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Concentration of the eigenfunctions of Schrödinger operators B. S. Mityagin |
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Abstract: We consider a Schrödinger operator $$\lim_{x \to \infty} \frac{Q(tx)}{Q(x)} = t^{\beta}, \quad \beta \geq 2.$$ Rescale measures, or their densities, on $$\varphi_k(x) = x_k \psi_k^2(x_k x).$$ The behavior of measures For any $$ \lim_{k \to \infty} \int_{-\infty}^{\infty}f(x) \varphi_k(x) \, dx = c(\beta) \int_{-1}^1 f(x) \frac{ dx}{(1 - |x|^{\beta})^{1/2}} $$ where $c(\beta) = \frac{\Gamma( \frac{1}{2} + \frac{1}{\beta})}{2 \pi^{1/2} \Gamma(1 + \frac{1}{\beta})}$. Such statements, in the context of the theory of orthogonal polynomials, are well known (Rakhmanov, Mhaskar–Saff, Lubinsky). In the algebraic case, i.e., when The talks is based on our joint work with Petr Siegl (Queen's University Belfast, UK) and Joseph Viola (University of Nantes, France) [1], [2]. Language: English References |
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