Distribution of zeros of discrete and continuous polynomials from their recurrence relation

The hypergeometric polynomials in a continous or a discrete variable, whose canonical forms are the so-called classical orthogonal polynomial systems, are ob jects which naturally appear in a broad range of physical and mathematical elds from quantum mechanics, the theory of vibrating strings and th...

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Bibliographic Details
Authors: Álvarez Nodarse, Renato, Sánchez Dehesa, Jesús
Format: article
Status:Published version
Publication Date:2002
Country:España
Institution:Universidad de Sevilla (US)
Repository:idUS. Depósito de Investigación de la Universidad de Sevilla
OAI Identifier:oai:idus.us.es:11441/41700
Online Access:http://hdl.handle.net/11441/41700
https://doi.org/10.1016/S0096-3003(01)00071-6
Access Level:Open access
Keyword:Orthogonal polynomials
Three-term recurrence relation
Distribution of zeros
Moments of zeros
Spectral asymptotics
Description
Summary:The hypergeometric polynomials in a continous or a discrete variable, whose canonical forms are the so-called classical orthogonal polynomial systems, are ob jects which naturally appear in a broad range of physical and mathematical elds from quantum mechanics, the theory of vibrating strings and the theory of group representations to numerical analysis and the theory of Sturm-Liouville di erential and di erence equations. Often, they are encountered in the form of a three term recurrence relation (TTRR) which connects a polynomial of a given order with the polynomial of the contiguous orders. This relation can be directly found, in particular, by use of Lanczos-type methods, tight-binding models or the application of the conventional discretisation procedures to a given di erential operator. Here the distribution of zeros and its asymptotic limit, characterized by means of its moments around the origin, are found for the continuous classical (Hermite, Laguerre, Jacobi, Bessel) polynomials and for the discrete classical (Charlier, Meixner, Kravchuk, Hahn) polynomials by means of a general procedure which (i) only requires the three-term recurrence relation and (ii) avoids the often high-brow subleties of the potential theoretic considerations used in some recent approaches. The moments are given in an explicit manner which, at times, allows us to recognize the analytical form of the corresponding distribution.