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中国物理学会期刊

碟形玻色-爱因斯坦凝聚体中(0, 0, 2)剪刀模的朗道阻尼和频移

CSTR: 32037.14.aps.68.20190661

Landau damping and frequency-shift of (0, 0, 2) scissors mode in a disc-shaped Bose-Einstein condensate

CSTR: 32037.14.aps.68.20190661
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  • 应用哈特里-福克-博戈留波夫平均场理论近似和基于托马斯-费米近似的解析方法, 研究碟形玻色-爱因斯坦凝聚体中(0, 0, 2)剪刀模的朗道阻尼和频移, 计算阻尼系数和频移大小以及它们的温度依赖. 计算中, 在集体激发本征频移微扰关系中考虑元激发弛豫及其弛豫之间的正交关系以获得阻尼和频移的计算公式, 把凝聚体基态波函数取为高斯分布函数的一级近似以消除托马斯-费米近似中三模耦合矩阵元的发散. 采用与相关实验研究相同的粒子数、囚禁频率和各向异性参量, 理论计算结果与相关实验测量结果相符合. 由于理论的复杂性和计算的困难性, 在大多数基于平均场理论的单分量和两分量玻色-爱因斯坦凝聚集体激发阻尼和频移的研究中采用半经典近似, 把准粒子激发能谱看成是连续的来积分计算各个准粒子跃迁对阻尼和频移的贡献, 而本文和本文前期工作按分立的准粒子激发频谱计算阻尼或频移, 并在研究过程中提出了考虑元激发弛豫及弛豫之间正交关系的改进方法, 希望这种方法对今后的工作有一定参考价值.

     

    By using the Hartree-Fock-Bogoliubov approximation of mean-field theory and the analytic method based on Thomas-Feimi approximation, the Landau damping and frequency-shift of (0, 0, 2) scissors mode in a disc-shaped Bose-Einstein condensate are investigated and the damping rate and frequency-shift magnitude as well as their temperature dependence are calculated. In the calculation, the practical relaxations of the elementary excitations and the orthometric relation among the relaxations are considered in the relation for the perturbed eigenfrequency of mean-field theory to obtain the calculation formula of damping and frequency-shift, and the first-order approximation of Gaussian distribution function is employed for the ground-state wavefunction to eliminate the divergence of the three-mode coupling matrix elements in Thomas-Fermi approximation. Taking the same parameters of particle number, trapping frequency and anisotropy as those in relevent experiment research, our theoretical calculation results accord with the relevent experimental measurement results. Because of the complexity of the theory and the difficulty of calculation, most of mean-field theory researches on damping and frequency shift of collective excitation in one and two component Bose-Einstein condensates adopt semi-classical approximation, the quasi-particle excitation spectrum is regarded as continuously integrating each quasi-particle transition contribution to damping and frequency shift. In this paper, the damping and frequency shift are calculated according to the discrete quasi-particle excitation spectrum, and in the course of the study the improving of method of considering the practical relaxations of the elementary excitations and the orthometric relation among the relaxations is put forward. It is hoped that the method will have some reference value in the future work.

     

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