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Wigner functions, signed particles, and the harmonic oscillator

机译:威格纳函数,有符号粒子和谐波振荡器

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In this paper, we introduce the simple harmonic oscillator and we address it in the Wigner formulation of quantum mechanics, therefore describing the whole problem in terms of quasi-distribution functions defined over the phase-space. The harmonic oscillator represents a very important problem as it provides exact solutions in both stationary and transient regimes. Subsequently, we outline the time-dependent signed particle Wigner Monte Carlo method and simulate the oscillator problem starting from stationary initial conditions, i.e. rotationally invariant functions in the phase-space, showing no evolution in time of the distribution function as expected. This work is, thus, twofold. On the one hand, one may see it as a short review effort to demonstrate the convenience of utilizing a phase-space approach in this particular context, suggesting that it could be the case again for different interesting problems. On the other hand, it represents a further opportunity to validate the signed particle Monte Carlo method, showing that a new reliable and powerful tool is available for the time-dependent simulation of quantum systems.
机译:在本文中,我们介绍了简单的谐振子,并在量子力学的Wigner公式中对其进行了介绍,因此根据在相空间上定义的拟分布函数来描述整个问题。谐波振荡器代表了一个非常重要的问题,因为它提供了稳态和瞬态两种状态下的精确解决方案。随后,我们概述了与时间有关的有符号粒子Wigner蒙特卡洛方法,并从固定的初始条件(即相空间中的旋转不变函数)开始模拟了振荡器问题,表明分布函数的时间没有预期的演变。因此,这项工作是双重的。一方面,可以将它看作是简短的回顾工作,以证明在这种特定情况下利用相空间方法的便利性,这表明对于其他有趣的问题也可能再次出现。另一方面,它为验证有符号粒子蒙特卡罗方法提供了进一步的机会,表明有一个新的可靠而强大的工具可用于时间依赖的量子系统仿真。

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