Most of the quadratic systems are closely connected with the observation of some physical quantity, since the observation essentially coincides with the weighted mean operation in some sense, in view of the fact that an information obtained from the crude physical phenomenon through the observation is a certain mean image. Form of the mean operation (especially the weight function) will be steadily improved with the progress of science. At the stage where the effect of observation on the crude fluctuation is unknown yet, however, a mean squaring operation in the special form seems to be the most natural one to take. The above physical quantity may be random or have a well-defined representation in time, accompanied by noise which interferes with measurement. Quite apart from the instrument problem of realizing a optimum stable detector, there is an inherent limit to the precision of any measurement performed in a finite time, owing to the random nature of noise power itself. A typical input to the mean squaring system is considered as acombination of normal random noise and a regular signal with a definite structure. The random input process is considered to be the noise and signal generated by stationary process, and it will be further assumed that the random input noise has Gaussian probabilityd istribution.
The focus of this paper is to find out how the output probability distributions of signal and noise are given after mean squaring rectification. The above output fluctuation is treated as a probability problem of “distance” in an
N-dimensional function space with
N=2
TW (
W: frequency interval,
T: time interval), where the distance is taken as the mean squared fluctuation. From this point of view, many explicit expressions of probability density distribution for normal random noise and a regular signal, after passing a mean squaring circuit and an audio band-pass filter of arbitrary width, are experimentally and theoretically derived in connection with the sampling theorem. In this case, the output fluctuation is reasonably expressed by one ripple parameter
m. This parameter
m is proved to be approximately equivalent to
TW expressed in the samplingtheorem.
The experimental and theoretical results described in this paper are also applicable to the other fields of measurement on random phenomena, since the mean energy (taking a mean squaring form) is a universal physical quantity.
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