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Reconstruction of Gaussian quantum mechanics from Liouville mechanics with an epistemic restriction

机译:从Liouville力学到认知约束重构高斯量子力学。

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摘要

How would the world appear to us if its ontology was that of classical mechanics but every agent faced anrestriction on how much they could come to know about the classical state? We show that in most respects itnwould appear to us as quantum. The statistical theory of classical mechanics, which specifies how probabilityndistributions over phase space evolve under Hamiltonian evolution and under measurements, is typically callednLiouville mechanics, so the theory we explore here is Liouville mechanics with an epistemic restriction. Thenparticular epistemic restrictionwe posit as our foundational postulate specifies two constraints. The first constraintnis a classical analog of Heisenberg’s uncertainty principle; the second-order moments of position and momentumndefined by the phase-space distribution that characterizes an agent’s knowledge are required to satisfy the samenconstraints as are satisfied by the moments of position and momentum observables for a quantum state. Thensecond constraint is that the distribution should have maximal entropy for the given moments. Starting fromnthis postulate, we derive the allowed preparations, measurements, and transformations and demonstrate thatnthey are isomorphic to those allowed in Gaussian quantum mechanics and generate the same experimentalnstatistics. We argue that this reconstruction of Gaussian quantum mechanics constitutes additional evidence innfavor of a research program wherein quantum states are interpreted as states of incomplete knowledge and thatnthe phenomena that do not arise in Gaussian quantum mechanics provide the best clues for how one mightnreconstruct the full quantum theory.
机译:如果世界的本体论是经典力学的本体,但是每个代理人都可以了解到多少关于经典状态的知识,世界将如何出现在我们眼前?我们证明,在大多数方面,它不会对我们来说是量子的。经典力学的统计理论指定了在哈密顿演化和测量下相空间上的概率分布如何演化,通常被称为利维尔力学,因此我们在这里探讨的理论是具有认识论限制的利维尔力学。然后,作为我们的基本假设,我们提出了特殊的认知约束,它规定了两个约束。第一个约束条件是海森堡不确定性原理的经典比喻。需要由表征代理知识的相空间分布定义的位置和动量的二阶矩来满足与量子状态的位置和动量的矩所满足的相同约束。第二个约束是给定时刻的分布应具有最大熵。从该假设出发,我们得出允许的准备,测量和转换,并证明它们与高斯量子力学允许的同构,并且产生相同的实验统计量。我们认为,高斯量子力学的这种重构构成了一项研究计划的额外证据,该研究计划将量子态解释为不完全知识的状态,并且高斯量子力学中未出现的现象为如何重构完整的量子理论提供了最佳线索。 。

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  • 来源
    《PHYSICAL REVIEW A》 |2012年第1期|1-25|共25页
  • 作者单位

    School of Physics The University of Sydney Sydney New South Wales 2006 Australia;

    Controlled Quantum Dynamics Theory Imperial College London London SW7 2BW United Kingdom;

    Perimeter Institute for Theoretical Physics 31 Caroline Street North Waterloo Ontario Canada N2L 2Y5;

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