A Method of Composition Orthogonality and New Sequences of Orthogonal Polynomials and Functions for Non-Classical Weights” [J

A Method of Composition Orthogonality and New Sequences of Orthogonal Polynomials and Functions for Non-Classical Weights” [J

A METHOD OF COMPOSITION ORTHOGONALITY AND NEW SEQUENCES OF ORTHOGONAL POLYNOMIALS AND FUNCTIONS FOR NON-CLASSICAL WEIGHTS S. YAKUBOVICH DEPARTMENT OF MATHEMATICS, FAC. SCIENCES OF UNIVERSITY OF PORTO, RUA DO CAMPO ALEGRE, 687; 4169-007 PORTO (PORTUGAL) ABSTRACT. A new method of composition orthogonality is introduced. It is applied to generate new sequences of orthogonal polynomials and functions. In particular, classical orthogonal polynomials are interpreted in the sense of composition orthogonality. Finally, new sequences of orthogonal polynomials with respect to the weight 2 ν/2 function ρ (x),ρν (x)= 2x Kν (2√x), x > 0,ν 0, where Kν (z) is the modified Bessel function or Macdon- ν ≥ ald function, are investigated. Differential properties, recurrence relations, explicit representations, generating functions and Rodrigues-type formulae are obtained. The corresponding multiple orthogonal polynomials are exhibited. 1. INTRODUCTION AND PRELIMINARY RESULTS α In studying Prudnikov’s sequence of orthogonal polynomials(see [10]) with the weight function x ρν (x), ν/2 where ρν (x)= 2x Kν (2√x), x > 0,ν 0, α > 1 and Kν (z) is the Macdonald or modified Bessel func- tion [1], Vol. II the author interpreted this≥ sequence− in terms of the Laguerre composition orthogonality, involving the differential operator θ = xDx, where D = d/dx. The main aim of this paper is to extend the method, employing classical orthogonal polynomials (Hermite, Laguerre, Jacobi) [1] to find new sequences of orthogonal polynomials with non-classical weights such as, for instance, the square of Macdonald func- tion and other hypergeometricfunctions. In fact, we will define the composition orthogonality in the follow- ing way. Definition 1. Let ω(t),ϕ(t) t [a,b], ∞ a < b ∞ be nonnegative functions, θ = tDt. Let f ,g be complex-valued functions such∈ that the− product≤ of two≤ operators f (θ)g(θ) commutes. Then f , g are compositionally orthogonal with respect to the measure ω(t)dt relatively to the function ϕ if b f (θ)g(θ) ϕ(t) ω(t)dt = 0. (1.1) a { } Z We will see in the sequel that this definition suits well with the vector space of polynomials over R, when the composition orthonormality of the sequence Pn n 0 is defined by { } ≥ arXiv:2006.11752v3 [math.CA] 4 Mar 2021 b Pn(θ)Pm(θ) ϕ(t) ω(t)dt = δn,m, (1.2) a { } Z Date: March 5, 2021. 2000 Mathematics Subject Classification. 33C10, 42C05, 44A15 . Key words and phrases. Classical orthogonal polynomials, Macdonald function, Tricomi function, generalized hypergeometric function. E-mail: [email protected]. The work was partially supported by CMUP, which is financed by national funds through FCT(Portugal), under the project with reference UIDB/00144/2020. 1 2 S. Yakubovich where δn,m, n,m N0 is the Kronecker symbol. Moreover, for some class of functions ϕ it is possible to transform the left-hand∈ side of the equality (1.2) to the usual orthogonality with respect to a new weight function. Then since the n-th power of the operator θ satisfies the Viskov-type identity [8] n n n n n θ = (xDx) = x D x , n N0, (1.3) ∈ we can get via integration by parts new properties of the sequence Pn n 0 and its relationship, for instance, with classical orthogonal polynomials. In fact, let us consider a class{ } of≥ functions ϕ representable by the modified Laplace transform of some nonnegative function ψ ∞ 1 x/t ϕ(t)= e− ψ(x)dx, t [a,b] (0,∞). (1.4) t 0 ∈ ⊂ Z Hence it is easily seen that k 1 x/t k 1 x/t k 1 x/t θ t− e− = (tDt) t− e− = x t− e− , k N0, (1.5) ∈ and therefore, differentiatingn under theo integral signn in (1.4),o we derive ∞ k 1 x/t k θ ϕ(t) = e− x ψ(x)dx, k N0. (1.6) { } t 0 ∈ Z It is indeed allowed, for instance, due to the assumed convergence of the integral ∞ x/b k e− x ψ(x)dx < ∞, k N0. (1.7) 0 ∈ Z Consequently, returning to (1.2) we write its left-hand side in the form b b ∞ x/t dxdt Pn(θ)Pm(θ) ϕ(t) ω(t)dt = e− Pn(x)Pm(x)ψ(x)ω(t) . (1.8) a { } a 0 t Z Z Z The interchange of the order of integration on the right-hand side in (1.8) is permitted by Fubini’s theorem under the imposed condition b ∞ x/t k dxdt e− x ψ(x)ω(t) < ∞, k N0, (1.9) a 0 t ∈ Z Z and, combining with (1.2), we find the equalities b ∞ Pn(θ)Pm(θ) ϕ(t) ω(t)dt = Pn(x)Pm(x)ψ(x)Ω(x)dx = δn,m, (1.10) a { } 0 Z Z where b dt Ω(x)= e x/t ω(t) , x > 0. (1.11) − t Za Thus we see that the sequence Pn n 0 is orthonormal over (0,∞) with respect to the measure Ω(x)dx. Moreover, one can consider the left-hand{ } ≥ side of the first equality in (1.10) as an inner product on the vector space of polynomials over R (a pre-Hilbert space) b p,q = p(θ)q(θ) ϕ(t) ω(t)dt, (1.12) h i a { } Z inducing the norm by the equality Composition orthogonality and new sequences of orthogonal polynomials and functions 3 ∞ 1/2 p = p, p = p2(x)ψ(x)Ω(x)dx . (1.13) || || h i 0 Z p 2. THE USE OF CLASSICAL ORTHOGONAL POLYNOMIALS 2.1. Laguerre polynomials. We begin to consider sequences of orthogonal polynomials which are compo- ν t R ν sitionally orthogonalwith respect to the measure t e− dt over + related to Laguerre polynomials Ln n 0, ν > 1. In fact, letting ω(t)= tν e t , t > 0 in (1.2), we get { } ≥ − − ∞ ν t Pn(θ)Pm(θ) ϕ(t) t e− dt = δn,m. (2.1) 0 { } Z The corresponding integral (1.11) is calculated in [1], Vol. II, and we obtain ∞ x/t t ν 1 ν/2 Ω(x)= e− − t − dt = 2x Kν 2√x ρν (x), x > 0, (2.2) 0 ≡ Z where Kν (z) is the modified Bessel function or Macdonald function [9]. The function ρν has the Mellin- Barnes integral representation in the form (cf. [10]) γ+i∞ 1 s ρν (x)= Γ(ν + s)Γ(s)x− ds , x,γ R+, ν R, (2.3) 2πi γ i∞ ∈ ∈ Z − where Γ(z) is Euler’s gamma-function[1], Vol. I. The asymptotic behavior of the modified Bessel function at infinity and near the origin [1], Vol. II gives the corresponding values for the function ρν , ν R. Precisely, we have ∈ (ν ν )/2 ρν (x)= O x −| | , x 0, ν = 0, ρ0(x)= O(logx), x 0, (2.4) → 6 → ν/2 1/4 2√x ρν (x)= O x − e− , x +∞. (2.5) → Therefore, if the condition (cf. (1.9)) ∞ k x ρν (x)ψ(x)dx < ∞, k N0 (2.6) 0 ∈ Z holds valid, we arrive at the following proposition. Proposition 1. Let ν > 1,ϕ,ψ be nonnegative functions defined on R+ which are related by the modi- fied Laplace transform (1.4−). Then under condition (2.6) the finiteness of the integral ∞ k x/M x e− ψ(x)dx < ∞, k N0 (2.7) 0 ∈ Z for some M > 0 the sequence Pn n 0 of orthogonal polynomials with respect to the measure ρν (x)ψ(x)dx { } ≥ over R+ is compositionally orthogonal in the sense of Laguerre relatively to the function ϕ, i.e. ∞ ∞ ν t Pn(θ)Pm(θ) ϕ(t) t e− dt = Pn(x)Pm(x)ρν (x)ψ(x)dx = δn,m. (2.8) 0 { } 0 Z Z Proof. Since via (2.7) the integral ∞ 1 x/t k e− x ψ(x)dx, k N0 t 0 ∈ Z converges uniformly with respect to t [1/M,M],M > 0, the consecutive differentiation under the integral sign is allowed, and we derive, recalling∈ (1.6) 4 S. Yakubovich ∞ 1 x/t Pn(θ)Pm(θ) ϕ(t) = Pn(θ)Pm(θ) e− ψ(x)dx { } t 0 Z 1 ∞ = e x/t P (x)P (x)ψ(x)dx. t − n m Z0 Then ∞ M ∞ ν t x/t ν 1 t Pn(θ)Pm(θ) ϕ(t) t e− dt = lim e− Pn(x)Pm(x)ψ(x)t − e− dxdt 0 { } M ∞ 1/M 0 Z → Z Z ∞ = Pn(x)Pm(x)ρν (x)ψ(x)dx = δn,m, Z0 where the latter equality is guaranteed by condition (2.6) and Fubini’s theorem. α ν,α Remark 1. Letting ν 0,ψ(x)= x , α > 1, we find the sequence Pn n 0 of Prudnikov’s orthogonal polynomials studied in [10≥] − { } ≥ ∞ ∞ ν,α ν,α α α ν t Pn (x)Pm (x)ρν (x)x dx = Γ(α + 1) Pn(θ)Pm(θ) t t e− dt = δn,m. (2.9) 0 0 { } Z Z 2.2. Hermite polynomials. Other interesting case is the Hermite orthogonality with respect to the measure t2 e− dt over R. Our method will work on the following even extension of the modified Laplace transform (1.4) ∞ 1 x/ t ϕ( t )= e− | |ψ(x)dx, t R 0 . (2.10) | | t 0 ∈ \{ } | | Z Hence when the Parseval identity for the Mellin transform [6] suggests the equality ∞ γ+i∞ x/t t2 dt 1 s s e− − = Γ Γ(s) x− ds, x,γ > 0.

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