one on another, as well as the corresponding tool of n-dimensional Stieltjes integrals, <strong>and</strong> healso essentially supplemented {the theory of} limit theorems.In our time, the Chebyshev, Markov <strong>and</strong> Liapunov direction outlined above culminated inBernstein’s investigations (1925 – 1926) who was the first to prove the mainmultidimensional limit theorem <strong>and</strong> to provide the most thorough <strong>and</strong> deep study ofsequences of dependent variables.Recalling that mechanics does not restrict its objects by considering systems of a finitenumber of material points, it would have certainly been unnatural to suppose that the theoryof probability will not go beyond the patterns that only study a finite number of r<strong>and</strong>omvariables. Excluding Bachelier (1900), who remained misunderstood, not puremathematicians but physicists (Smoluchowski, Fokker, Planck), biologists (Fisher) 1 ,actuaries (Lundberg) <strong>and</strong> those applying statistics to technology (Fry) originated widerinvestigations. All their studies may be regarded as particular cases of a general theory ofstochastic processes, that is, of a general theory of r<strong>and</strong>om changes of the states of somesystem in time.Already when the state of a studied system is determined at each given moment t by thecorresponding value of a single parameter x, this latter, if understood as a function x(t) oftime, provides an example of a r<strong>and</strong>om function. Other applications of such functions are yetvery little developed, but it seems likely that they ought to be very numerous <strong>and</strong> important,in particular for the theory of r<strong>and</strong>om oscillations, for the construction of a statistical theoryof turbulence <strong>and</strong> in quantum physics. In all these applications, the state of a system at eachgiven moment is described by some function of a certain number of arguments; <strong>and</strong>, since thevery state of the system is r<strong>and</strong>om, we deal with some r<strong>and</strong>om function already at each fixedt.The study of r<strong>and</strong>om functions <strong>and</strong>, therefore, of distributions in functional spaces,inevitably leads to a certain revision of the axiomatic basis of the theory of probability. Asufficiently general axiomatic exposition of the fundamentals of the theory, satisfying all therequirements of modern physics <strong>and</strong> other applied fields, was created during the last decade.The guiding principle of a considerable part of the pertinent studies was, however, not thedesire to cover a wide range of new applications going beyond the old boundaries, but thewish to trace, in all their generality, the recently discovered deep similarities between anumber of notions of the theory of probability <strong>and</strong> the metric theory of functions of a realvariable.The formulation of new problems led also to the creation of new analytic tools, such as,first, integral, differential <strong>and</strong> integro-differential equations of stochastic processes thatoriginated as a generalization of the Smoluchowski integral equation <strong>and</strong> the Fokker – Planckdifferential equation. And the second side of the new machinery should be the still very littledeveloped theory of characteristic functions <strong>and</strong> moments for distributions in infinitedimensional(in particular, in functional) spaces. We note in concluding that the differential<strong>and</strong> integro-differential equations of stochastic processes led to the construction of a verypowerful method for proving limit theorems which directly adjoin the studies of theChebyshev direction.We can now systematize the new currents in the theory of probability which is the aim ofmy report.1) Investigations that originated owing to the analogy with the metric theory of functionsof a real variable.a) The general axiomatics of the theory of probability (Borel, Fréchet, Kolmogorov,Hopf).b) Research connected with the law of large numbers (Borel, Cantelli, Slutsky, Fréchet,Khinchin, Kolmogorov, Glivenko, Lévy).2) New patterns created owing to the physical <strong>and</strong> other applied issues.
a) The theory of stochastic processes (Finetti, Hostinsky, Hadamard, Mises, Kolmogorov,Fréchet, Khinchin, Lévy).b) The theory of r<strong>and</strong>om functions (Wiener, Slutsky, Lévy).3) New analytic toolsa) Equations of stochastic processes (Kolmogorov, Hostinsky, Fréchet, Bernstein,Pontriagin).b) Characteristic functions <strong>and</strong> moments in infinite-dimensional <strong>and</strong> functional spaces(Khinchin).c) New methods of proving limit theorems (Kolmogorov, Petrovsky, Bernstein, Khinchin,Bavli).1a. As stated above, all the problems of probability theory considered up to the lastdecades can be reduced to the study of a finite number of r<strong>and</strong>om variables. All theprobabilities encountered here will be determined if we provide an n-dimensional distributionfunction of these variables. In particular, Mises, in his course in the theory of probability(1931), systematically kept to the mentioned restriction. In his terminology, this wasexpressed by assuming that the set of indications (Merkmalmenge) of an arbitrary collectivewas always a set of points of an n-dimensional space.It is the most natural to perceive a distribution function in an n-dimensional space as anadditive function in a domain of that space. The mathematical interpretation of a problem inthe theory of probability of the indicated classical type depends exclusively on thecorresponding distribution function. Therefore, if the only aim of the axiomatic theory ofprobability is the most compact <strong>and</strong> clear enumeration of the logical assumptions ofsubsequent mathematical constructions, then, when dealing with problems of the classicaltype, it would be simplest to select directly as the axioms the characteristic properties ofdistribution functions (non-negativity; additivity; <strong>and</strong> their being equal to 1 for the completespace). According to my deep conviction, the axiomatics of probability theory cannot haveany other goals because the question about the applicability of a given mathematical patternto some concrete physical phenomena cannot in essence be solved by the axiomatic method.Mises’ attempt clearly illustrates this idea. To confine his construction within the boundariesof fixed axioms, he is compelled only to postulate the approach of the frequencies to certainlimits as the trials are unboundedly continued, without saying anything about when,beginning with what finite number of repetitions, may we conclude that the formerpractically coincide with the latter. Indeed, an answer to this question can only be providedafter going beyond the boundaries of a rigorously formal mathematical thinking. Thus, theMises axioms, irrespective of the connected intrinsic difficulties, are, one the one h<strong>and</strong>, notneeded for justifying the mathematical theory, <strong>and</strong> insufficient for substantiating itsapplicability on the other h<strong>and</strong>.My system of axioms [1] is a direct generalization of the properties of distributionfunctions listed above. This generalization allows us to cover all those new non-classicalproblems described in the Introduction. I only indicate here one point concerning theaxiomatic construction of the main notions of the theory of probability, – that point, which,as it seems to me, still requires to be developed.In the applications, researchers often consider conditional probabilities which aredetermined under the restriction that some r<strong>and</strong>om variable x took a definite particular valuex = a. If x has a continuous law of distribution, the elementary method of determining theconditional probability P x=a (A) of event A given that x = a,P x=a (A) = P(A|x = a)/P(x = a),
- Page 4 and 5: [3] I bear in mind the well-known p
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described, from the viewpoint that
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conditional variance and determined
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Romanovsky [45] and Kolmogorov [46]
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Let S be the general population wit
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Part 1. Russian/Soviet AuthorsAmbar
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2. On necessary and sufficient cond
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Gnedenko, B.V., Groshev, A.V. 1. On
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52. ( (Mathematical Principl
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Kozuliaev, P.A. 1. Sur la répartit
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Obukhov, A.M. 1. Normal correlation
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30. Généralisations d’un théor
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22. Alcune applicazioni dei coeffic
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10. A.N. Kolmogorov. The Theory of
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Kuznetsov, Stratonovich & Tikhonov
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In the homogeneous case H s t = H t
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to such a generalization. He only s
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In the particular case of a charact
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as it is usual for the modern theor
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1. {The second reference to Pugache
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Smirnov, Romanovsky and others made
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determined the precise asymptotic c
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for finite values of N, M and R 2 .
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Mikhalevich’s findings by far exc
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Uch. Zap. = Uchenye ZapiskiUkr = Uk
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Khinchin, A.Ya. 43. Math. Ann. 101,
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7. DAN 115, 1957, 49 - 52.Pinsker,
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Anderson, T.W., Darling, D.A. (1952
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Statistical problems in radio engin
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observations for its power with reg
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securing against mistakes (A.N. Kry
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of the others, then its distributio
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In Kiev, in the 1930s, N.M. Krylov