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Cauchy distribution probability theory. Cauchy distribution. "koshi distribution" in books

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Cauchy distribution
Probability Density

The green curve corresponds to the standard Cauchy distribution

distribution function

The colors are in accordance with the chart above
Designation \mathrm(C)(x_0,\gamma)
Options x_0- shift factor
\gamma > 0- scale factor
Carrier x \in (-\infty; +\infty)
Probability Density \frac(1)(\pi\gamma\,\left)
distribution function \frac(1)(\pi) \mathrm(arctg)\left(\frac(x-x_0)(\gamma)\right)+\frac(1)(2)
Expected value does not exist
Median x_0
Fashion x_0
Dispersion +\infty
Asymmetry coefficient does not exist
Kurtosis coefficient does not exist
Differential entropy \ln(4\,\pi\,\gamma)
Generating function of moments not determined
characteristic function \exp(x_0\,i\,t-\gamma\,

Definition

Let the distribution of a random variable X given by density f_X(x), having the form:

f_X(x) = \frac(1)(\pi\gamma \left) = ( 1 \over \pi ) \left[ ( \gamma \over (x - x_0)^2 + \gamma^2 ) \right],

  • x_0 \in \mathbb(R)- shift parameter;
  • \gamma > 0- scale parameter.

Then they say that X has a Cauchy distribution and write X \sim \mathrm(C)(x_0,\gamma). If x_0 = 0 And \gamma = 1, then this distribution is called standard Cauchy distribution.

distribution function

F^(-1)_X(x) = x_0 + \gamma\,\mathrm(tg)\,\left[\pi\,\left(x-(1 \over 2)\right)\right].

This allows a sample to be generated from the Cauchy distribution using the inverse transform method.

Moments

\int\limits_(-\infty)^(\infty)\!x^(\alpha)f_X(x)\, dx

not defined for \alpha \geqslant 1, nor the mathematical expectation (although the integral of the 1st moment in the sense of the main value is equal to: \lim\limits_(c \rightarrow \infty) \int\limits_(-c)^(c) x \cdot ( 1 \over \pi ) \left[ ( \gamma \over (x - x_0)^2 + \ gamma^2 ) \right]\, dx = x_0), neither the variance nor the higher-order moments of this distribution have been determined. It is sometimes said that the mathematical expectation is not defined and the variance is infinite.

Other properties

  • The Cauchy distribution is infinitely divisible.
  • The Cauchy distribution is stable. In particular, the sample mean of a sample from a standard Cauchy distribution itself has a standard Cauchy distribution: if X_1,\ldots, X_n \sim \mathrm(C)(0,1), That
\overline(X) = \frac(1)(n) \sum\limits_(i=1)^n X_i \sim \mathrm(C)(0,1)

Relationship with other distributions

  • If U \sim U, That
x_0 + \gamma\,\mathrm(tg)\,\left[\pi\left(U-(1 \over 2)\right)\right] \sim \mathrm(C)(x_0,\gamma).
  • If X_1, X_2 are independent normal random variables such that X_i \sim \mathrm(N)(0,1),\; i=1,2, That
\frac(X_1)(X_2) \sim \mathrm(C)(0,1).
  • The standard Cauchy distribution is a special case of Student's distribution:
\mathrm(C)(0,1) \equiv \mathrm(t)(1).

Appearance in practical problems

  • The Cauchy distribution characterizes the length of the segment cut off on the abscissa by a straight line fixed at a point on the y-axis if the angle between the line and the y-axis has a uniform distribution on the interval (−π; π) (i.e. the direction of the line is isotropic on the plane).
  • In physics, the Cauchy distribution (also called the Lorentz form) describes the profiles of uniformly broadened spectral lines.
  • The Cauchy distribution describes the amplitude-frequency characteristics of linear oscillatory systems in the vicinity of resonant frequencies.
P Probability distributions
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Discrete: Bernoulli | Binomial | Geometric | Hypergeometric | Logarithmic | Negative binomial | Poisson | Discrete Uniform Multinomial
Absolutely continuous: Beta | Weibulla | Gamma | Hyperexponential | Gompertz distribution | Kolmogorov | Cauchy| Laplace | Lognormal | Normal (Gaussian) | Logistics | Nakagami | Pareto | Pearson | | Exponential | Variance-gamma Multidimensional normal | copula

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An excerpt characterizing the Cauchy Distribution

Rostov gave the spurs to his horse, called out to non-commissioned officer Fedchenko and two more hussars, ordered them to follow him, and rode at a trot downhill in the direction of the continuing screams. Rostov was both terribly and merry to go alone with three hussars there, to this mysterious and dangerous foggy distance, where no one had been before him. Bagration shouted to him from the mountain so that he would not go further than the stream, but Rostov pretended not to hear his words, and, without stopping, rode on and on, constantly deceived, mistaking bushes for trees and potholes for people and constantly explaining his deceptions. Having trotted downhill, he no longer saw either ours or the enemy's fires, but he heard the cries of the French louder and clearer. In the hollow he saw something like a river in front of him, but when he reached it, he recognized the road he had traveled. Riding out onto the road, he held his horse back, undecided whether to ride on it or cross it and ride uphill across the black field. It was safer to drive along the road brightened in the fog, because people could be seen more quickly. “Follow me,” he said, crossed the road and began to gallop up the mountain, to the place where the French picket had been standing since evening.
“Your Honor, here it is!” one of the hussars spoke from behind.
And before Rostov had time to make out something suddenly blackened in the fog, a light flashed, a shot clicked, and the bullet, as if complaining about something, buzzed high in the fog and flew out of hearing. The other gun did not fire, but a light flashed on the shelf. Rostov turned his horse and galloped back. Another four shots rang out at different intervals, and bullets sang in different tones somewhere in the fog. Rostov reined in his horse, which had cheered up just as much as he did from the shots, and rode off at a pace. "Well, more, well, more!" a cheerful voice spoke in his soul. But there were no more shots.
Just approaching Bagration, Rostov again put his horse into a gallop and, holding his hand at the visor, rode up to him.
Dolgorukov kept insisting on his opinion that the French had retreated and only in order to deceive us they had put out fires.
– What does this prove? - he said at the time when Rostov drove up to them. “They could have retreated and left the pickets.
- Apparently, not everyone has left yet, prince, - said Bagration. Until tomorrow morning, we'll find out tomorrow.
“There is a picket on the mountain, Your Excellency, everything is the same as it was in the evening,” Rostov reported, leaning forward, holding his hand at the visor and unable to restrain the smile of fun caused in him by his trip and, most importantly, by the sounds of bullets.
“Good, good,” said Bagration, “thank you, Mr. Officer.
“Your Excellency,” said Rostov, “permit me to ask you.
- What's happened?
- Tomorrow our squadron is assigned to the reserves; let me ask you to attach me to the 1st squadron.
- What's your last name?
- Count Rostov.
- Oh good. Stay with me as an orderly.
- Ilya Andreich's son? Dolgorukov said.
But Rostov did not answer him.
“So I hope, Your Excellency.
- I'll order.
“Tomorrow, very possibly, they will send some kind of order to the sovereign,” he thought. - God bless".

The cries and fires in the enemy army came from the fact that while the order of Napoleon was being read to the troops, the emperor himself was riding around his bivouacs. The soldiers, seeing the emperor, lit bunches of straw and, shouting: vive l "empereur!, ran after him. Napoleon's order was as follows:
"Soldiers! The Russian army comes out against you to avenge the Austrian, Ulm army. These are the same battalions which you defeated at Gollabrunn and which you have been constantly pursuing to this place ever since. The positions we occupy are powerful, and as long as they go to get around me on the right, they will expose me to the flank! Soldiers! I myself will lead your battalions. I will keep far from the fire if you, with your usual courage, bring disorder and confusion into the ranks of the enemy; but if victory is even for a moment doubtful, you will see your emperor exposed to the first blows of the enemy, because there can be no hesitation in victory, especially on a day when the honor of the French infantry, which is so necessary for the honor of his nation, is at stake.

Physical Encyclopedia

CAUCHI DISTRIBUTION

CAUCHI DISTRIBUTION

Probability distribution with density

and distribution function

Shift parameter, >0 - scale parameter. Reviewed in 1853 by O. Cauchy. characteristic function K. r. equal to exp ; moments of order R 1 do not exist, so law of large numbers for K. r. fails [if X 1 ..., X n are independent random variables with the same K. r., then n -1 (X 1 + ... + X n) has the same K. r.]. Family K. r. closed under linear transformations: if the random variable X has a distribution (*), then aX+b also has K. r. with parameters , . K. r.- sustainable distribution with exponent 1, symmetrical about a point x=. K. r. has, for example, the relationship X/Y independent normally distributed random variables with zero means, as well as a function , where the random variable Z evenly distributed over . They also consider multidimensional analogs of K. r.

Lit.: V. Feller, Introduction to probability theory and its applications, trans. from English, vol. 2, M., 1984.

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"KOSHI DISTRIBUTION" in books

Distribution

From the book Memories and Reflections on the Past author Bolibrukh Andrey Andreevich

Distribution Long before graduating from graduate school, I decided on the choice of my future profession, deciding to become a teacher of mathematics at a university. I quite consciously did not want to go to work in any research institute, guided by the following two

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37. Koshas and Chakras To deeply understand the meaning of pranayama in all its dimensions, which goes far beyond purely physiological limits, it is necessary to know the fundamental principles of Indian philosophy. However, I dare to assure Western readers that here they will not meet with

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5. Maxwell distribution (velocity distribution of gas molecules) and Boltzmann

From the book Medical Physics author Podkolzina Vera Alexandrovna

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Cauchy

From the book Encyclopedic Dictionary (K) author Brockhaus F. A.

author TSB

Cauchy distribution

TSB

Cauchy theorem

From the book Great Soviet Encyclopedia (KO) of the author TSB

Augustin Cauchy

author Duran Antonio

Augustin Cauchy In the first half of the 19th century, a clear foundation for the analysis of infinitesimals was finally formed. The solution of this problem was started by Cauchy and completed by Weierstrass. Significant contributions were also made by Bernard Bolzano with his papers on continuous functions that go beyond

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From the book Truth in the Limit [Infinitesimal Analysis] author Duran Antonio

Euler, Cauchy, and the Aesthetic Value of Mathematics We should also talk about the aesthetic beginning, because, contrary to the opinion of many, aesthetics is not only not alien to mathematics, but also constitutes a significant part of it. The title of this chapter - "Tamed infinitesimals" - indicates that

It would seem that the Cauchy distribution looks very attractive for describing and modeling random variables. However, in reality this is not the case. The properties of the Cauchy distribution are sharply different from those of the Gaussian, Laplace, and other exponential distributions.

The fact is that the Cauchy distribution is close to the flattest. Recall that a distribution is said to be extremely gentle if, as x -> + oo, its probability density

For the Cauchy distribution, there is not even the first initial moment of the distribution, that is, the mathematical expectation, since the integral defining it diverges. In this case, the distribution has both a median and a mode, which are equal to the parameter a.

Of course, the variance of this distribution (the second central moment) is also equal to infinity. In practice, this means that the estimate of the variance for a sample of the Cauchy distribution will increase indefinitely with the increase in the amount of data.

It follows from the above that the approximation by the Cauchy distribution of random processes , which are characterized by a finite mathematical expectation and a finite variance, is invalid.

So, we have obtained a symmetrical distribution depending on three parameters, which can be used to describe samples of random variables, including those with gentle slopes. However, this distribution has disadvantages, which were considered when discussing the Cauchy distribution, namely, the mathematical expectation exists only for a > 1, the variance is finite only for OS > 2, and in general, the final moment of the k-th order distribution exists for a > k .

Figure 14.1 uses 8,000 samples from the known Cauchy distribution, which has an infinite mean and variance. The Cauchy distribution is described in more detail below. The series used here has been "normalized" by subtracting the mean and dividing by the sample standard deviation. Thus, all units are expressed in standard deviations. For comparison, we use 8,000 Gaussian random variables that have been normalized in a similar way. It is important to understand that the next two steps will always end up with a mean of 0 and a standard deviation of 1 because they have been normalized to these values. Convergence means that the time series is rapidly moving towards a stable value.

These two well-known distributions, the Cauchy distribution and the normal distribution, have many uses. They are also the only two members of the family of stable distributions for which probability density functions can be explicitly derived. In all other fractional cases, they must be evaluated, usually by numerical means. We will discuss one of these methods in a later section of this chapter.

In Chapter 14, we examined the serial standard deviation and mean of the US stock exchange and compared it with the time series derived from the Cauchy distribution. We did this to see the effect of infinite variance and mean on the time series. Sequential standard deviation - the standard deviation of the time series when we add at a time

Make a first approximation of Z to u(o,F) by taking the weighted mean of the F quantiles of the Cauchy and Gaussian distributions.

Table A3.2 converts the results of Table A3.1 into quantiles. To find out which value of F explains 99 percent of the observations for a=1.0, move down the F column to the left to 0.99 and across to u=31.82. The Cauchy distribution requires observations of 31.82 s from the mean to cover 99 percent of the probability. In contrast, the normal case reaches the 99% level at u=3.29. This differs from the standard normal case, which is 2.326 standard deviations rather than 3.29 s.

P(> (nm)1/2T(n/2) n For n = 1, the corresponding distribution is called the Cauchy distribution.

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At the same time, in the general case, even if some random variables X, . .., X are mutually independent and have the same distribution, this does not mean that they form a white noise process, since the random variable Xt may simply have no mean and/or variance (we can again point to the Cauchy distribution as an example).

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Such long-tailed distributions, especially in Pareto data, led Levy (1937), a French mathematician, to formulate a generalized density function , of which normal distributions were special cases, as well as Cauchy distributions. Levy used a generalized version of the Central Limit Theorem. These distributions correspond to a large class of natural phenomena, but they have received little attention because of their unusual and seemingly intractable problems. Their unusual properties continue to make them unpopular, but their other properties are so close to our results in the capital markets that we must investigate them. In addition, the stable Levy distributions have been found to be useful in describing the statistical properties of turbulent flow and l/f noise - and besides, they are fractal.

Figure 14.2(a) shows the sequential standard deviation for the same two series. Sequential standard deviation, like serial mean, is a calculation of the standard deviation as observations are added one at a time. In this case, the difference is even more striking. Random Eyad quickly converges to a standard deviation of 1. The Cauchy distribution, in contrast, never converges. Instead, it is characterized by several large intermittent jumps and large deviations from the normalized value of 1.

This is the logarithm of the characteristic function for the Cauchy distribution, which is known to have infinite variance and mean. In this case, 8 becomes the median of the distribution, and c becomes the seven-interquartile range.

Holt and Crow (1973) found a probability density function for a = 0.25 - 2.00 and P between -1.00 and +1.00, both in increments of 0.25. The methodology they used interpolated between known distributions, such as the Cauchy and normal distributions, and the integral representation from Zolotarev's work (Zolotarev, 1964/1966). Tables prepared for the former

As we discussed in Chapter 14, explicit expressions for stable distributions exist only for special cases of normal and Cauchy distributions. However, Bergstrom (1952) developed the series expansion that Famay and Roll used to approximate densities for many values ​​of alpha. When a > 1.0, they could use Bergstrom's results to derive the next convergent series

CAUCHY DISTRIBUTION, the probability distribution of a random variable X, having a density

where - ∞< μ < ∞ и λ>0 - parameters. The Cauchy distribution is unimodal and symmetrical with respect to the point x = μ, which is the mode and median of this distribution [figures a and b show graphs of the density p(x; λ, μ) and the corresponding distribution function F (x; λ, μ) for μ =1 ,5 and λ = 1]. The mathematical expectation of the Cauchy distribution does not exist. The characteristic Cauchy function of the distribution is e iμt - λ|t| , -∞< t < ∞. Произвольное Коши распределение с параметрами μ и λ выражается через стандартное Коши распределение с параметрами 0 и 1 формулой

If independent random variables X 1 ,...,X n have the same Cauchy distribution, then their arithmetic mean (X 1 + ... + X n)/n for any n = 1,2, ... has the same distribution; this fact was established by S. Poisson (1830). The Cauchy distribution is a stable distribution. The ratio X/Y of independent random variables X and Y with a standard normal distribution has a Cauchy distribution with parameters 0 and 1. The distribution of the tangent tg Z of a random variable Z, with a uniform distribution on the interval [-π/2, π/2], also has a Cauchy distribution with parameters 0 and 1. The Cauchy distribution was considered by O. Cauchy (1853).