Irreducibility of generalized Hermite-Laguerre Polynomials III

preprint2016arXivOpen access

Abstract

For a positive integer nn and a real number αα, the generalized Laguerre polynomials are defined by \begin{align*} L^{(α)}_n(x)=\sum^n_{j=0}\frac{(n+α)(n-1+α)\cdots (j+1+α)(-x)^j}{j!(n-j)!}. \end{align*} These orthogonal polynomials are solutions to Laguerre's Differential Equation which arises in the treatment of the harmonic oscillator in quantum mechanics. Schur studied these Laguerre polynomials for its interesting algebraic properties. He obtained irreducibility results of Ln(±12)(x)L^{(\pm \frac{1}{2})}_n(x) and Ln(±12)(x2)L^{(\pm \frac{1}{2})}_n(x^2) and derived that the Hermite polynomials H2n(x)H_{2n}(x) and H2n+1(x)x\frac{H_{2n+1}(x)}{x} are irreducible for each nn. In this article, we extend Schur's result by showing that the family of Laguerre polynomials Ln(q)(x)L^{(q)}_n(x) and Ln(q)(xd)L^{(q)}_n(x^d) with q∈{±13,±23,±14,±34}q\in \{\pm \frac{1}{3}, \pm \frac{2}{3}, \pm \frac{1}{4}, \pm \frac{3}{4}\}, where dd is the denominator of qq, are irreducible for every nn except when q=14,n=2q=\frac{1}{4}, n=2 where we give the complete factorization. In fact, we derive it from a more general result.

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