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arXiv quant-ph/0609157quant-ph
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维格纳分布的信息论意义

Information-theoretic significance of the Wigner distribution

B. Roy Frieden, Bernard H. Soffer

摘要:

一个粗粒度的维格纳分布p_{W}(x,u)服从正性推导出的信息论的考虑。设p(x,u)为纯态粒子位置和动量涨落x,u的未知联合概率密度函数。假设其傅里叶变换F. T. [p(x,u)]=| Z(x,z)|exp[iPsi(x,z)]被构造为全息图。(Such全息图通常用于外差干涉测量法。考虑一个粒子随机地照亮这个相位全息图。测量其两个位置坐标。要求测量值通过相位函数Psi(x,z)的变化包含有关真实位置的极大量Fisher信息。极值解给出输出PDF p(x,u),其是Wigner p_{W}(x,u)与定义位置x或动量u中的不确定性的仪器函数的卷积。卷积自然地从该方法中产生,并且是一维的,与通常用于粗粒度目的的二维卷积相比。如果一维工具函数足够宽,则输出服从正性,如PDF所要求的那样。这一结果适用于一大类系统:那些振幅a(x)在其边界处相同的系统(例如:具有正宇称的状态a(x);具有周期性边界条件;被困在盒子中的自由粒子)。

英文摘要:

A coarse grained Wigner distribution p_{W}(x,u) obeying positivity derives out of information-theoretic considerations. Let p(x,u) be the unknown joint PDF (probability density function) on position- and momentum fluctuations x,u for a pure state particle. Suppose that the phase part Psi(x,z) of its Fourier transform F.T.[p(x,u)]=|Z(x,z)|exp[iPsi(x,z)] is constructed as a hologram. (Such a hologram is often used in heterodyne interferometry.) Consider a particle randomly illuminating this phase hologram. Let its two position coordinates be measured. Require that the measurements contain an extreme amount of Fisher information about true position, through variation of the phase function Psi(x,z). The extremum solution gives an output PDF p(x,u) that is the convolution of the Wigner p_{W}(x,u) with an instrument function defining uncertainty in either position x or momentum u. The convolution arises naturally out of the approach, and is one-dimensional, in comparison with the two-dimensional convolutions usually proposed for coarse graining purposes. The output obeys positivity, as required of a PDF, if the one-dimensional instrument function is sufficiently wide. The result holds for a large class of systems: those whose amplitudes a(x) are the same at their boundaries (Examples: states a(x) with positive parity; with periodic boundary conditions; free particle trapped in a box).

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