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Quantum mechanics and the hydrogen atom in a generalized Wigner-Seitz cell

机译:广义Wigner-Seitz单元中的量子力学和氢原子

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摘要

We investigate the energy spectrum of a nonrelativistic quantum particle and a hydrogen-like atom placed in a vacuum cavity with general boundary conditions ensuring confinement. When these conditions, as in the Wigner-Seitz model, admit a large amplitude of the wave function on the boundary of the cavity, a nonperturbative rearrangement of lower energy levels of the spectrum occurs, which is essentially different from the case of the confinement by a potential barrier. A nontrivial role in this spectrum rearrangement is played by the von Neumann-Wigner effect of repulsion of nearby levels. For such a confined state of a hydrogen-like atom in a spherical cavity of radius R with the boundary formed by a potential layer of depth d, we show that the lowest energy level of the atom has a pronounced minimum at physically meaningful layer parameters and that the binding energy can be much greater than E_(1s), the energy of the 1s level of a free-standing atom, and that the regime where the atom binding is much greater than E_(1s) becomes possible for a cavity with R ~ 10-100 nm.
机译:我们研究非相对论性量子粒子和类氢原子在真空腔中的能谱,并在一般边界条件下确保禁闭。当这些条件(如在Wigner-Seitz模型中)允许在腔的边界上出现较大的波函数振幅时,会发生光谱较低能级的非扰动重排,这与通过一个潜在的障碍。冯·诺伊曼·威格纳排斥附近能级的作用在这种频谱重排中发挥了重要作用。对于半径为R的球形空腔中的类氢原子的这种受限状态,其边界由深度为d的势能层形成,我们表明,该原子的最低能级在具有物理意义的层参数下具有明显的最小值,并且R的空腔的结合能可能远大于E_(1s),自由原子的1s能级的能量,并且原子结合远大于E_(1s)的状态成为可能〜10-100 nm。

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