Abstract
We consider a Sinai billiard where the usual hard disk scatterer is replaced by a repulsive potential with V(r)λrα close to the origin. Using periodic orbit theory and numerical evidence we show that its spectral statistics tends to Poisson statistics for large energies when α<2 and to Wigner-Dyson statistics when α>2, while for α=2 it is independent of energy, but depends on λ. We apply the approach of Altshuler and Levitov [Phys. Rep. 288, 487 (1997)] to show that the transition in the spectral statistics is accompanied by a dynamical localization-delocalization transition. This behavior is reminiscent of a metal-insulator transition in disordered electronic systems.
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