2016
DOI: 10.1353/ajm.2016.0048
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Nodal intersections for random eigenfunctions on the torus

Abstract: We investigate the number of nodal intersections of random Gaussian Laplace eigenfunctions on the standard two-dimensional flat torus ("arithmetic random waves") with a fixed smooth reference curve with nonvanishing curvature. The expected intersection number is universally proportional to the length of the reference curve, times the wavenumber, independent of the geometry.Our main result prescribes the asymptotic behaviour of the nodal intersections variance for smooth curves in the high energy limit; remarka… Show more

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Cited by 37 publications
(69 citation statements)
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“…A computation shows that when Σ is a sphere or a hemisphere, the lower bound in (1.15) is achieved, hence the leading term in (1.14) vanishes: in this case the variance is of lower order than m/N (see section 7 for details). As in the problem of nodal intersections against a curve on T 2 [36], the theoretical maximum of the variance leading term is achieved in the case of intersection with a 3 Lattice points on circles equidistribute [19,20] for a density one sequence of energies. To the other extreme, Cilleruelo proved that there exist sequences s.t.…”
Section: Statement Of Main Resultsmentioning
confidence: 99%
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“…A computation shows that when Σ is a sphere or a hemisphere, the lower bound in (1.15) is achieved, hence the leading term in (1.14) vanishes: in this case the variance is of lower order than m/N (see section 7 for details). As in the problem of nodal intersections against a curve on T 2 [36], the theoretical maximum of the variance leading term is achieved in the case of intersection with a 3 Lattice points on circles equidistribute [19,20] for a density one sequence of energies. To the other extreme, Cilleruelo proved that there exist sequences s.t.…”
Section: Statement Of Main Resultsmentioning
confidence: 99%
“…manifold of identically zero curvature (straight lines in dimension 2, planes in dimension 3). As the case of Σ contained in a plane is excluded by the assumptions of Theorem 1.3, the upper bound of A 2 · π 2 /30 for the leading coefficient in (1.14) is a supremum rather than a maximum, as in [36] (see section 7).…”
Section: Statement Of Main Resultsmentioning
confidence: 99%
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