2021
DOI: 10.1088/1367-2630/abd27c
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Phase diagram, stability and magnetic properties of nonlinear excitations in spinor Bose–Einstein condensates

Abstract: The static properties, i.e., existence and stability, as well as the quench-induced dynamics of nonlinear excitations of the vortex-bright type appearing in two-dimensional harmonically confined spin-1 Bose-Einstein condensates are investigated. Linearly stable vortex-bright-vortex and bright-vortex-bright solutions arise in both antiferromagnetic and ferromagnetic spinor gases upon quadratic Zeeman energy shift variations. The precessional motion of such coherent structures is subsequently monitored dynamical… Show more

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Cited by 32 publications
(17 citation statements)
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“…The bulk ordered state is suppressed in the core of the DW, in which the macroscopic wave functions vary continuously between the two states. The core of a topological defect in spin-1 BECs has been revealed to exhibit complicated states [32,[39][40][41][42][43][44][45][46][47][48][49]. Similarly, there are different possibilities for the local states at the wall in our system.…”
Section: The Energy Densities G(mentioning
confidence: 79%
“…The bulk ordered state is suppressed in the core of the DW, in which the macroscopic wave functions vary continuously between the two states. The core of a topological defect in spin-1 BECs has been revealed to exhibit complicated states [32,[39][40][41][42][43][44][45][46][47][48][49]. Similarly, there are different possibilities for the local states at the wall in our system.…”
Section: The Energy Densities G(mentioning
confidence: 79%
“…An immediate extension of this work points towards richer systems, e.g., spinor BECs [73][74][75]. These systems are already experimentally realizable [76][77][78], and several works have already exposed the existence of stable solitonic structures both experimentally [32] and theoretically [70,[79][80][81][82]].…”
Section: Conclusion and Future Perspectivesmentioning
confidence: 99%
“…Following Refs. [4,46,47], we consider, in particular, a 23 Na condensate with a a = (a 2 −a 0 )/3 ≈ 2a B and a s = (2a 2 +a 0 )/3 ≈ 50a B in our simulations where a B = 0.0529 nm is the Bohr radius, thus giving c 2 /c 0 ≈ 0.04. For instance, for trapping frequencies Ω = 2π × 10 Hz and and N ≈ 4 × 10 6 , we get c 0 = 2 × 10 4 .…”
Section: A Modelmentioning
confidence: 99%
“…A key feature of spinor condensates is the presence of both spin-independent and spin-dependent interactions [8,9]. Depending on the sign of the latter, the gases can be antiferromagnetic, as in the case of 23 Na [3,4] or ferromagnetic (weakly or strongly, respectively) for 87 Rb [6,7] and 7 Li [12,13]. The phase diagram of the potential ground states (depending on the spin-dependent interactions and the role of external magnetic fields through the so-called quadratic Zeeman effect) has been extensively studied, e.g., in Ref.…”
Section: Introductionmentioning
confidence: 99%
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