Abstract
We study ultra-cold bosons out of equilibrium in a one-dimensional (1D) setting and probe the breaking of integrability and the resulting relaxation at the onset of the crossover from one to three dimensions. In a quantum Newton's cradle type experiment, we excite the atoms to oscillate and collide in an array of 1D tubes and observe the evolution for up to 4.8 seconds (400 oscillations) with minimal heating and loss. By investigating the dynamics of the longitudinal momentum distribution function and the transverse excitation, we observe and quantify a two-stage relaxation process. In the initial stage single-body dephasing reduces the 1D densities, thus rapidly drives the 1D gas out of the quantum degenerate regime. The momentum distribution function asymptotically approaches the distribution of quasimomenta (rapidities), which are conserved in an integrable system. In the subsequent long time evolution, the 1D gas slowly relaxes towards thermal equilibrium through the collisions with transversely excited atoms. Moreover, we tune the dynamics in the dimensional crossover by initializing the evolution with different imprinted longitudinal momenta (energies). The dynamical evolution towards the relaxed state is quantitatively described by a semiclassical molecular dynamics simulation.
Highlights
In physical realization in the laboratory, “integrability” is never perfectly maintained
To study the non-equilibrium dynamics after the Bragg pulses, we explore the momentum distribution function (MDF) f (t, k) for an evolution time up to 4.8 s (400 oscillation periods)
We have investigated the relaxation processes of bosons at the onset of the dimensional crossover from 1D to 3D
Summary
We start our experiment by preparing a 87Rb BEC in an all-optical trap. The prepared 1D gases are characterized by the following key parameters: Atom number. The atom number per tube varies across the 1D trap array. To balance the contributions from each tube, we calculate the weighted-average atom number. To account for the inhomogeneous distribution of atoms over the tubes, we calculate the weighted average for γ. The reduced temperature T = 2ħh2kB T /(mg12D), together with γ, characterize the degeneracy of 1D gases. Our Newton’s cradle experiments start in the intermediate regime of degeneracy and approach the non-degenerate limit as the dephasing occurs. Heating is evaluated by holding a BEC in the identical trapping potential without a Bragg-pulse excitation. We can safely neglect the effect of tunneling
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