applications to linear functional and linear interpolation are sketched. New and known examples of bivariate Appell polynomial sequences are given. Keywords: Polynomial sequences; Appell polynomials; bivariate Appell sequence 1. Introduction Appell polynomials have many applications in various disciplines: probability the- ory [1–5], number theory [6], linear recurrence [7], general linear interpolation [8–12], operators approximation theory [13–17]. In [18], P. Appell introduced a class of polynomi- als by the following equivalent conditions: fAngn2IN is an Appell sequence (An being a Citation: Costabile, F.A.; polynomial of degree n) if either Gualtieri, M.I.; Napoli, A. General 8 Bivariate Appell Polynomials via d An(x) > = nA − (x), n ≥ 1, Matrix Calculus and Related > n 1 <> dx Interpolation Hints. Mathematics 2021, A (0) = a , a 6= 0, a 2 IR, n ≥ 0, 9, 964. https://doi.org/ > n n 0 n > 10.3390/math9090964 :> A0(x) = 1, Academic Editor: Clemente Cesarano or ¥ n xt t A(t)e = ∑ An(x) , Received: 13 March 2021 n=0 n! Accepted: 23 April 2021 ¥ tk Published: 25 April 2021 where A(t) = ∑ ak , a0 6= 0, ak 2 IR, k ≥ 0. -
Explicit Inverse of a Tridiagonal (P, R)–Toeplitz Matrix
Explicit inverse of a tridiagonal (p; r){Toeplitz matrix A.M. Encinas, M.J. Jim´enez Departament de Matemtiques Universitat Politcnica de Catalunya Abstract Tridiagonal matrices appears in many contexts in pure and applied mathematics, so the study of the inverse of these matrices becomes of specific interest. In recent years the invertibility of nonsingular tridiagonal matrices has been quite investigated in different fields, not only from the theoretical point of view (either in the framework of linear algebra or in the ambit of numerical analysis), but also due to applications, for instance in the study of sound propagation problems or certain quantum oscillators. However, explicit inverses are known only in a few cases, in particular when the tridiagonal matrix has constant diagonals or the coefficients of these diagonals are subjected to some restrictions like the tridiagonal p{Toeplitz matrices [7], such that their three diagonals are formed by p{periodic sequences. The recent formulae for the inversion of tridiagonal p{Toeplitz matrices are based, more o less directly, on the solution of second order linear difference equations, although most of them use a cumbersome formulation, that in fact don not take into account the periodicity of the coefficients. This contribution presents the explicit inverse of a tridiagonal matrix (p; r){Toeplitz, which diagonal coefficients are in a more general class of sequences than periodic ones, that we have called quasi{periodic sequences. A tridiagonal matrix A = (aij) of order n + 2 is called (p; r){Toeplitz if there exists m 2 N0 such that n + 2 = mp and ai+p;j+p = raij; i; j = 0;:::; (m − 1)p: Equivalently, A is a (p; r){Toeplitz matrix iff k ai+kp;j+kp = r aij; i; j = 0; : : : ; p; k = 0; : : : ; m − 1: We have developed a technique that reduces any linear second order difference equation with periodic or quasi-periodic coefficients to a difference equation of the same kind but with constant coefficients [3]. -
Toeplitz and Toeplitz-Block-Toeplitz Matrices and Their Correlation with Syzygies of Polynomials
TOEPLITZ AND TOEPLITZ-BLOCK-TOEPLITZ MATRICES AND THEIR CORRELATION WITH SYZYGIES OF POLYNOMIALS HOUSSAM KHALIL∗, BERNARD MOURRAIN† , AND MICHELLE SCHATZMAN‡ Abstract. In this paper, we re-investigate the resolution of Toeplitz systems T u = g, from a new point of view, by correlating the solution of such problems with syzygies of polynomials or moving lines. We show an explicit connection between the generators of a Toeplitz matrix and the generators of the corresponding module of syzygies. We show that this module is generated by two elements of degree n and the solution of T u = g can be reinterpreted as the remainder of an explicit vector depending on g, by these two generators. This approach extends naturally to multivariate problems and we describe for Toeplitz-block-Toeplitz matrices, the structure of the corresponding generators. Key words. Toeplitz matrix, rational interpolation, syzygie 1. Introduction. Structured matrices appear in various domains, such as scientific computing, signal processing, . They usually express, in a linearize way, a problem which depends on less pa- rameters than the number of entries of the corresponding matrix. An important area of research is devoted to the development of methods for the treatment of such matrices, which depend on the actual parameters involved in these matrices. Among well-known structured matrices, Toeplitz and Hankel structures have been intensively studied [5, 6]. Nearly optimal algorithms are known for the multiplication or the resolution of linear systems, for such structure. Namely, if A is a Toeplitz matrix of size n, multiplying it by a vector or solving a linear system with A requires O˜(n) arithmetic operations (where O˜(n) = O(n logc(n)) for some c > 0) [2, 12]. -
A Note on Multilevel Toeplitz Matrices
Spec. Matrices 2019; 7:114–126 Research Article Open Access Lei Cao and Selcuk Koyuncu* A note on multilevel Toeplitz matrices https://doi.org/110.1515/spma-2019-0011 Received August 7, 2019; accepted September 12, 2019 Abstract: Chien, Liu, Nakazato and Tam proved that all n × n classical Toeplitz matrices (one-level Toeplitz matrices) are unitarily similar to complex symmetric matrices via two types of unitary matrices and the type of the unitary matrices only depends on the parity of n. In this paper we extend their result to multilevel Toeplitz matrices that any multilevel Toeplitz matrix is unitarily similar to a complex symmetric matrix. We provide a method to construct the unitary matrices that uniformly turn any multilevel Toeplitz matrix to a complex symmetric matrix by taking tensor products of these two types of unitary matrices for one-level Toeplitz matrices according to the parity of each level of the multilevel Toeplitz matrices. In addition, we introduce a class of complex symmetric matrices that are unitarily similar to some p-level Toeplitz matrices. Keywords: Multilevel Toeplitz matrix; Unitary similarity; Complex symmetric matrices 1 Introduction Although every complex square matrix is similar to a complex symmetric matrix (see Theorem 4.4.24, [5]), it is known that not every n × n matrix is unitarily similar to a complex symmetric matrix when n ≥ 3 (See [4]). Some characterizations of matrices unitarily equivalent to a complex symmetric matrix (UECSM) were given by [1] and [3]. Very recently, a constructive proof that every Toeplitz matrix is unitarily similar to a complex symmetric matrix was given in [2] in which the unitary matrices turning all n × n Toeplitz matrices to complex symmetric matrices was given explicitly. -
Totally Positive Toeplitz Matrices and Quantum Cohomology of Partial Flag Varieties
JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY Volume 16, Number 2, Pages 363{392 S 0894-0347(02)00412-5 Article electronically published on November 29, 2002 TOTALLY POSITIVE TOEPLITZ MATRICES AND QUANTUM COHOMOLOGY OF PARTIAL FLAG VARIETIES KONSTANZE RIETSCH 1. Introduction A matrix is called totally nonnegative if all of its minors are nonnegative. Totally nonnegative infinite Toeplitz matrices were studied first in the 1950's. They are characterized in the following theorem conjectured by Schoenberg and proved by Edrei. Theorem 1.1 ([10]). The Toeplitz matrix ∞×1 1 a1 1 0 1 a2 a1 1 B . .. C B . a2 a1 . C B C A = B .. .. .. C B ad . C B C B .. .. C Bad+1 . a1 1 C B C B . C B . .. .. a a .. C B 2 1 C B . C B .. .. .. .. ..C B C is totally nonnegative@ precisely if its generating function is of theA form, 2 (1 + βit) 1+a1t + a2t + =exp(tα) ; ··· (1 γit) i Y2N − where α R 0 and β1 β2 0,γ1 γ2 0 with βi + γi < . 2 ≥ ≥ ≥···≥ ≥ ≥···≥ 1 This beautiful result has been reproved many times; see [32]P for anP overview. It may be thought of as giving a parameterization of the totally nonnegative Toeplitz matrices by ~ N N ~ (α;(βi)i; (~γi)i) R 0 R 0 R 0 i(βi +~γi) < ; f 2 ≥ × ≥ × ≥ j 1g i X2N where β~i = βi βi+1 andγ ~i = γi γi+1. − − Received by the editors December 10, 2001 and, in revised form, September 14, 2002. 2000 Mathematics Subject Classification. Primary 20G20, 15A48, 14N35, 14N15.