自洽随机有限温度建模:具有局部(s 波)和长程(双极)相互作用的超冷玻色气体

Nick P. Proukakis, Gerasimos Rigopoulos, Alex Soto
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摘要

我们提出了一种包含热波动和随机贡献的广义自洽量子动力学理论,用于模拟通过一般长程相互作用的超冷玻色气体。我们的广义方程采用有效场理论的通常形式,将系统的相干、低洼模式与不相干、高洼、热模式分开。低洼模式由随机朗文方程描述,该方程包含两个明确的随时间变化的碰撞项(对应于耗散和能量校正贡献)及其相应的加法和乘法随机噪声项。通过将这样一个方程与水相玻尔兹曼方程描述的非相干(热)粒子的显式非平衡气体耦合,我们从而超越了早期的随机方法(包括完整的 SPGPE)和受双气体图景(即所谓的 ZNG 形式)启发的广义动力学模型,这些模型通常用于短程相互作用,如超冷碱原子中的相关相互作用。通过为长程相互作用势添加自洽的泊松方程,我们的模型进一步包含了长程相互作用。我们的方法直接导致有限温度玻色-爱因斯坦凝聚在长程相互作用系统中的自洽模型,在这个系统中,热波动比量子波动占主导地位。虽然这种方法可普遍用于各种可实验的长程相互作用系统,但我们在此特别关注研究得比较透彻的双极性原子凝聚物的情况。在这一特殊背景下,我们通过波格列乌波夫-德-根纳方程的常规途径,对慢速(相干)模式进行了某种特别的扩展,从而补充了我们对快速(非相干)模式波动的凯尔迪什非均衡分析。
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Self-Consistent Stochastic Finite-Temperature Modelling: Ultracold Bose Gases with Local (s-wave) and Long-Range (Dipolar) Interactions
We formulate a generalized self-consistent quantum kinetic theory including thermal fluctuations and stochastic contributions for modelling ultracold Bose gases interacting via a generic long-range interaction. Our generalised equations take the usual form of an effective field theory, separating coherent, low-lying, modes of the system from incoherent, higher-lying, thermal modes. The low-lying modes are described by a stochastic Langevin equation with two explicitly time-dependent collisional terms (corresponding to a dissipative and an energy-correcting contribution) and their corresponding additive and multiplicative stochastic noise terms. By coupling such an equation to an explicitly non-equilibrium gas of incoherent (thermal) particles described by a quantum Boltzmann equation, we thus extend beyond both earlier stochastic approaches (including the full SPGPE) and generalised kinetic models inspired by a two-gas picture (the so-called ZNG formalism) commonly used in the context of short-range interactions, such as those relevant in ultracold alkali atoms. Long-range interactions are further included into our model by the self-consistent addition of a Poisson-like equation for the long-range interaction potential. Our approach leads directly to a self-consistent model for finite-temperature Bose-Einstein condensation in a long-range interacting system within the regime where thermal fluctuations dominate over quantum fluctuations. While such an approach could be of general use for a variety of experimentally-accessible long-range interacting systems, we focus specifically here on the well-studied case of dipolar atomic condensates. In this particular context, we additionally supplement our Keldysh non-equilibrium analysis for fluctuations of the fast (incoherent) modes by a somewhat ad hoc extension of the slow (coherent) modes via the usual route of Bogoliubov-de Gennes equations.
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