Statistical properties of the localization measure of chaotic eigenstates and the spectral statistics in a mixed-type billiard
arXiv:2104.11325 · doi:10.1103/PhysRevE.100.062208
Abstract
We study the quantum localization in the chaotic eigenstates of a billiard with mixed-type phase space, after separating the regular and chaotic eigenstates, in the regime of slightly distorted circle billiard where the classical transport time in the momentum space is still large enough, although the diffusion is not normal. In quantum systems with discrete energy spectrum the Heisenberg time , where is the mean level spacing, is an important time scale.The classical transport time scale in relation to the Heisenberg time scale (their ratio is the parameter ) determines the degree of localization of the chaotic eigenstates, whose measure is based on the information entropy. We show that is linearly related to normalized inverse participation ratio. The localization of chaotic eigenstates is reflected also in the fractional power-law repulsion between the nearest energy levels in the sense that the probability density to find successive levels on a distance goes like for small , where , and corresponds to completely extended states. We show that the level repulsion exponent is empirically a rational function of , and the mean as a function of is also well approximated by a rational function. In both cases there is some scattering of the empirical data around the mean curve, which is due to the fact that actually has a distribution, typically with quite complex structure, but in the limit well described by the beta distribution. Like in other systems, goes from to when goes from to . is a function of , similar to the quantum kicked rotator and the stadium billiard.
14 pages, 10 figures, 1 table. arXiv admin note: substantial text overlap with arXiv:2104.10679
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