Vortex lattices in binary Bose-Einstein condensates with dipole-dipole interactions

被引:38
作者
Kumar, Ramavarmaraja Kishor [1 ]
Tomio, Lauro [2 ,3 ]
Malomed, Boris A. [4 ,5 ]
Gammal, Arnaldo [1 ]
机构
[1] Univ Sao Paulo, Inst Fis, BR-05508090 Sao Paulo, SP, Brazil
[2] Univ Estadual Paulista, Inst Fis Teor, BR-01156970 Sao Paulo, SP, Brazil
[3] DCTA, Inst Tecnol Aeronaut, BR-12228900 Sao Jose Dos Campos, SP, Brazil
[4] Tel Aviv Univ, Sch Elect Engn, Fac Engn, Dept Phys Elect, IL-69978 Tel Aviv, Israel
[5] ITMO Univ, St Petersburg 197101, Russia
基金
巴西圣保罗研究基金会; 美国国家科学基金会; 以色列科学基金会;
关键词
VORTICES; STATES; ALGORITHM; DROPLETS;
D O I
10.1103/PhysRevA.96.063624
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We study the structure and stability of vortex lattices in two-component rotating Bose-Einstein condensates with intrinsic dipole-dipole interactions and contact interactions. To address experimentally accessible coupled systems, we consider Dy-164-Dy-162 and Er-168-Dy-164 mixtures, which feature different miscibilities. The corresponding dipole moments are mu(Dy) = 10 mu(B) and mu(Er) = 7 mu(B), where mu(B) is the Bohr magneton. For comparison we also discuss a case where one of the species is nondipolar. Under a large aspect ratio of the trap, we consider mixtures in the pancake-shaped format, which are modeled by effective two-dimensional coupled Gross-Pitaevskii equations, with a fixed polarization of the magnetic dipoles. Then, the miscibility and vortex-lattice structures are studied by varying the coefficients of the contact interactions (assuming the use of the Feshbach-resonance mechanism) and the rotation frequency. We present phase diagrams for several types of lattices in the parameter plane of the rotation frequency and the ratio of inter-and intraspecies scattering lengths. The vortex structures are found to be diverse for the more miscible Dy-164-Dy-162 composition, with a variety of shapes, whereas for the less miscible case of Er-168-Dy-164, the lattice patterns mainly feature circular or square formats.
引用
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页数:9
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