Introduction to Orthogonal Polynomials: Definition and basic properties

Similar documents
Legendre s Equation. PHYS Southern Illinois University. October 18, 2016

Orthogonal Polynomials and Gaussian Quadrature

APPENDIX B GRAM-SCHMIDT PROCEDURE OF ORTHOGONALIZATION. Let V be a finite dimensional inner product space spanned by basis vector functions

i x i y i

Approximation theory

Orthogonal polynomials

Curve Fitting and Approximation

SPECTRAL METHODS: ORTHOGONAL POLYNOMIALS

Scientific Computing

ORTHOGONAL POLYNOMIALS

Power Series Solutions to the Legendre Equation

Advanced Computational Fluid Dynamics AA215A Lecture 2 Approximation Theory. Antony Jameson

Power Series Solutions to the Legendre Equation

8.2 Discrete Least Squares Approximation

Chapter 1 Divide and Conquer Algorithm Theory WS 2016/17 Fabian Kuhn

Vectors in Function Spaces

Chapter 1 Divide and Conquer Polynomial Multiplication Algorithm Theory WS 2015/16 Fabian Kuhn

ORTHOGONAL POLYNOMIALS FOR THE OSCILLATORY-GEGENBAUER WEIGHT. Gradimir V. Milovanović, Aleksandar S. Cvetković, and Zvezdan M.

MATH 312 Section 6.2: Series Solutions about Singular Points

Orthogonal polynomials

Interpolation and Cubature at Geronimus Nodes Generated by Different Geronimus Polynomials

5.1 Learning using Polynomial Threshold Functions

LEGENDRE POLYNOMIALS AND APPLICATIONS. We construct Legendre polynomials and apply them to solve Dirichlet problems in spherical coordinates.

PUTNAM TRAINING POLYNOMIALS. Exercises 1. Find a polynomial with integral coefficients whose zeros include

Best approximation in the 2-norm

Program : M.A./M.Sc. (Mathematics) M.A./M.Sc. (Final) Paper Code:MT-08 Numerical Analysis Section A (Very Short Answers Questions)

MAT Linear Algebra Collection of sample exams

Linear Independence. Stephen Boyd. EE103 Stanford University. October 9, 2017

ON LINEAR COMBINATIONS OF

Quadratures and integral transforms arising from generating functions

Numerical Linear Algebra Chap. 2: Least Squares Problems

Mathematical Methods wk 1: Vectors

Mathematical Methods wk 1: Vectors

Inner products. Theorem (basic properties): Given vectors u, v, w in an inner product space V, and a scalar k, the following properties hold:

Hankel determinants, continued fractions, orthgonal polynomials, and hypergeometric series

SYMMETRY AND SPECIALIZABILITY IN THE CONTINUED FRACTION EXPANSIONS OF SOME INFINITE PRODUCTS

Mathematical Induction Again

Chebyshev approximation

OPSF, Random Matrices and Riemann-Hilbert problems

Mathematical Induction Again

Bivariate Lagrange interpolation at the Padua points: The generating curve approach

Introduction to orthogonal polynomials. Michael Anshelevich

3. Coding theory 3.1. Basic concepts

Moreover this binary operation satisfies the following properties

Lecture 4.6: Some special orthogonal functions

d 1 µ 2 Θ = 0. (4.1) consider first the case of m = 0 where there is no azimuthal dependence on the angle φ.

Lecture 6, Sci. Comp. for DPhil Students

Two special equations: Bessel s and Legendre s equations. p Fourier-Bessel and Fourier-Legendre series. p

Inverses. Stephen Boyd. EE103 Stanford University. October 28, 2017

Spectral Theory of Orthogonal Polynomials

Chapter 4. Series Solutions. 4.1 Introduction to Power Series

Nonlinear Integral Equation Formulation of Orthogonal Polynomials

An Analysis of Five Numerical Methods for Approximating Certain Hypergeometric Functions in Domains within their Radii of Convergence

Linear Algebra. and

1. Algebra 1.5. Polynomial Rings

BIVARIATE LAGRANGE INTERPOLATION AT THE PADUA POINTS: THE IDEAL THEORY APPROACH

18.S34 (FALL 2007) PROBLEMS ON ROOTS OF POLYNOMIALS

ON THE CHEBYSHEV POLYNOMIALS. Contents. 2. A Result on Linear Functionals on P n 4 Acknowledgments 7 References 7

INTERPOLATION. and y i = cos x i, i = 0, 1, 2 This gives us the three points. Now find a quadratic polynomial. p(x) = a 0 + a 1 x + a 2 x 2.

Class notes: Approximation

Solutions: Problem Set 3 Math 201B, Winter 2007

An idea how to solve some of the problems. diverges the same must hold for the original series. T 1 p T 1 p + 1 p 1 = 1. dt = lim

On Orthogonal Polynomials in Several Variables

Jumping Sequences. Steve Butler 1. (joint work with Ron Graham and Nan Zang) University of California Los Angelese

Further Mathematical Methods (Linear Algebra) 2002

Chapter 1: Systems of linear equations and matrices. Section 1.1: Introduction to systems of linear equations

This ODE arises in many physical systems that we shall investigate. + ( + 1)u = 0. (λ + s)x λ + s + ( + 1) a λ. (s + 1)(s + 2) a 0

BMT 2016 Orthogonal Polynomials 12 March Welcome to the power round! This year s topic is the theory of orthogonal polynomials.

1/30: Polynomials over Z/n.

INTEGER POWERS OF ANTI-BIDIAGONAL HANKEL MATRICES

Applied Linear Algebra in Geoscience Using MATLAB

Mathematical Induction Assignments

MATRIX INTEGRALS AND MAP ENUMERATION 2

General Power Series

Index. for Ɣ(a, z), 39. convergent asymptotic representation, 46 converging factor, 40 exponentially improved, 39

Measures, orthogonal polynomials, and continued fractions. Michael Anshelevich

Special classes of polynomials

Measures, orthogonal polynomials, and continued fractions. Michael Anshelevich

ENCYCLOPEDIA OF MATHEMATICS AND ITS APPLICATIONS. Special Functions GEORGE E. ANDREWS RICHARD ASKEY RANJAN ROY CAMBRIDGE UNIVERSITY PRESS

Recurrence Relations and Fast Algorithms

On Gauss-type quadrature formulas with prescribed nodes anywhere on the real line

Multiple Orthogonal Polynomials

Background and Definitions...2. Legendre s Equation, Functions and Polynomials...4 Legendre s Associated Equation and Functions...

Mathematical Olympiad Training Polynomials

Polynomial approximation via de la Vallée Poussin means

Exercise 11. Isao Sasano

GAUSS-LAGUERRE AND GAUSS-HERMITE QUADRATURE ON 64, 96 AND 128 NODES

Approximation Theory

A trigonometric orthogonality with respect to a nonnegative Borel measure

Math 255 Honors: Gram-Schmidt Orthogonalization on the Space of Polynomials

INNER PRODUCT SPACE. Definition 1

Math Assignment 11

Zeros of Jacobi Polynomials and associated. Inequalities

14 Fourier analysis. Read: Boas Ch. 7.

Basic Algebra. Final Version, August, 2006 For Publication by Birkhäuser Boston Along with a Companion Volume Advanced Algebra In the Series

MATH 220: INNER PRODUCT SPACES, SYMMETRIC OPERATORS, ORTHOGONALITY

swapneel/207

The Generating Functions for Pochhammer

(Inv) Computing Invariant Factors Math 683L (Summer 2003)

Solving Linear Systems Using Gaussian Elimination. How can we solve

Transcription:

Introduction to Orthogonal Polynomials: Definition and basic properties Prof. Dr. Mama Foupouagnigni African Institute for Mathematical Sciences, Limbe, Cameroon and Department of Mathematics, Higher Teachers Training College University of Yaounde I, Cameroon Email:mfoupouagnigni@aims-cameroon.org AIMS-Volkswagen Stiftung Workshop on Introduction to Orthogonal Polynomials and Applications Hotel Prince de Galles, Douala, Cameroon, October 5-12, 2018

Table of Contents 1 Why should we study orthogonal polynomials? 2 An example of a system of orthogonal polynomials 3 Construction of a system of orthogonal polynomials 4 Definition of orthogonal polynomials 5 Basis properties of orthogonal polynomials 6 Tutorials: Solving assignments

Main objectives 1 Give an example of a system of orthogonal polynomials 2 Provide a method for constructing a system orthogonal Polynomials 3 Define the notion of orthogonal polynomials; 4 Provide (with some illustrations on the proof) some basic properties such as: the uniqueness of a family of orthogonal polynomials; the matrix representation; the three-term recurrence relation, the Christoffel-Darboux formula and some of its consequences such as the interlacing properties of the zeros. 5 Finally we discuss and solve, as a short tutorial, some assignments given within the first talk which are mainly proof of some results provided earlier.

Why should we study orthogonal polynomials? Orthogonal polynomials are to be seen as a sequence of polynomials (p n ) n with deg(p n ) = n with orthogonality property. They are very useful in practice in various domains of mathematics, physics, engineering and so on because of the many properties and relations they satisfy: 1 Orthogonality (all of them) 2 Three term recurrence relation (all of them) 3 Darboux-Christoffel formula (all of them) 4 Matrix representation (all of them); 5 Gauss quadrature (all of them): used for approximation of integrals; 6 second-order holonomic differential, difference or q-difference equation (classical ones); 7 Fourth-order holonomic differential, difference or q-difference equations (Laguerre-Hahn class); 8 Rodrigues formula (classical ones); 9 Partial differential, difference or q-difference equations (OP of several variables); 10 Expansion of continuous function with integrable square derivable in terms of Fourier series of OP (classical OP); 11....

AMS subject classification for Orthogonal Polynomials

The Chebyshev polynomials of the first kind Chebyshev polynomials of the first kind are defined by T n (x) = cos(nθ), x = cos θ, 0 < θ < π (1) {w0} and fulfil the following properties: 1 T n is a polynomial of degree n in x: This can be seen from the recurrence relation T n+1 (x) + T n 1 (x) = 2xT n (x), n 1, T 0 (x) = 1, T 1 (x) = x; (2) {w1} 2 (T n ) n satisfies the orthogonality relation π 1 dx cos(nθ) cos(mθ)dθ = k n δ n,m = T n (x) T m (x) (3) 0 1 1 x 2 (with k 0 = π, k n = π 2, n 1), obtained using the change of variable {w2} x = cos θ, 0 < θ < π and the linearization formula 2 cos nθ cos mθ = cos(n + m)θ + cos(n m)θ. 3 Monic Chebyshev polynomial of degree n is the polynomial deviating less { from zero on [ 1, 1] among monic polynomials } of degree n: min max q n(x), q n R[x], q n (x) = x n +... 1 x 1 4 Second-order holonomic differential equation: = max 1 x 1 21 n T n (x) = 2 1 n. (4) {w3} (1 x 2 ) T n (x) x T n(x) + n 2 T n (x) = 0, n 0. (5) {w4}

First 10 Chebyshev I Polynomials From the three-term recurrence relation, one can generate any T n : T n+1 (x) = 2xT n (x) T n 1 (x), n 1, T 0 (x) = 1, T 1 (x) = x; T 2 (x) = 2 x 2 1, T 3 (x) = 4 x 3 3 x, T 4 (x) = 8 x 4 8 x 2 + 1, T 5 (x) = 16 x 5 20 x 3 + 5 x, (6) {w5} T 6 (x) = 32 x 6 48 x 4 + 18 x 2 1, T 7 (x) = 64 x 7 112 x 5 + 56 x 3 7 x, T 8 (x) = 128 x 8 256 x 6 + 160 x 4 32 x 2 + 1, T 9 (x) = 256 x 9 576 x 7 + 432 x 5 120 x 3 + 9 x. The zeros x n,k of T n ranked in increasing order are: ( ) (2(n k) + 1 x n,k = cos π, k = 1..n. 2n (7) {w6}

Graphic of the first 10 Chebyshev I Polynomials

Orthogonality relations for the Chebyshev I Polynomials Summing up, we have seen that the Chebyshev polynomials T n satisfy: and the orthogonality condition: deg(t n ) = n 0; 1 dx 1 T n (x) T m (x) = 0, n m, dx T n (x) T n (x) 1 x 2 1 x 2 1 1 0, n 0. The polynomial sequence (T n ) n is said to be orthogonal with respect to the weight function ρ(x) = 1 1 x 2 defined over the interval ] 1, 1[. It is an orthogonal polynomial sequence. Assignment 1: Establish relations (1)-(7).

Construction of a system of orthogonal polynomials:part 1 Let us consider a scalar product (, ) defined on R[x] R[x] where R[x] is the ring of polynomials with real variable. As scalar product, it fulfills the following properties: (p, p) 0, p R[x], and (p, p) = 0 = p = 0, (8) {w7} (p, q) = (q, p), p, q R[x], (9) (λ p, q) = λ (p, q), λ R, p, q R[x], (10) (p + q, r) = (p, r) + (q, r), p, q, r R[x]. (11) As examples of scalar products on R[x] with connections to known systems of orthogonal polynomials, we mention: (p, q) = 1 1 connected to Chebyshev polynomials; (p, q) = dx p(x) q(x), (12) {w8} 1 x 2 N w k p(k) q(k), N N { }, (13) {w9} k=0 leading to orthogonal polynomials of a discrete variable.

Construction of a system of orthogonal polynomials: Part 2 Theorem (Gram-Schmidt orthogonalisation process) The polynomial systems (q n ) n and (p n ) n defined recurrently by the relations n 1 q 0 = 1, q n = x n satisfy the relations k=0 (q k, x n ) (q k, q k ) q k, n 1, p k = deg(q n ) = deg(p n ) = n, n 0, (q n, q m ) = 0, n m, (q n, q n ), 0 n n, (p n, p m ) = 0, n m, (p n, p n ) = 1, n n. q k, k 0, (14) {w10 (qk, q k ) The proof is done by induction on n: Assignment 2. The polynomial systems (q n ) n and (p n ) n are said to be orthogonal with respect to the scalar product (, ). They represent the same orthogonal polynomial system with different normalisation: (q n ) n is monic (to say the coefficient of the leading monomial is equal to 1) while (p n ) n is orthonormal ( (p n, p n ) = 1).

Definition of orthogonal polynomials: Part 1 Orthogonality with respect to a scalar product A system (p n ) n of polynomials is said to be orthogonal with respect to the scalar product (, ) if it satisfies the following 2 conditions deg(p n ) = n, n 0, (15) {w11 (p n, p m ) = 0, n m, (p n, p n ) 0, n n. (16) {w12 When scalar product is defined by a Stieltjes integral When the scalar product (, ) is defined by a Stieltjes integral (p, q) = b a p(x) q(x) dα(x), (17) {w13 where α is an appropriate real-valued function, then (16) reads b p n (x) p m (x) dα(x) = 0, n m, b a a p n (x) p n (x) dα(x) 0, n 0. (18) {w14

Definition of the Stieltjes integral

Definition of orthogonal polynomials: Part 2 When scalar product is defined by the Riemann When the scalar product is defined by a Stieltjes integral (17) with dα(x) = w(x) dx where w is an appropriate function, then (16) reads b a p n (x) p m (x) w(x) dx = 0, n m, b a p n (x) p n (x) w(x) dx 0, n 0. (p n ) n is said to be orthogonal with respect to the weight function w. Because of the form of the orthogonality relation, the variable here is continuous. When scalar product is defined by a special Stieltjes function When the scalar product is defined by a Stieltjes integral (17) where w is an appropriate step function on N or on {0, 1,..., N}, then (14) reads N (p, q) = w(k) p(k) q(k), N N { }. (19) {w17 k=0 (p n ) n is said to be orthogonal with respect to the discrete weight function w. Because of the form of the orthogonality relation, the variable is discrete. Assignment 3: Find the first five monic polynomials orthogonal with respect to the weight w(x) = 1 defined on the interval [ 1, 1].

Basis properties of orthogonal polynomials: Part 1 In this section, we will assume that the polynomial sequence (p n ) n satisfies deg(p n ) = n, n 0 and the orthogonality relation (18) which we recall here: b a p n (x) p m (x) dα(x) = 0, n m, b a p n (x) p n (x) dα(x) 0, n 0. Then we have the following properties: Lemma (Equivalent orthogonality relation) The orthogonality relation (18) is equivalent to b a p n (x) x m dα(x) = 0, n 1, 0 m n 1, b a p n (x) x n dα(x) 0, n 0. The previous equation implies that p n is orthogonal to any polynomial of degree less than n. (20) {w18

Basis properties of orthogonal polynomials Theorem (Uniqueness of an orthogonal polynomial system) To a scalar product (, ) on R[x] is associated a unique up to a multiplicative factor system of orthogonal polynomials: If (p n ) n and (q n ) n are both orthogonal with respect to a scalar product (, ), then there exists a sequence (α n ) n with α n 0, n 0 such that p n = α n q n, n 0. Proof s Indication: For a fixed n 1, we expand p n in terms of the (q k ) k and obtain n p n = c k,n q k, with Hence k=0 c k,n = (p n, q k ) = 0, for 0 k n 1. (q k, q k ) p n = (p n, q n ) (q n, q n ) q n.

Basis properties of orthogonal polynomials Theorem (Matrix representation of a system of orthogonal polynomials) Denoting by µ n the moment with respect to the Stieltjes measure dα µ n = b and n the Hankel determinant defined by a x n dα(x), n 0, n = det(µ k+j ) 0 k,j n 0, n 0, then the monic polynomial sequence orthogonal with respect to the Stieltjes measure dα is given by p n = 1 n 1 µ 0 µ 1 µ n 1 µ n µ 1 µ 1 µ n 1 µ n+1...... (21) {w19 µ n 1 µ n µ 2n 2 µ 2n 1 1 x x n 1 x n. Assignment 4: Proof of the theorem. Proof s indication: Prove that (p n, x k ) = 0, 0 k n 1, (p n, x n ) 0.

Basis properties of orthogonal polynomials Theorem (Three-term recurrence relation) Any polynomial sequence (p n ), orthogonal with respect to a scalar product (, ) defined by the Stieltjes integral satisfies the following relation called three-term recurrence relation x p n (x) = with a n a n+1 p n+1 + ( bn a n b n+1 a n+1 ) p n + a n 1 a n d 2 n d 2 n 1 p n 1, p 1 = 0, p 0 = 1, (22) {w20 p n = a n x n + b n x n 1 + low factors, (23) {w21 and d 2 n = (p n, p n ).. Assignment 5: Prove this theorem. Remark When (p n ) is monic (ie. a n = 1) or orthonormal (ie. d n = 1), then Equation (refw20) can be written respectively in the following forms: p n+1 = (x β n ) p n γ n p n 1, p 1 = 0, p 0 = 1, x p n = α n+1 p n+1 + β n p n + α n p n 1, p 1 = 0, p 0 = 1.

Basis properties of orthogonal polynomials: TTRR Proof s indication For fixed n 0, we expand x p n in the basis {p 0, p 1,..., p n+1 } to obtain Hence n+1 x p n = c k,n p k, k=0 c k,n = (xp n, p k ) (p k, p k ) = (p n, xp k ) = 0, 0 k < n 1. (p k, p k ) x p n = c n+1,n p n+1 + c n,n p n + c n 1,n p n 1. (24) {w22 Inserting (23) and (24) into (22) and identifying the leading coefficients of the monomials x n+1 and x n yields c n+1,n = a n a n+1, c n,n = ( bn b ) n+1. (25) {w23 a n a n+1

Basis properties of orthogonal polynomials Three-term recurrence relation Using twice (24) combined with the scalar product gives c n,n 1 dn 2 = (x p n, p n 1 ) = (p n, x p n 1 ) = c n 1,n dn 1 2 from where we deduct using (25) that c n 1,n = a n 1 a n d 2 n d 2 n 1.

Basis properties of orthogonal polynomials Theorem (Christofell-Darboux formula) Any system of orthogonal polynomials satisfying the three-term recurrence relation xp n (x) = a ( n bn p n+1 + b ) n+1 p n + a n 1 dn 2 p n 1, p 1 = 0, p 0 = 1, a n+1 a n a n+1 a n d 2 n 1 satisfies a so-called Christofell-Darboux formula given respectively in its initial form and confluent form as n k=0 p k (x)p k (y) d 2 k n k=0 p k (x)p k (x) d 2 k = a n a n+1 1 d 2 n = a n a n+1 1 d 2 n p n+1 (x) p n (y) p n+1 (y) p n (x), x y (26) {w24 x y ( p n+1 (x) p n (x) p n+1 (x) p n(x) ). (27) {w25 Assignment 6: Prove the Christoffel-Darboux formula and its confluent form

Basis properties of orthogonal polynomials Proof of the Christoffel-Darboux formula For the proof of (26), we multiply by p k (y) Equation (24) in which n is replaced by k to obtain x p k (x) p k (y) = c k+1,k p k+1 (x) p k (y) + c k,k p k (x) p k (y) + c k 1,k p k 1 (x) p k (y). Interchanging the role of x and y in the previous equation, we obtain y p k (x) p k (y) = c k+1,k p k+1 (y) p k (x) + c k,k p k (x) p k (y) + c k 1,k p k 1 (y) p k (x). Subtracting the last equation from the last but one, we obtain that p k (x) p k (y) d 2 k A k+1 (x, y) = c k+1,k d 2 k = A k+1(x, y) A k (x, y), x y (p k+1 (x) p k (y) p k+1 (y) p k (x)) taking into account the relation c k+1,k = c k,k+1. dk 2 dk+1 2 Equation (27) is obtained by taking the limit of (26) when y goes to x. = a k a k+1 1 d 2 k

Basic properties of Orthogonal Polynomials Theorem (On the zeros of orthogonal polynomials) If (p n ) n is an orthogonal polynomial system, the we have: 1 p n and p n+1 have no common zero. The same applies for P n and P n; 2 p n has n real simple zeros x n,k satisfying a < x n,k < b, 1 k n. 3 if x n,1 < x n,2 < < x n,n are the n zeros of p n, then a < x n+1,k < x n,k < x n+1,k+1, 1 k n.

Graphic of the first 10 Chebyshev I Polynomials

Tutorials: Solving assignments As tutorial, please solve assignment 1 to 6.

Thanks for your kind attention