在光学加谐波阱的吸引玻色-爱因斯坦凝聚中原子的临界数目

S. Adhikari
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引用次数: 5

摘要

利用随时间平均场Gross-Pitaevskii方程的数值解,研究了吸引玻色-爱因斯坦凝聚体在联合一维光学晶格和轴对称谐波阱上的稳定性,并计算了稳定凝聚体的临界原子数。我们还计算了双阱势中的临界原子数,它总是大于轴对称谐波阱中的临界原子数。在没有光阱的情况下,通过在谐波阱的轴向移动光晶格势的一个节点,可以使光阱中的临界原子数比相应的数更小或更大。原子临界数的这种变化可以用实验观察到,并与目前的计算进行比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The critical number of atoms in an attractive Bose–Einstein condensate on optical plus harmonic traps
The stability of an attractive Bose–Einstein condensate on a joint one-dimensional optical lattice and an axially symmetrical harmonic trap is studied using the numerical solution of the time-dependent mean-field Gross–Pitaevskii equation and the critical number of atoms for a stable condensate is calculated. We also calculate this critical number of atoms in a double-well potential which is always greater than that in an axially symmetrical harmonic trap. The critical number of atoms in an optical trap can be made smaller or larger than the corresponding number in the absence of the optical trap by moving a node of the optical lattice potential in the axial direction of the harmonic trap. This variation of the critical number of atoms can be observed experimentally and compared with the present calculations.
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