Communication theory and physics

D. Gabor
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引用次数: 94

Abstract

The electromagnetic signals used in communication are subject to the general laws of radiation. One obtains a complete representation of a signal by dividing the time-frequency plane into cells of unit area and associating with every cell a "ladder" of distinguishable steps in signal intensity. The steps are determined by Einstein's law of energy fluctuation, involving both waves and photons. This representation, however, gives only one datum per cell, viz. the energy, while in the classical description one has two data; an amplitude and a phase. It is shown in the second part of the paper that both descriptions are practically equivalent in the long-wave region, or for strong signals, as they contain approximately the same number of independent, distinguishable data, but the classical description is always a little less complete than the quantum description. In the best possible experimental analysis the number of distinguishable steps in the measurement of amplitude and phase is only the fourth root of the number of photons. Thus it takes a hundred million photons per cell in order to define amplitude and phase to one percent each.
通信理论与物理
用于通信的电磁信号受一般辐射规律的约束。通过将时频平面划分为单位面积的单元,并将每个单元与信号强度可区分步骤的“阶梯”相关联,可以得到信号的完整表示。这些步骤是由爱因斯坦的能量涨落定律决定的,包括波和光子。然而,在这种表述中,每个细胞只给出一个数据,即能量,而在经典的描述中,每个细胞有两个数据;一个振幅和一个相位。本文第二部分表明,这两种描述在长波区域或强信号中实际上是等效的,因为它们包含大约相同数量的独立的、可区分的数据,但经典描述总是比量子描述更不完整。在最好的实验分析中,在测量振幅和相位时可区分的步骤数仅为光子数的四分之一。因此,每个细胞需要1亿个光子才能将振幅和相位分别定义为1%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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