Preservation of the Bayes Property in the Problem of Estimating Functions of the Mean of the Normal Law

1989 ◽  
Vol 33 (2) ◽  
pp. 399-402
Author(s):  
V. N. Ol’man

1. It is widely felt that any method of rejecting observations with large deviations from the mean is open to some suspicion. Suppose that by some criterion, such as Peirce’s and Chauvenet’s, we decide to reject observations with deviations greater than 4 σ, where σ is the standard error, computed from the standard deviation by the usual rule; then we reject an observation deviating by 4·5 σ, and thereby alter the mean by about 4·5 σ/ n , where n is the number of observations, and at the same time we reduce the computed standard error. This may lead to the rejection of another observation deviating from the original mean by less than 4 σ, and if the process is repeated the mean may be shifted so much as to lead to doubt as to whether it is really sufficiently representative of the observations. In many cases, where we suspect that some abnormal cause has affected a fraction of the observations, there is a legitimate doubt as to whether it has affected a particular observation. Suppose that we have 50 observations. Then there is an even chance, according to the normal law, of a deviation exceeding 2·33 σ. But a deviation of 3 σ or more is not impossible, and if we make a mistake in rejecting it the mean of the remainder is not the most probable value. On the other hand, an observation deviating by only 2 σ may be affected by an abnormal cause of error, and then we should err in retaining it, even though no existing rule will instruct us to reject such an observation. It seems clear that the probability that a given observation has been affected by an abnormal cause of error is a continuous function of the deviation; it is never certain or impossible that it has been so affected, and a process that completely rejects certain observations, while retaining with full weight others with comparable deviations, possibly in the opposite direction, is unsatisfactory in principle.


1933 ◽  
Vol 29 (2) ◽  
pp. 231-234 ◽  
Author(s):  
Harold Jeffreys

Gauss gave a well-known proof that under certain conditions the postulate that the arithmetic mean of a number of measures is the most probable estimate of the true value, given the observations, implies the normal law of error. I found recently that in an important practical case the mean is the most probable value, although the normal law does not hold. I suggested an explanation of the apparent discrepancy, but it does not seem to be the true one in the case under consideration.


1940 ◽  
Vol 60 (1) ◽  
pp. 40-46 ◽  
Author(s):  
A. C. Aitken

It is well known, and fundamentally important in the justification of the current mode of deriving Student's t-distribution, that the mean m of n values xi all obeying the same normal law of probability, and the associated estimate of variance, namelyare statistically independent.


Sensors ◽  
2021 ◽  
Vol 21 (15) ◽  
pp. 4964
Author(s):  
Pavel Prudkovskii ◽  
Andrey Leontyev ◽  
Kirill Kuznetsov ◽  
Galiya Kitaeva

Statistical distributions of the analog readings of an antenna-coupled THz superconducting bolometer were measured and analyzed under a special type of irradiation by low-energy fluxes of THz photons with Poisson photon statistics and controllable mean photon numbers. The photons were generated via low-gain parametric down-conversion in pulse-pumped Mg:LiNbO3 crystal placed to a cooled cryostat together with the bolometer NbN film. Results of theoretical approximation of experimental histograms reveal the discrete nature of THz detection by superconducting bolometers and open a way for studying their quantum characteristics. It is shown that bolometer readings per pulse consist of discrete counts (“single charges”), with the mean number linearly dependent on the number of input photons. Contributions of single counts to a total analog reading are statistically distributed according to the normal law, with average values slightly depending on the number of counts in each reading. A general formula is proposed to describe the relationship between continuous statistical distribution of the bolometer readings and discrete quantum statistics of the incident photons.


2016 ◽  
Vol 2016 (5) ◽  
pp. 115-120
Author(s):  
Ольга Дадыкина ◽  
Olga Dadykina

Silicon carbide black grinding powders 54CF180-F36, mass-produced at Volzhsky Abrasive Plant are studied. Powders are screened into fractions according to GOST R 52381. Measurement of a grain width of each fraction was carried out by means of a photome-tric method using specially developed software. For the vast majority of fractions the grain width follows the normal distribution law. The deviation of the grain width from the normal law can be observed at the frac-tions settled on the second sieve and the pallet. With decreasing the nominal mesh size of a pass sieve in each grit size the arithmetic mean of grain width of the main fraction decreases, dispersion reduces from the fraction settling on the second sieve to the fourth and increases at the fraction settling on the pallet. In case of the identical mesh size of a pass sieve the mean and dispersion of grain width fraction increase with grinding powder grit increase. For each grit size the functional dependences of the mean and dispersion of grain width fraction on a mesh size of a pass sieve are established.


The normal or Gaussian law of error rests partly on a particular hypothesis about the nature of error, that the error of any individual observation is the resultant of a large number of comparable and independent components; and partly on comparison with frequencies in actual series of observations. Both arguments are defective. The theory does not prove that the law is true for errors of any magnitude, even if its fundamental hypothesis is accepted. It involves a number of approximations, and when the effects of these are examined it is found that the law should hold only up to a moderate multiple of the standard error. This is obvious in the simplest case of the binomial distribution, since the normal law predicts a finite though small chance of an error of any amount, but the binomial law is rigidly limited at each end. The assertion of the normal law for errors of any magnitude as the limit of the binomial really assumes that the number of components is infinite, and that all have the same infinitesimal range. This is a very remarkable hypothesis. There may be some inductive reason, in cases where many sources of variation have already been determined and allowed for, to suppose that there are several others just below the magnitude that can be detected separately; but there is every reason to suppose that these are not infinite in number, but merely the largest members of a convergent series, and in such a case there is no reason to suppose that their resultant will tend to the normal law. Whittaker and Robinson give a striking example to the contrary (1924, p. 178), where the components all follow the median law and their magnitudes diminish. Indeed, if there is one dominant component the law for the resultant will approximate to the law for that component separately. Even if there are several equal components the proof may fail. Fisher has shown (1922, p. 321) that if several errors follow the law P (dx/h) (1+x2)-1dx the mean of any number will follow the same law with the same constants.


1973 ◽  
Vol 17 (3) ◽  
pp. 543-547
Author(s):  
A. S. Kholevo

1971 ◽  
Vol 48 (2) ◽  
pp. 339-352 ◽  
Author(s):  
K. Narahari Rao ◽  
R. Narasimha ◽  
M. A. Badri Narayanan

Using a hot wire in a turbulent boundary layer in air, an experimental study has been made of the frequent periods of activity (to be called ‘bursts’) noticed in a turbulent signal that has been passed through a narrow band-pass filter. Although definitive identification of bursts presents difficulties, it is found that a reasonable characteristic value for the mean interval between such bursts is consistent, at the same Reynolds number, with the mean burst periods measured by Kline et al. (1967), using hydrogen-bubble techniques in water. However, data over the wider Reynolds number range covered here show that, even in the wall or inner layer, the mean burst period scales with outer rather than inner variables; and that the intervals are distributed according to the log normal law. It is suggested that these ‘bursts’ are to be identified with the ‘spottiness’ of Landau & Kolmogorov, and the high-frequency intermittency observed by Batchelor & Townsend. It is also concluded that the dynamics of the energy balance in a turbulent boundary layer can be understood only on the basis of a coupling between the inner and outer layers.


2019 ◽  
Vol 73 (4) ◽  
pp. 408-410
Author(s):  
Alexandre Galvão Patriota

Sign in / Sign up

Export Citation Format

Share Document