Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:cond-mat/0304148 · Journal of Physics B Atomic Molecular and Optical Physics

Deformation of dark solitons in inhomogeneous Bose–Einstein condensates

Nicholas G. Parker, Nick P. Proukakis, M. L. Leadbeater, Charles S. Adams

Published Jun 23, 2003• 39 citations
arXivHTMLPDF

Abstract

A dark soliton becomes unstable when it is incident on a background density gradient, and the induced instability results in the emission of sound. Detailed quantitative studies of sound emission are performed for various potentials, such as steps, linear ramps and Gaussian traps. The amount of sound emission is found to be a significant fraction of the soliton energy for typical potentials. Continuous emission of sound is found to lead to an apparent deformation of the soliton profile. The power emitted by the soliton is shown to be parametrized by the square of the displacement of the centre of mass of the soliton from its density minimum, thus highlighting the significance of the inhomogeneity-induced soliton deformation.

DOI
10.1088/0953-4075/36/13/318

Related papers

Deformation of Dark Solitons in Inhomogeneous Bose-Einstein Condensates

NG Parker, Nick P. Proukakis, M. Leadbeater +1 more

A dark soliton becomes unstable when it is incident on a background density gradient, and the induced instability results in the emission of sound. Detailed quantitative studies of sound emission are performed for various potentials, such as steps, linear ramps and Gaussian traps. The amount of sound emission is found to be a significant fraction of the soliton energy for typical potentials. Continuous emission of sound is found to lead to an apparent deformation of the soliton profile. The power emitted by the soliton is shown to be parametrized by the square of the displacement of the centre of mass of the soliton from its density minimum, thus highlighting the significance of the inhomogeneity-induced soliton deformation.

•Dec 31, 2003•0 citations

Dark Soliton Dynamics in Confined Bose-Einstein Condensates

Parker Ng, Nick P. Proukakis, C. S. Adams

Dilute atomic Bose-Einstein condensates are inherently nonlinear systems and support solitary wave solutions. An important distinction from optical systems is the inhomogeneous background density, which results from the traps used to confine the atoms. As in optical systems, dark solitary waves in three-dimensional geometries are unstable to transverse excitations, which lead to a bending of the dark soliton plane and decay into vortex rings. Highly elon-gated geometries can now be achieved experimentally, in which the condensate dynamics are effectively one-dimensional, and the motion of the dark soliton is governed by the inhomogeneous longitudinal density. We show that a dark soliton is fundamentally unstable to such a changing background density, by means of numerical simulations of the soliton under various potentials (e.g. steps, ramps, harmonic traps, and optical lattices). This leads to the emission of radiation in the form of sound waves. The power emitted is found to be proportional to the square of the soliton acceleration. The latter quantity is shown to be proportional to the deformation of the apparent soliton profile, arising from the sound field in the region of the soliton. We demonstrate that the ensuing interactions between the soliton and sound field, and therefore the dynamics of the soliton, can be controlled experimentally via manipulation of the emitted sound, achieved by modifying the trap geometry. In this manner, it is possible to induce a rapid decay of the soliton, stabilise the soliton, or even pump energy into the soliton by means of parametric driving. 1

•Dec 31, 2007•1 citation

Dynamical instability of a dark soliton in a quasi-one-dimensional Bose–Einstein condensate perturbed by an optical lattice

N G Parker, Nick P. Proukakis, C F Barenghi +1 more

The motion of a dark soliton is investigated in a one-dimensional dilute Bose–Einstein condensate confined in a harmonic trap and an optical lattice. The harmonic trap induces a dynamical instability of the soliton, culminating in sound emission. The presence of the perturbing optical lattice enhances the instability, and in addition, dephases the emitted sound waves, thus preventing stabilization of the soliton by sound reabsorption. This instability can be probed experimentally by monitoring the soliton oscillations under various lattice configurations, which can be realized by changing the intensity and angle between the laser beams that form the lattice. For short enough times, such that the emitted sound does not reinteract with the soliton, the power emitted by the soliton is found to be proportional to the square of the local soliton acceleration, which is in turn proportional to the deformation of the soliton profile.

arXiv:cond-mat/0310759•Journal of Physics B Atomic Molecular and Optical Physics•Mar 24, 2004•41 citations

Dynamical instability of a dark soliton in a quasi-one-dimensional Bose-Einstein condensate perturbed by an optical lattice

Nicholas G. Parker, Nick P. Proukakis, Carlo Barenghi +1 more

The motion of a dark soliton is investigated in a one-dimensional dilute Bose-Einstein condensate confined in a harmonic trap and an optical lattice. The harmonic trap induces a dynamical instability of the soliton, culminating in sound emission. The presence of the perturbing optical lattice enhances the instability, and in addition, dephases the emitted sound waves, thus preventing stabilization of the soliton by sound reabsorption. This instability can be probed experimentally by monitoring the soliton oscillations under various lattice configurations, which can be realized by changing the intensity and angle between the laser beams that form the lattice. For short enough times, such that the emitted sound does not reinteract with the soliton, the power emitted by the soliton is found to be proportional to the square of the local soliton acceleration, which is in turn proportional to the deformation of the soliton profile.

•Dec 31, 2003•0 citations

Coupling between Topological Excitations and the Background Sound Field in Atomic Bose-Einstein Condensates

Nick P. Proukakis, Nicholas G. Parker, Carlo Barenghi +1 more

Topological excitations in quantum fluids are coupled to the background sound field. This leads to a continuous exchange of energy between the two systems, as a result of which, the topological excitation can become deformed and its trajectory modified. These effects are considered in detail for dark solitons in trapped one-dimensional atomic Bose-Einstein condensates. The energy emitted by the dark soliton incident on a background potential gradient is shown to be proportional to the square of both the soliton deformation and the local soliton acceleration. Depending on the trap geometry, this energy can be partly or fully reabsorbed by the soliton, thus affecting its stability. The extension to vortices in trapped atomic condensates is discussed.

•Dec 31, 2004•0 citations

Coupling Between Topological Excitations And The Background Sound Field In Atomic Bose-einstein Condensates

Nick P. Proukakis, Nicholas G. Parker, Carlo F. Barenghi +1 more

Topological excitations in quantum fluids are coupled to the background sound field. This leads to a continuous exchange of energy between the two systems, as a result of which, the topological excitation can become deformed and its trajectory modified. These effects are considered in detail for dark solitons in trapped one-dimensional atomic Bose-Einstein condensates. The energy emitted by the dark soliton incident on a back-ground potential gradient is shown to be proportional to the square of both the soliton deformation and the local soliton acceleration. Depending on the trap geometry, this energy can be partly or fully reabsorbed by the soliton, thus affecting its stability. The extension to vortices in trapped atomic condensates is discussed.

•Dec 31, 2004•0 citations
A dark soliton becomes unstable when it is incident on a background density gradient, and the induced instability results in the emission of sound. Detailed quantitative studies of sound emission are performed for various potentials, such as steps, linear ramps and Gaussian traps. The amount of sound emission is found to be a significant fraction of the soliton energy for typical potentials. Continuous emission of sound is found to lead to an apparent deformation of the soliton profile. The power emitted by the soliton is shown to be parametrized by the square of the displacement of the centre of mass of the soliton from its density minimum, thus highlighting the significance of the inhomogeneity-induced soliton deformation.
A dark soliton becomes unstable when it is incident on a background density gradient, and the induced instability results in the emission of sound. Detailed quantitative studies of sound emission are performed for various potentials, such as steps, linear ramps and Gaussian traps. The amount of sound emission is found to be a significant fraction of the soliton energy for typical potentials. Continuous emission of sound is found to lead to an apparent deformation of the soliton profile. The power emitted by the soliton is shown to be parametrized by the square of the displacement of the centre of mass of the soliton from its density minimum, thus highlighting the significance of the inhomogeneity-induced soliton deformation.
Dilute atomic Bose-Einstein condensates are inherently nonlinear systems and support solitary wave solutions. An important distinction from optical systems is the inhomogeneous background density, which results from the traps used to confine the atoms. As in optical systems, dark solitary waves in three-dimensional geometries are unstable to transverse excitations, which lead to a bending of the dark soliton plane and decay into vortex rings. Highly elon-gated geometries can now be achieved experimentally, in which the condensate dynamics are effectively one-dimensional, and the motion of the dark soliton is governed by the inhomogeneous longitudinal density. We show that a dark soliton is fundamentally unstable to such a changing background density, by means of numerical simulations of the soliton under various potentials (e.g. steps, ramps, harmonic traps, and optical lattices). This leads to the emission of radiation in the form of sound waves. The power emitted is found to be proportional to the square of the soliton acceleration. The latter quantity is shown to be proportional to the deformation of the apparent soliton profile, arising from the sound field in the region of the soliton. We demonstrate that the ensuing interactions between the soliton and sound field, and therefore the dynamics of the soliton, can be controlled experimentally via manipulation of the emitted sound, achieved by modifying the trap geometry. In this manner, it is possible to induce a rapid decay of the soliton, stabilise the soliton, or even pump energy into the soliton by means of parametric driving. 1
The motion of a dark soliton is investigated in a one-dimensional dilute Bose–Einstein condensate confined in a harmonic trap and an optical lattice. The harmonic trap induces a dynamical instability of the soliton, culminating in sound emission. The presence of the perturbing optical lattice enhances the instability, and in addition, dephases the emitted sound waves, thus preventing stabilization of the soliton by sound reabsorption. This instability can be probed experimentally by monitoring the soliton oscillations under various lattice configurations, which can be realized by changing the intensity and angle between the laser beams that form the lattice. For short enough times, such that the emitted sound does not reinteract with the soliton, the power emitted by the soliton is found to be proportional to the square of the local soliton acceleration, which is in turn proportional to the deformation of the soliton profile.
The motion of a dark soliton is investigated in a one-dimensional dilute Bose-Einstein condensate confined in a harmonic trap and an optical lattice. The harmonic trap induces a dynamical instability of the soliton, culminating in sound emission. The presence of the perturbing optical lattice enhances the instability, and in addition, dephases the emitted sound waves, thus preventing stabilization of the soliton by sound reabsorption. This instability can be probed experimentally by monitoring the soliton oscillations under various lattice configurations, which can be realized by changing the intensity and angle between the laser beams that form the lattice. For short enough times, such that the emitted sound does not reinteract with the soliton, the power emitted by the soliton is found to be proportional to the square of the local soliton acceleration, which is in turn proportional to the deformation of the soliton profile.
Topological excitations in quantum fluids are coupled to the background sound field. This leads to a continuous exchange of energy between the two systems, as a result of which, the topological excitation can become deformed and its trajectory modified. These effects are considered in detail for dark solitons in trapped one-dimensional atomic Bose-Einstein condensates. The energy emitted by the dark soliton incident on a background potential gradient is shown to be proportional to the square of both the soliton deformation and the local soliton acceleration. Depending on the trap geometry, this energy can be partly or fully reabsorbed by the soliton, thus affecting its stability. The extension to vortices in trapped atomic condensates is discussed.
Topological excitations in quantum fluids are coupled to the background sound field. This leads to a continuous exchange of energy between the two systems, as a result of which, the topological excitation can become deformed and its trajectory modified. These effects are considered in detail for dark solitons in trapped one-dimensional atomic Bose-Einstein condensates. The energy emitted by the dark soliton incident on a back-ground potential gradient is shown to be proportional to the square of both the soliton deformation and the local soliton acceleration. Depending on the trap geometry, this energy can be partly or fully reabsorbed by the soliton, thus affecting its stability. The extension to vortices in trapped atomic condensates is discussed.