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7. Probability and Statistics Soviet Essays - Sheynin, Oscar

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Kuznetsov, Stratonovich & Tikhonov [18; 20; 21] called the factors a n <strong>and</strong> b n momentous<strong>and</strong> correlational functions respectively. They began to realize a wide program of applyingthis tool to solving concrete problems (also see Cherenkov [1]).A more elementary theory only using the first moments A 1 (f) <strong>and</strong> B 1 (f) <strong>and</strong> the secondcentral moments B 2 (f) is widely applied in contributions to technical sciences. The quadraticfunctional B 2 (f) is reduced to a sum of squares by an adequate choice of the coordinates; thisis simply Pugachev’s canonical expansion [13]. Pugachev’s book [21] summarizes theeffective methods <strong>and</strong> the experience in applying the theory of r<strong>and</strong>om functions inengineering 1 .The theory of distributions in infinite-dimensional linear spaces, when compared with thetheory of finite-dimensional distributions, suffers from some defects. Thus, not anycontinuous positive-definite functional H(f) having H(0) = 1 is a characteristic functional ofsome distribution. Even for the Hilbert space the additional conditions which should haveensured the existence of a corresponding distribution remain scarcely effective. This factdoes not, however, persist in the theory of generalized r<strong>and</strong>om functions also having manydirect applications. A number of findings pertaining to the theory of generalized functionswere contained in Gelf<strong>and</strong>’s short note [65].2. Stationary Processes <strong>and</strong> Homogeneous R<strong>and</strong>om FieldsWe (G&K, §§4.3 – 4.4) briefly mentioned the works of Khinchin, Kolmogorov, Zasukhin<strong>and</strong> Krein on the spectral theory of stationary processes. During that previous period themain achievements were as follows. The contributions of Slutsky on stationary sequences<strong>and</strong> Wiener’s general harmonic analysis brought about the underst<strong>and</strong>ing that stationarity ofa process automatically leads to the possibility of a spectral representation. Khinchin [72]provided an appropriate harmonious <strong>and</strong> very simple general spectral theory of stationary (inthe wide sense) processes that initiated a large section of the modern theory of probability.Kolmogorov remarked that from a formal mathematical point of view this theory was a directcorollary of the spectral theory of one-parameter groups of unitary operators. This enabledhim to offer a simple exposition of the findings of Khinchin <strong>and</strong> Cramér, <strong>and</strong> to construct,issuing from the works of Wold, a spectral theory of extrapolation <strong>and</strong> interpolation ofstationary sequences [84; 90; 92].After its continuous analogue was discovered; <strong>and</strong> after itwas supplemented with the somewhat later Wiener theory of filtration, it acquired essentialimportance for radio engineering <strong>and</strong> the theory of regulation. Kolmogorov [85; 86] providedthe theory of processes with stationary increments in a geometric form. Zasukhin [1] solvedsome problems of the many-dimensional spectral theory (see a modern explication of hisfindings in Rosanov (1958)). Finally, Krein [85] offered the abovementioned continuousversion of the theory of extrapolation. In particular, he established that the divergence of theintegral+∞log1+− ∞f ( λ)d λ2λwith f() being the spectral density was necessary <strong>and</strong> sufficient for singularity (i.e., for thepossibility of precise extrapolation). Yaglom’s essay [12] described the further developmentof the spectral theory of stationary processes up to 1952. Krein [134] <strong>and</strong> Yaglom [11; 15;19] devoted their writings to issues in extrapolation <strong>and</strong> filtration for stationary onedimensionalprocesses. Rosanov [2; 3] studied the many-dimensional case for sequences 2 ; inparticular, he discovered an effective necessary <strong>and</strong> sufficient condition for the possibility of

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