Classical diffusion in double-delta-kicked particles
arXiv:physics/0408088 · doi:10.1103/PhysRevE.74.026210
Abstract
We investigate the classical chaotic diffusion of atoms subjected to {\em pairs} of closely spaced pulses (`kicks) from standing waves of light (the -KP). Recent experimental studies with cold atoms implied an underlying classical diffusion of type very different from the well-known paradigm of Hamiltonian chaos, the Standard Map. The kicks in each pair are separated by a small time interval , which together with the kick strength , characterizes the transport. Phase space for the -KP is partitioned into momentum `cells' partially separated by momentum-trapping regions where diffusion is slow. We present here an analytical derivation of the classical diffusion for a -KP including all important correlations which were used to analyze the experimental data. We find a new asymptotic () regime of `hindered' diffusion: while for the Standard Map the diffusion rate, for , oscillates about the uncorrelated, rate , we find analytically, that the -KP can equal, but never diffuses faster than, a random walk rate. We argue this is due to the destruction of the important classical `accelerator modes' of the Standard Map. We analyze the experimental regime , where quantum localisation lengths are affected by fractal cell boundaries. We find an approximate asymptotic diffusion rate , in correspondence to a regime in the Standard Map associated with 'golden-ratio' cantori.
14 pages, 10 figures, error in equation in appendix corrected
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- Classical and Quantum Transport in One-Dimensional Periodically Kicked Systems
- Classical and quantum anomalous diffusion in a system of 2-kicked Quantum Rotors