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Asymptotics of instability zones of the Hill operator with a two term potential

Mathematical Physics 2016-09-07 v1 Functional Analysis math.MP

Abstract

Let γn\gamma_n denote the length of the nn-th zone of instability of the Hill operator Ly=y[4tαcos2x+2α2cos4x]y,Ly= -y^{\prime \prime} - [4t\alpha \cos2x + 2 \alpha^2 \cos 4x ] y, where α0,\alpha \neq 0, and either both α,t\alpha, t are real, or both are pure imaginary numbers. For even nn we prove: if t,nt, n are fixed, then, for α0, \alpha \to 0, γn=8αn2n[(n1)!]2k=1n/2(t2(2k1)2)(1+O(α)), \gamma_n = | \frac{8\alpha^n}{2^n [(n-1)!]^2} \prod_{k=1}^{n/2} (t^2 - (2k-1)^2) | (1 + O(\alpha)), and if α,t \alpha, t are fixed, then, for n, n \to \infty, γn=8α/2n[24...(n2)]2cos(π2t)[1+O(lognn)]. \gamma_n = \frac{8 |\alpha/2|^n}{[2 \cdot 4 ... (n-2)]^2} | \cos (\frac{\pi}{2} t) | [ 1 + O (\frac{\log n}{n}) ]. Similar formulae (see Theorems \ref{thm2} and \ref{thm4}) hold for odd n.n. The asymptotics for α0\alpha \to 0 imply interesting identities for squares of integers.

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Cite

@article{arxiv.math-ph/0509034,
  title  = {Asymptotics of instability zones of the Hill operator with a two term potential},
  author = {Plamen Djakov and Boris Mityagin},
  journal= {arXiv preprint arXiv:math-ph/0509034},
  year   = {2016}
}

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39 pages