二维相互作用玻色子多体激发态中的旋涡

Mateusz Ślusarczyk, Krzysztof Pawłowski
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引用次数: 0

摘要

量子漩涡在二维量子多体系统物理学中扮演着重要角色,尽管它们通常是在单粒子框架(如均场方法)中被理解的。受孤子和漩涡态之间关系研究的启发,我们在此研究了陷于圆盘中相互影响的粒子的 N 体哈密顿的特征态所产生的漩涡。我们分析了通过连续测量粒子位置而出现的状态。这些状态的密度、相位和能量与平均场涡旋非常相似。我们讨论了它们的相似性,但也指出了纯粹的多体特征,例如由于其中心的量子波动而导致的涡旋涂抹。多体系统的 ab initio 分析和均场方法得到了 Bogoliubov 方法分析的支持。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Vortices in the Many-Body Excited States of Interacting Bosons in Two Dimension
Quantum vortices play an important role in the physics of two-dimensional quantum many-body systems, though they usually are understood in the single-particle framework like the mean-field approach. Inspired by the study on the relations between solitons and yrast states, we investigate here the emergence of vortices from the eigenstates of a N -body Hamiltonian of interacting particles trapped in a disk. We analyse states that appear by consecutively measuring the positions of particles. These states have densities, phases, and energies closely resembling mean-field vortices. We discuss similarities, but also point out purely many-body features, such as vortex smearing due to the quantum fluctuation of their center. The ab initio analysis of the many-body system, and mean-field approaches are supported by the analysis within the Bogoliubov approach.
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