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Resonant and Non-Resonant Modulated Amplitude Waves for Binary Bose-Einstein Condensates in Optical Lattices

机译:二元系统的谐振和非共振调制振幅波   光学格子中的玻色 - 爱因斯坦凝聚体

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摘要

We consider a system of two Gross-Pitaevskii (GP) equations, in the presenceof an optical-lattice (OL) potential, coupled by both nonlinear and linearterms. This system describes a Bose-Einstein condensate (BEC) composed of twodifferent spin states of the same atomic species, which interact linearlythrough a resonant electromagnetic field. In the absence of the OL, we findplane-wave solutions and examine their stability. In the presence of the OL, wederive a system of amplitude equations for spatially modulated states which arecoupled to the periodic potential through the lowest-order subharmonicresonance. We determine this averaged system's equilibria, which representspatially periodic solutions, and subsequently examine the stability of thecorresponding solutions with direct simulations of the coupled GP equations. Wefind that symmetric (equal-amplitude) and asymmetric (unequal-amplitude)dual-mode resonant states are, respectively, stable and unstable. The unstablestates generate periodic oscillations between the two condensate components,which is possible only because of the linear coupling between them. We alsofind four-mode states, but they are always unstable. Finally, we brieflyconsider ternary (three-component) condensates.
机译:我们考虑两个存在光学和晶格(OL)势的Gross-Pitaevskii(GP)方程的系统,该方程由非线性项和线性项耦合。该系统描述了由相同原子种类的两个不同的自旋态组成的玻色-爱因斯坦凝聚物(BEC),它们通过共振电磁场线性相互作用。在没有OL的情况下,我们找到平面波解决方案并检查其稳定性。在存在OL的情况下,推导了用于空间调制状态的振幅方程组,该振幅方程组通过最低阶次谐波共振耦合到周期电势。我们确定了这个平均系统的平衡,该平衡代表了周期周期的解,然后通过耦合GP方程的直接仿真检查了相应解的稳定性。我们确定对称(等幅)和非对称(不等幅)双模共振态分别是稳定的和不稳定的。不稳定状态在两个凝结水成分之间产生周期性的振荡,这仅是因为它们之间存在线性耦合是可能的。我们还找到了四模式状态,但它们始终不稳定。最后,我们简要考虑三元(三组分)冷凝物。

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