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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Quantum kinetic theory. VI. The growth of a Bose-Einstein condensate - art. no. 033606
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Quantum kinetic theory. VI. The growth of a Bose-Einstein condensate - art. no. 033606

机译:量子动力学理论。 VI。玻色-爱因斯坦冷凝物的增长-艺术没有。 033606

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A detailed analysis of the growth of a Bose-Einstein condensate is given, based on quantum kinetic theory, in which we take account of the evolution of the occupations of lower trap levels, and of the full Bose-Einstein formula for the occupations of higher trap levels, as well as the Bose-stimulated direct transfer of atoms to the condensate level introduced by Gardiner et nl. [Phys. Rev. Lett. 79, 1793 (1997); 81, 5266 (1998)]. We find good agreement with experiment at higher temperatures, but at lower temperatures the experimentally observed growth rate is somewhat more rapid. We also confirm the picture of the "kinetic" region of evolution, introduced by Kagan, Svistunov, and Shlyapnikov (Zh. Eksp. Teor. Fit. 101, 538 (1992) [Sov. Phys. JETP 75, 387 (1992)]), for the time up to the initiation of the condensate. The behavior after initiation essentially follows our original growth equation, but with a substantially increased rate coefficient. Our modeling of growth implicitly gives a model of the spatial shape of the density profile of the condensate-vapor system as the condensate grows, and thus provides an alternative to the present phenomenological fitting procedure, based on the sum of a zero-chemical potential vapor and a Thomas-Fermi-shaped condensate. Our method fives substantially different results for condensate numbers and temperatures obtained from phenomenological fits, but fits the published column density data very well. [References: 34]
机译:基于量子动力学理论,给出了玻色-爱因斯坦凝聚物生长的详细分析,其中我们考虑了陷阱水平较低的职业的演变,以及玻色-爱因斯坦关于较高陷阱的职业的完整公式。陷阱能级,以及由加德纳(Gardiner)等人引入的玻色刺激的原子直接转移至冷凝物能级。 [物理牧师79,1793(1997); 81,5266(1998)]。我们发现在较高温度下与实验有很好的一致性,但是在较低温度下,实验观察到的生长速度会更快一些。我们还确认了由Kagan,Svistunov和Shlyapnikov(Zh。Eksp。Teor。Fit。101,538(1992)[Sov。Phys。JETP 75,387(1992))引入的进化“动力学”区域的图片。 ),直到凝结水开始为止。引发后的行为基本上遵循我们最初的增长方程,但是速率系数大大增加。我们的增长模型隐含了一个随着凝结水的增长而形成的凝结水蒸气系统密度分布的空间形状的模型,从而基于零化学势蒸气的总和为当前的现象拟合程序提供了一种替代方法。和托马斯·费米形的冷凝物。对于从现象学拟合获得的冷凝物数量和温度,我们的方法得出的结果实质上不同,但是非常适合已发布的色谱柱密度数据。 [参考:34]

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