wholly dom<strong>in</strong>ates now <strong>the</strong> teach<strong>in</strong>g <strong>of</strong> ma<strong>the</strong>matical analysis <strong>and</strong> anumber <strong>of</strong> o<strong>the</strong>r ma<strong>the</strong>matical discipl<strong>in</strong>es) which sharply separates <strong>the</strong>pert<strong>in</strong>ent contents <strong>in</strong>to ma<strong>the</strong>matical <strong>and</strong> applied parts.At <strong>the</strong> beg<strong>in</strong>n<strong>in</strong>g <strong>of</strong> <strong>the</strong> century textbooks on <strong>the</strong> <strong>the</strong>ory <strong>of</strong>probability had conta<strong>in</strong>ed very many real examples <strong>of</strong> statistical data;<strong>in</strong> <strong>the</strong> new textbooks such examples are disappear<strong>in</strong>g. A naturalprocess <strong>of</strong> demarcat<strong>in</strong>g teach<strong>in</strong>g ma<strong>the</strong>matical <strong>the</strong>ory <strong>and</strong> applicationsis possibly go<strong>in</strong>g on. Indeed, had we wished to <strong>in</strong>clude applications <strong>in</strong>a textbook on ma<strong>the</strong>matical analysis, we would have to expoundmechanics, physics, probability <strong>the</strong>ory <strong>and</strong> much o<strong>the</strong>r material.It is a fact, however, that <strong>the</strong> applications <strong>of</strong> ma<strong>the</strong>matical analysisnaturally f<strong>in</strong>d <strong>the</strong>mselves <strong>in</strong> courses <strong>and</strong> textbooks on mechanics <strong>and</strong>physics, but that <strong>the</strong> applications <strong>of</strong> <strong>the</strong> <strong>the</strong>ory <strong>of</strong> probability, whiledisappear<strong>in</strong>g from textbooks on ma<strong>the</strong>matical sciences, are not yetbe<strong>in</strong>g <strong>in</strong>serted elsewhere. It follows that <strong>the</strong> ma<strong>in</strong> methods <strong>of</strong> properwork with actual data <strong>and</strong>, <strong>in</strong> particular, <strong>of</strong> how to decide whe<strong>the</strong>rsome statistical premises are fulfilled or not, are not <strong>in</strong>cludedanywhere.I have <strong>the</strong>refore thought it appropriate to <strong>in</strong>sert here a part <strong>of</strong> <strong>the</strong>semethods. They are <strong>in</strong>deed constitut<strong>in</strong>g its, so to say, didactical part.All such methods are particular, <strong>and</strong> are described <strong>in</strong> a natural way byconcrete examples. However, <strong>the</strong> <strong>in</strong>clusion <strong>of</strong> a few such examples,that seemed to me important for one or ano<strong>the</strong>r reason, pursues <strong>in</strong>addition ano<strong>the</strong>r <strong>and</strong> more general aim. I attempted to prove that, <strong>in</strong>spite <strong>of</strong> a possible logical groundlessness, a stochastic <strong>in</strong>vestigationcan provide a practically doubtless result. Confidence <strong>in</strong>tervals, criteria<strong>of</strong> significance <strong>and</strong> o<strong>the</strong>r statistical methods to which, <strong>in</strong> particular,Alimov objects, are serv<strong>in</strong>g <strong>in</strong> <strong>the</strong>se examples perfectly well <strong>and</strong> allowus to make def<strong>in</strong>ite practical conclusions. But <strong>of</strong> course, realapplications <strong>of</strong> probability <strong>the</strong>ory both at <strong>the</strong> time <strong>of</strong> Laplace <strong>and</strong>nowadays are <strong>of</strong> a particular <strong>and</strong> concrete type. As to my attitudetowards all-embrac<strong>in</strong>g global constructions, it is sufficiently expressed<strong>in</strong> Chapter 1.2.1. On a new confirmation <strong>of</strong> <strong>the</strong> Mendelian laws. We explicateKolmogorov’s paper (1940) directly connected with <strong>the</strong> discussion <strong>of</strong>biological problems which took place <strong>the</strong>n 18 .At first, some simple <strong>the</strong>oretical <strong>in</strong>formation. Suppose thatsuccessive repetitions <strong>of</strong> an observed event constitute a genu<strong>in</strong>estatistical ensemble <strong>and</strong> its results are values <strong>of</strong> some r<strong>and</strong>om variableξ. The results <strong>of</strong> n experiments are traditionally denotedx 1 , ..., x n (2.1)(not ξ 1 ,..., ξ n ) <strong>and</strong> F n (x) is called <strong>the</strong> empirical distribution function:F x<strong>the</strong> number <strong>of</strong> x < x among all x ,..., x= (2.2)ni1 nn( ) .This function changes by jumps <strong>of</strong> size 1/n at po<strong>in</strong>ts (2.1); for <strong>the</strong>sake <strong>of</strong> simplicity we assume that among those numbers <strong>the</strong>re are noequal to each o<strong>the</strong>r. That function <strong>the</strong>refore depends on <strong>the</strong> r<strong>and</strong>om100
values <strong>of</strong> (2.1) realized <strong>in</strong> <strong>the</strong> n experiments <strong>and</strong> is <strong>the</strong>refore itselfr<strong>and</strong>om. In addition, <strong>the</strong>re exists a non-r<strong>and</strong>om (<strong>the</strong>oretical)distribution functionF(x) = P[ξ < x] = P[x i < x] (2.3)<strong>of</strong> each result <strong>of</strong> <strong>the</strong> experiment.Kolmogorov proved that at n → ∞ <strong>the</strong> magnitudeλ = sup n | F( x) − F ( x) |(2.4)nhas some st<strong>and</strong>ard distribution (<strong>the</strong> Kolmogorov distribution); <strong>the</strong>supremum is taken over <strong>the</strong> values <strong>of</strong> x. This result is valid under as<strong>in</strong>gle assumption that F(x) is cont<strong>in</strong>uous. Now not only <strong>the</strong>asymptotic distribution <strong>of</strong> (2.4) is known, but also its distributions at n= 2, 3, ...The practical sense <strong>of</strong> <strong>the</strong> empirical distribution function F n (x)consists, first <strong>of</strong> all, <strong>in</strong> that its graph vividly represents <strong>the</strong> samplevalues (2.1). In a certa<strong>in</strong> sense this function at sufficiently large values<strong>of</strong> n resembles <strong>the</strong> <strong>the</strong>oretical distribution function F(x). [...]There also exists ano<strong>the</strong>r method <strong>of</strong> representation <strong>of</strong> a samplecalled histogram [...] Given a large number <strong>of</strong> observations, itresembles <strong>the</strong> density <strong>of</strong> distribution <strong>of</strong> r<strong>and</strong>om variable ξ. However, itis only expressive (<strong>and</strong> almost <strong>in</strong>dependent from <strong>the</strong> choice <strong>of</strong> <strong>the</strong><strong>in</strong>tervals <strong>of</strong> group<strong>in</strong>g) for <strong>the</strong> number <strong>of</strong> observations <strong>of</strong> <strong>the</strong> order <strong>of</strong> atleast a few tens. The histogram is more commonly used, but <strong>in</strong> allcases I decidedly prefer to apply <strong>the</strong> empirical distribution function.The Kolmogorov criterion based on statistics λ, see (2.4), can beapplied for test<strong>in</strong>g <strong>the</strong> fit <strong>of</strong> <strong>the</strong> supposed <strong>the</strong>oretical law F(x) to <strong>the</strong>observational data (2.1) represented by function (2.2). However, that<strong>the</strong>oretical law ought to be precisely known. A common (but graduallybe<strong>in</strong>g ab<strong>and</strong>oned) mistake was <strong>the</strong> application <strong>of</strong> <strong>the</strong> Kolmogorovcriterion for test<strong>in</strong>g <strong>the</strong> hypo<strong>the</strong>sis <strong>of</strong> <strong>the</strong> k<strong>in</strong>d The <strong>the</strong>oreticaldistribution function is normal. Indeed, <strong>the</strong> normal law is onlydeterm<strong>in</strong>ed to <strong>the</strong> choice <strong>of</strong> its parameters a (<strong>the</strong> mean) <strong>and</strong> σ (meansquare scatter). In <strong>the</strong> hypo<strong>the</strong>sis formulated just above <strong>the</strong>separameters are not mentioned; it is assumed that <strong>the</strong>y are determ<strong>in</strong>edby sample data, naturally through <strong>the</strong> estimators1x s x xn2 2; = ∑ (i− ) .n −1i=1Thus, <strong>in</strong>stead <strong>of</strong> statistic (2.4), <strong>the</strong> statisticx − xsup n | F0[ ] − Fn( x) |(2.5)sis meant. Here, F 0 is <strong>the</strong> st<strong>and</strong>ard normal law N(0, 1).Statistic (2.5) differs from (2.4) <strong>in</strong> that <strong>in</strong>stead <strong>of</strong> F(x) it <strong>in</strong>cludes F 0which depends on (2.1), x <strong>and</strong> s <strong>and</strong> is <strong>the</strong>refore r<strong>and</strong>om. Typical101
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Studies in the History of Statistic
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Introduction by CompilerI am presen
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(Lect. Notes Math., No. 1021, 1983,
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sufficiently securely that a carefu
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is energy?) from chapter 4 of Feynm
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demand to apply transfinite numbers
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for stating that Ω consists of ele
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chances to draw a more suitable apa
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Let the space of elementary events
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2.3. Independence. When desiring to
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Eξ = ∑ aipi.Our form of definiti
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absolutely precisely if the pertine
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where x is any real number. If dens
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probability can be coupled with an
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Nowadays we are sure that no indepe
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λ = λ(T)with λ(T) being actually
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(1/B n )(m − A n )instead of the
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along with ξ. For example, if ξ i
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µ( − p0) ÷np0 (1 − p0)nhas an
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distribution of the maximal term |s
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ξ (ω) + ... + ξ (ω)n1n{ω :|
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P{max ξ(t) ≥ x} = 0.01, 0 ≤ t
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1. This example and considerations
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IIV. N. TutubalinTreatment of Obser
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