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      Scaling of Harmonic Oscillator Eigenfunctions and Their Nodal Sets Around the Caustic

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          Abstract

          In previous work we proved that the density of zeros of random eigenfunctions of the isotropic Harmonic Oscillator have different orders in the Planck constant h in the allowed and forbidden regions: In the allowed region the density is of order h^{-1} while it is h^{-1/2} in the forbidden region. In this article we study the density in the transition region around the caustic between the allowed and forbidden regions. Our main result is that the density is of order h^{-2/3} in an h^{2/3}-tube around the caustic. This tube radius is the 'critical radius'. For tubes of larger radius h^{alpha} with 0 < alpha < 2 we obtain density results which interpolate between this critical radius result and our prior ones in the allowed and forbidden region. We also show that the Hausdorff (d-2)-dimensional measure of the intersection of the nodal set with the caustic is of order h^{-2/3}. The asymptotics involve a fine study of the Airy scaling asymptotics of the eigenspace projections kernel near the caustic.

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          Theory of reproducing kernels

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            Level-Spacing Distributions and the Airy Kernel

            Scaling level-spacing distribution functions in the ``bulk of the spectrum'' in random matrix models of \(N\times N\) hermitian matrices and then going to the limit \(N\to\infty\), leads to the Fredholm determinant of the sine kernel \(\sin\pi(x-y)/\pi (x-y)\). Similarly a scaling limit at the ``edge of the spectrum'' leads to the Airy kernel \([{\rm Ai}(x) {\rm Ai}'(y) -{\rm Ai}'(x) {\rm Ai}(y)]/(x-y)\). In this paper we derive analogues for this Airy kernel of the following properties of the sine kernel: the completely integrable system of P.D.E.'s found by Jimbo, Miwa, M{\^o}ri and Sato; the expression, in the case of a single interval, of the Fredholm determinant in terms of a Painlev{\'e} transcendent; the existence of a commuting differential operator; and the fact that this operator can be used in the derivation of asymptotics, for general \(n\), of the probability that an interval contains precisely \(n\) eigenvalues.
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              $L^p$ eigenfunction bounds for the Hermite operator

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                Author and article information

                Journal
                2016-02-22
                2016-02-26
                Article
                1602.06848
                ac5e8a72-e516-4634-9f56-5362b54d054c

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                v2. Fixed several typos and corrected statement of Thm 1.6
                math-ph math.MP math.PR math.SP

                Mathematical physics,Functional analysis,Mathematical & Computational physics,Probability

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