2020
DOI: 10.1016/j.physleta.2020.126430
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Density structures and giant vortex in spin-orbit coupled Bose-Einstein condensates with the harmonic-plus-radial potential

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Cited by 4 publications
(2 citation statements)
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“…For the thermodynamic properties of condensates, the specific heat, transition temperature and condensation fraction of interacting Bose gases are also modified by anharmonic potential [27]. On the other hand, after the realization of SO coupled BECs [3], the SO coupling breaks the Galilean invariance of the system and regulates the collapse of the condensates [46], and the anharmonicity of external potential can induce novel vortex structures [47][48][49] and topological defects [21] in the rotating condensates such as skyrmion, meron cluster, skyrmion string and various skyrmion lattices [50]. Similar phenomena occurs in rotating dipolar condensates due to anharmonic trap [30].…”
Section: Introductionmentioning
confidence: 99%
“…For the thermodynamic properties of condensates, the specific heat, transition temperature and condensation fraction of interacting Bose gases are also modified by anharmonic potential [27]. On the other hand, after the realization of SO coupled BECs [3], the SO coupling breaks the Galilean invariance of the system and regulates the collapse of the condensates [46], and the anharmonicity of external potential can induce novel vortex structures [47][48][49] and topological defects [21] in the rotating condensates such as skyrmion, meron cluster, skyrmion string and various skyrmion lattices [50]. Similar phenomena occurs in rotating dipolar condensates due to anharmonic trap [30].…”
Section: Introductionmentioning
confidence: 99%
“…[33][34][35][36] Recently, spin-orbit coupled spinor BECs in the different periodic potentials, like the toroidal trap, spin-dependent periodic potential and radially-periodic potential are investigated, which results in many exotic ground-state phases and solitons. [37][38][39][40][41][42][43][44][45][46] In this paper, we consider 2D spin-orbit coupled spin-1 BECs in two types of radially-periodic potentials, i.e., spinindependent and spin-dependent radially-periodic potentials. For the BECs in a spin-independent radially-periodic potential, the density of each component exhibits the periodic density modulation along the azimuthal direction, which realizes the necklacelike state in the ferromagnetic BECs.…”
Section: Introductionmentioning
confidence: 99%