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

Nonlinear Dynamics

Bright and dark solitons under spatiotemporal modulation in (2+1)-dimensional Spin-1 Bose-Einstein condensates

Nan Li, Su-Yong Xu, Yunzhou Sun, Quan Chen

Published Sep 9, 2024• 7 citations
Publisher
DOI
10.1007/s11071-024-10243-4

Related papers

Spatiotemporal modulated solitons in a quasi-one-dimensional spin-1 Bose–Einstein condensates

Feiyan Liu, Su-Yong Xu, Houria Triki +2 more

Chaos Solitons & Fractals•May 3, 2024•29 citations

Oscillations and interactions of dark and dark–bright solitons in Bose–Einstein condensates

Christoph Becker, Simon Stellmer, Parvis Soltan-Panahi +6 more

arXiv:0804.0544•Nature Physics•May 4, 2008•594 citations

Phase diagram and dynamics of dark-bright vector solitons in spin-orbit-coupled Bose–Einstein condensate

T.F. Xu, W.L. Li, Zai-Dong Li +1 more

Chaos Solitons & Fractals•Apr 14, 2018•20 citations

Quasi-one-dimensional soliton in a self-repulsive spin-orbit-coupled dipolar spin-half and spin-one condensates

S. K. Adhikari

We study the formation of solitons in a uniform quasi-one-dimensional (quasi-1D) spin-orbit (SO) coupled self-repulsive pseudo spin-half and spin-one dipolar Bose-Einstein condensates (BEC), using the mean-field Gross-Pitaevskii equation. The dipolar atoms are taken to be polarized along the quasi-1D $x$ direction. In the pseudo spin-half case, for small SO-coupling, one can have dark-bright and bright-bright solitons. For large SO coupling, the dark-bright and bright-bright solitons may acquire a spatially-periodic modulation in density; for certain values of contact interaction paramerers there is only the normal bright-bright soliton without spatially-periodic modulation in density. In the spin-one anti-ferromagnetic case, for small SO coupling, one can have bright-bright-bright, dark-bright-dark, and bright-dark-bright solitons; and for large SO coupling, the dark-bright-dark and bright-dark-bright solitons are found to have spatially-periodic modulation in density. In the spin-one ferromagnetic case, for both small and large SO coupling, we find only bright-bright-bright solitons. All these solitons, specially those with a dark-soliton component, are dynamically stable as demonstrated by real-time propagation using the converged stationary solution obtained by imaginary-time propagation as the initial state.

arXiv:2601.12412•Jan 18, 2026•0 citations

Vector dark and bright soliton wave solutions and collisions for spin-1 Bose–Einstein condensate

Fajun Yu, Li Li

Nonlinear Dynamics•Dec 5, 2016•33 citations

Dynamically stabilized bright solitons in a two-dimensional Bose-Einstein condensate

Hiroki Saito

•Jan 1, 2003•0 citations
We study the formation of solitons in a uniform quasi-one-dimensional (quasi-1D) spin-orbit (SO) coupled self-repulsive pseudo spin-half and spin-one dipolar Bose-Einstein condensates (BEC), using the mean-field Gross-Pitaevskii equation. The dipolar atoms are taken to be polarized along the quasi-1D xxx direction. In the pseudo spin-half case, for small SO-coupling, one can have dark-bright and bright-bright solitons. For large SO coupling, the dark-bright and bright-bright solitons may acquire a spatially-periodic modulation in density; for certain values of contact interaction paramerers there is only the normal bright-bright soliton without spatially-periodic modulation in density. In the spin-one anti-ferromagnetic case, for small SO coupling, one can have bright-bright-bright, dark-bright-dark, and bright-dark-bright solitons; and for large SO coupling, the dark-bright-dark and bright-dark-bright solitons are found to have spatially-periodic modulation in density. In the spin-one ferromagnetic case, for both small and large SO coupling, we find only bright-bright-bright solitons. All these solitons, specially those with a dark-soliton component, are dynamically stable as demonstrated by real-time propagation using the converged stationary solution obtained by imaginary-time propagation as the initial state.