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Gaussian wave packets in phase space: The Fermi g(F) function

机译:相空间中的高斯波包:费米g(F)函数

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A pure quantum state can be equivalently represented by means of its wave function psi(q) or by the Fermi function g(F)(q,p), with q and p coordinates and conjugate momenta of the system of interest. We show that a Gaussian wave packet can be conveniently visualized in phase space by the curve g(F)(q,p)=0. The change in time of the g(F)=0 curve is calculated for a Gaussian packet evolving freely or under a constant or a harmonic force, and the spreading or shrinking of the packet is easily interpreted in phase space. We also discuss a gedanken prism microscope experiment for measuring the position-momentum correlation. This gedanken experiment, together with the well-known Heisenberg microscope and von Neumann velocimeter, is sufficient to fully determine the state of a Gaussian packet.
机译:纯量子态可以通过其波函数psi(q)或费米函数g(F)(q,p)等价表示,具有相关系统的q和p坐标以及共轭矩。我们表明,曲线g(F)(q,p)= 0可以方便地在相空间中可视化高斯波包。对于自由地或在恒定或谐波力作用下演化的高斯包,计算g(F)= 0曲线的时间变化,并且很容易在相空间中解释包的扩展或收缩。我们还讨论了用于测量位置动量相关性的更根肯棱镜显微镜实验。此实验与著名的海森堡显微镜和冯·诺依曼测速仪一起,足以完全确定高斯包的状态。

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