Periodic delta-like kicks first drive chaotic momentum diffusion, then quantum interference arrests the growth and localizes the momentum distribution.
This page describes the phenomenon using the current QPE preset and numerical modules as its primary source.
The surprise is temporal: kicks initially broaden momentum as if by diffusion, then interference among many kick histories arrests the growth. Localization occurs in momentum space.
Press Play and watch momentum space. The state starts near momentum mode n=0. Each kick multiplies psi by exp[-i k cos(theta)], producing rapid momentum spreading.
Then quantum interference takes over. The spread stops growing diffusively: <n^2> remains bounded while the classical standard-map reference continues to diffuse.
Analysis -> Kicked Rotor. The upper panel is the stroboscopic momentum carpet P(n). The lower panel compares the real 2D quantum <n^2> with a classical ensemble using the same parameters.
History. Fishman, Grempel and Prange connected the quantum kicked rotor to Anderson localization in 1982. Direct atomic observations of dynamical localization were reported by Moore et al. in 1994, followed by an explicit atom-optics delta-kicked-rotor realization with ultracold sodium in 1995.
Model boundary. X is the periodic rotor angle and Y is a harmonically confined spectator coordinate. Kicks are ideal instantaneous unitary impulses rather than finite laser pulses.
The quantum kicked rotor became a model system for quantum chaos. In 1995 Moore and collaborators realized the δ-kicked rotor with ultracold sodium atoms in a pulsed standing wave and observed dynamical localization.
| Representative platform | ultracold Na atoms in a pulsed 589 nm standing wave |
|---|---|
| Mapping basis | Na-23 kicked-rotor mapping with m_sim=0.10 |
| 1 QPE length unit | 14.4 nm |
| 1 QPE time unit | 0.749 µs |
| Energy scale E0=ħ/T0 | 0.879 neV |
| Equivalent frequency E0/h | 0.213 MHz |
| Note | One full 20.48-unit periodic X domain maps to one 589 nm/2 standing-wave period. Because the guided rotor uses m_sim=0.10, T0=m_phys L0^2/(m_sim hbar), giving about 0.749 us rather than the m_sim=1 kinetic time. |
Open Model & Constraints to see exactly what QPE computes and what is left outside the model. For current live values use Help → Current Experiment → Current Parameters.