超冷原子与一组固定杂质相互作用的束缚态

Marta Sroczy'nska, Z. Idziaszek
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引用次数: 1

摘要

在本文中,我们分析了原子与一组静态杂质相互作用的束缚态的性质。我们从单个原子与两个静态杂质相互作用的最简单系统开始。我们考虑了两种类型的原子-杂质相互作用:(i)由正则化δ表示的零范围势,(ii)更现实的极化势,代表原子-离子相互作用的远程部分。对于前者,我们得到了束缚态能量的解析结果。对于后者,我们应用有限元法进行了数值计算。然后,我们转向单原子与一维(1D)无限静态离子链相互作用的情况。这种设置类似于一维晶体固体的Kronig-Penney模型,其中能谱表现出能带结构行为。对于该体系,我们推导了假设正则三角洲相互作用的束缚态带结构的解析结果,并进行了数值计算,考虑极化势来模拟原子-杂质相互作用。当杂质之间的分离远远大于相互作用势的特征范围时,这两种方法都很符合。
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Bound states of an ultracold atom interacting with a set of stationary impurities
In this manuscript we analyse properties of bound states of an atom interacting with a set of static impurities. We begin with the simplest system of a single atom interacting with two static impurities. We consider two types of atom-impurity interaction: (i) zero-range potential represented by regularized delta, (ii) more realistic polarization potential, representing long-range part of the atom-ion interaction. For the former we obtain analytical results for energies of bound states. For the latter we perform numerical calculations based on the application of finite element method. Then, we move to the case of a single atom interacting with one-dimensional (1D) infinite chain of static ions. Such a setup resembles Kronig-Penney model of a 1D crystalline solid, where energy spectrum exhibits band structure behaviour. For this system, we derive analytical results for the band structure of bound states assuming regularized delta interaction, and perform numerical calculations, considering polarization potential to model atom-impurity interaction. Both approaches agree quite well when separation between impurities is much larger than characteristic range of the interaction potential.
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