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Integro-differential equation for Bose-Einstein condensates

机译:玻色-爱因斯坦凝聚物的积分微分方程

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We use the assumption that the potential for the A-boson system can be written as a sum of pairwise acting forces to decompose the wave function into Faddeev components that fulfill a Faddeev type equation. Expanding these components in terms of potential harmonic (PH) polynomials and projecting on the potential basis for a specific pair of particles results in a two-variable integro-differential equations suitable for A-boson bound-state studies. The solution of the equation requires the evaluation of Jacobi polynomials P_k~α β(x) and of the weight function W(z) which give severe numerical problems for very large A. However, using appropriate limits for A → ∞ we obtain a variant equation which depends only on the input two-body interaction, and the kernel in the integral part has a simple analytic form. This equation can be readily applied to a variety of bosonic systems such as microclusters of noble gasses. We employ it to obtain results for A ∈ (10-100) ~(87)Rb atoms interacting via interatomic interactions and confined by an externally applied trapping potential V_(trap)(r). Our results are in excellent agreement with those previously obtained using the potential harmonic expansion method (PHEM) and the diffusion Monte Carlo (DMC) method.
机译:我们使用这样一个假设,即可以将A玻色子系统的电势写为成对作用力的总和,以将波函数分解成满足Faddeev型方程的Faddeev分量。根据电势谐波(PH)多项式扩展这些分量并基于电势对特定的一对粒子进行投影,将得出适用于A玻色子束缚态研究的二变量积分微分方程。该方程式的求解需要评估Jacobi多项式P_k〜αβ(x)和权重函数W(z),这会给非常大的A带来严重的数值问题。但是,使用适当的A→∞极限,我们可以获得一个变体该方程仅取决于输入的两体相互作用,并且积分部分的核具有简单的解析形式。该方程式可以很容易地应用于各种玻色系统,例如稀有气体的微团簇。我们使用它来获得A∈(10-100)〜(87)Rb原子通过原子间相互作用而相互作用并受外部施加的俘获势V_(trap)(r)限制的结果。我们的结果与以前使用电势谐波扩展法(PHEM)和扩散蒙特卡洛(DMC)方法获得的结果非常一致。

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