Spin-orbit coupling controlling the topological vortical phase transition in spin-2 rotating Bose-Einstein condensates

被引:7
|
作者
Zhu, Hao [1 ,2 ]
Liu, Chao-Fei [3 ]
Wang, Deng-Shan [4 ]
Yin, Shou-Gen [1 ]
Zhuang, Lin [5 ]
Liu, Wu-Ming [2 ,6 ,7 ]
机构
[1] Tianjin Univ Technol, Sch Mat Sci & Engn, Key Lab Display Mat & Photoelect Devices, Tianjin Key Lab Photoelect Mat & Devices,Minist E, Tianjin 300384, Peoples R China
[2] Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
[3] Jiangxi Univ Sci & Technol, Sch Sci, Ganzhou 341000, Peoples R China
[4] Beijing Normal Univ, Sch Math Sci, Minist Educ, Lab Math & Complex Syst, Beijing 100875, Peoples R China
[5] Sun Yat Sen Univ, Sch Phys, Guangzhou 510257, Peoples R China
[6] Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100190, Peoples R China
[7] Songshan Lake Mat Lab, Dongguan 523808, Guangdong, Peoples R China
基金
国家重点研发计划;
关键词
GAS;
D O I
10.1103/PhysRevA.104.053325
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We investigate the combined effects of spin-orbit coupling and rotation on the topological vortical phase transition in F = 2 Bose-Einstein condensates. We find that the spin-orbit coupling can precisely manipulate the canonical atom current which is generated in the opposite direction of the gauge atom current and causes both a continuous and a discontinuous canonical angular momentum. We apply the canonical angular momentum and magnetization to reveal the emergence of novel topological excitations, such as the Anderson-Toulouse vortex as well as the vortex-dipole lattice. Especially, strong spin-orbit coupling can induce two perpendicular vortex chains. We also find that both the first-order and the second-order phase transition can be characterized by the canonical angular momentum and the magnetization. Differently from the spin singlet-pairing interaction, the spin-exchange interaction can adjust the canonical angular momentum and control the phase transition well. The topological vortical phase transition in an F = 2 cold-atom system is compatible with the current experiment and can be detected by the spin polarization procedure.
引用
收藏
页数:8
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