在强局部电位极限上

K. Murulane, S. Karataglidis, B. G. Giraud
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引用次数: 0

摘要

有限的、有界的、多体系统中,相互作用算符(公式:见文)是局部的,并且恰好强烈地支配着动能算符(公式:见文),仅通过对角化(公式:见文)就显示出经典的极限,因此出现了粒子间相关的清晰图景,例如位阻。这个极限表现出内在的对称性和质量公式的波动。这项工作研究了如何将这种涌现的对称性和波动外推到[公式:见文本]恢复的物理情况。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the strong local potential limit
Finite, bound, many-body systems, where the interaction operator, [Formula: see text], is local and happens to strongly dominate the kinetic energy operator, [Formula: see text], display a classical limit from diagonalizing [Formula: see text] alone, hence a clear picture of interparticle correlations, such as steric blocking emerges. This limit exhibits intrinsic symmetries and also fluctuations from mass formulae. This work investigates how such emergent symmetries and fluctuations might be extrapolated to physical situations where [Formula: see text] is reinstated.
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