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Springer eBooks

Bose Gas, Integrable Nonlinear Schrödinger Equations and Landaulifshitz Models

Vladimir G. Makhankov

Published Jan 1, 1990• 0 citations
Publisher
DOI
10.1007/978-94-009-2217-4_7

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Once its phase-space density is high enough, an interacting dilute Bose gas can be described by a macroscopic wave function obeying nonlinear dynamics. Ultracold Bose gases thus form coherent quantum fluids whose behavior becomes particularly rich in one dimension, where interactions and integrability tightly guide the evolution. In this thesis, we study a two-component weakly interacting 1D Bose gas that maps onto the attractive nonlinear Schrödinger equation (NLSE) in a certain limit, and more generally onto the Landau-Lifshitz equation (LLE), governing spin-chains. This correspondence enables the controlled preparation and exploration of multi-soliton solutions of both models. We first realize NLSE multi-solitons and characterize their dynamics, including their distinctive breathing behavior. Using the full LLE mapping, we then extend this implementation to multi-solitons with arbitrary depletion, thereby accessing a broader family of solitons and revealing features intrinsic to the underlying spin-chain description. Finally, we investigate weak integrability breaking and show that it drives the decomposition of multi-solitons into their constituents, rendering their encoded scattering data experimentally accessible. This provides a controlled pathway to probe integrable structures, opening prospects for studying soliton gases, interacting nonlinear waves, and the emergence of complex dynamics from nearly integrable systems.
The cubic nonlinear Schrödinger equation with repulsive nonlinearity and an elliptic function potential models a quasi-one-dimensional repulsive dilute gas Bose-Einstein condensate trapped in a standing light wave. New families of stationary solutions are presented. Some of these solutions have neither an analog in the linear Schrödinger equation nor in the integrable nonlinear Schrödinger equation. Their stability is examined using analytical and numerical methods. All trivial-phase stable solutions are deformations of the ground state of the linear Schrödinger equation. Our results show that a large number of condensed atoms is sufficient to form a stable, periodic condensate. Physically, this implies stability of states near the Thomas-Fermi limit.
Using a standing light wave potential, a stable quasi-one-dimensional attractive dilute-gas Bose-Einstein condensate can be realized. In a mean-field approximation, this phenomenon is modeled by the cubic nonlinear Schr\"odinger equation with attractive nonlinearity and an elliptic function potential of which a standing light wave is a special case. New families of stationary solutions are presented. Some of these solutions have neither an analog in the linear Schr\"odinger equation nor in the integrable nonlinear Schr\"odinger equation. Their stability is examined using analytic and numerical methods. Trivial-phase solutions are experimentally stable provided they have nodes and their density is localized in the troughs of the potential. Stable time-periodic solutions are also examined.