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Non-equilibrium Dynamics of Tunnel-Coupled Superfluids - Relaxation to a Phase-Locked Equilibrium State in a One-Dimensional Bosonic Josephson Junction (Paperback, 1st ed. 2020)
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Non-equilibrium Dynamics of Tunnel-Coupled Superfluids - Relaxation to a Phase-Locked Equilibrium State in a One-Dimensional Bosonic Josephson Junction (Paperback, 1st ed. 2020)
Series: Springer Theses
Expected to ship within 10 - 15 working days
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The relaxation of isolated quantum many-body systems is a major
unsolved problem of modern physics, which is connected to many
fundamental questions. However, realizations of quantum many-body
systems which are both well isolated from their environment and
accessible to experimental study are scarce. In recent years, the
field has experienced rapid progress, partly attributed to
ultra-cold atoms. This book presents the experimental study of a
relaxation phenomenon occurring in a one-dimensional bosonic
Josephson junction. The system consists of two 1D quasi
Bose-Einstein condensates of 87Rb, magnetically trapped on an atom
chip. Using radio-frequency dressing, the author deforms a single
harmonic trap, in which the atoms are initially condensed, into a
double-well potential and realizes a splitting of the wave
function. A large spatial separation and a tilt of the double-well
enable the preparation of a broad variety of initial states by
precisely adjusting the initial population and relative phase of
the two wave packets, while preserving the phase coherence. By
re-coupling the two wave packets, the author investigates tunneling
regimes such as Josephson (plasma) oscillations and macroscopic
quantum self-trapping. In both regimes, the tunneling dynamics
exhibits a relaxation to a phase-locked equilibrium state
contradicting theoretical predictions. The experimental results are
supported with an empirical model that allows quantitative
discussions according to various experimental parameters. These
results illustrate how strongly the non-equilibrium dynamics differ
from the equilibrium one, which is well described by thermodynamics
and statistical physics.
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