Quantum Mechanics of a Rotating Billiard

preprint2014arXivOpen access

Abstract

Integrability of a square billiard is spontaneously broken as it rotates about one of its corners. The system becomes quasi-integrable where the invariant tori are broken with respect to a certain parameter, λ=2E/ω2λ= 2E/ω^{2} where E is the energy of the particle inside the billiard and ωω is the angular frequency of rotation of billiard. We study the system classically and quantum mechanically in view of obtaining a correspondence in the two descriptions. Classical phase space in Poincaré surface of section shows transition from regular to chaotic motion as the parameter λλ is decreased. In the Quantum counterpart, the spectral statistics shows a transition from Poisson to Wigner distribution as the system turns chaotic with decrease in λλ. The wavefunction statistics however show breakdown of time-reversal symmetry as λλ decreases.

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