also <strong>the</strong> operations <strong>of</strong> various devices <strong>and</strong> systems. I also underst<strong>and</strong>prediction as design<strong>in</strong>g all k<strong>in</strong>ds <strong>of</strong> <strong>in</strong>struments, devices, systems etc.You can say that a forecast as a dem<strong>and</strong> <strong>of</strong> reproduc<strong>in</strong>g a publishedresult was be<strong>in</strong>g accepted as a def<strong>in</strong>ition <strong>of</strong> <strong>the</strong> f<strong>in</strong>al aim <strong>and</strong>dist<strong>in</strong>ctive feature <strong>of</strong> natural science even at <strong>the</strong>ir birth.That dem<strong>and</strong> apparently <strong>in</strong>cludes <strong>the</strong> most essential dist<strong>in</strong>ctionbetween natural science <strong>and</strong> magic. It should be regrettably stated thatforecast<strong>in</strong>g as <strong>the</strong> f<strong>in</strong>al aim <strong>of</strong> <strong>the</strong> <strong>the</strong>ories <strong>of</strong> natural science has partlyescap<strong>in</strong>g <strong>the</strong> attention <strong>of</strong> even <strong>the</strong> scientists <strong>the</strong>mselves. It seems thatthis circumstance causes <strong>the</strong> passion felt sometimes for such diffuseformulations <strong>of</strong> those goals <strong>of</strong> scientific research which are sometimesnoticeable as explanation or reveal<strong>in</strong>g <strong>the</strong> essence <strong>of</strong> phenomena.As an example I can cite <strong>the</strong> caustically <strong>in</strong>dicated (Kitaigorodsky1978) tendency <strong>of</strong> chemists to expla<strong>in</strong> a phenomenon with highprecision by <strong>in</strong>troduc<strong>in</strong>g after <strong>the</strong> event plenty adjust<strong>in</strong>g parameters<strong>in</strong>to formulas. A proper number <strong>of</strong> <strong>the</strong>se can always achieve an idealco<strong>in</strong>cidence <strong>of</strong> <strong>the</strong> <strong>the</strong>oretical <strong>and</strong> <strong>the</strong> empirical curves, only not before<strong>the</strong> latter was experimentally obta<strong>in</strong>ed.Kitaigorodsky (1978) <strong>of</strong>fered a formula for quantitatively <strong>in</strong>dicat<strong>in</strong>g<strong>the</strong> value P <strong>of</strong> a <strong>the</strong>ory: P = (k/n) − 1. Here, k is <strong>the</strong> number <strong>of</strong>magnitudes which can be predicted by that <strong>the</strong>ory, <strong>and</strong> n, <strong>the</strong> number<strong>of</strong> adjust<strong>in</strong>g parameters. The value <strong>of</strong> a <strong>the</strong>ory is <strong>the</strong>refore non-existentif k = n, <strong>and</strong> it is essential if k is much greater than n. The reader willbe certa<strong>in</strong>ly justified to believe that this proposal is a joke, but <strong>of</strong> ak<strong>in</strong>d that <strong>in</strong>cludes a large part <strong>of</strong> truth.A somewhat exaggerated stress on <strong>the</strong> idea <strong>of</strong> forecast<strong>in</strong>g noticeable<strong>in</strong> <strong>the</strong> newest discipl<strong>in</strong>e (Prognostika 1975/Prognostication 1978) islikely a reaction to <strong>the</strong> mentioned partial disregard <strong>of</strong> that fundamentalidea. In this connection I <strong>in</strong>dicate once more that <strong>in</strong> any concretebranch <strong>of</strong> natural science forecast<strong>in</strong>g is not at all a novelty <strong>and</strong> thatdur<strong>in</strong>g many years a large <strong>and</strong> specific experience <strong>of</strong> forecast<strong>in</strong>g hadbeen acquired with a great deal <strong>of</strong> trouble. It is hardly possible tocreate some essentially new, general <strong>and</strong> at <strong>the</strong> same time substantial<strong>the</strong>ory <strong>of</strong> forecast<strong>in</strong>g. Meanwhile, however, a unification <strong>of</strong>term<strong>in</strong>ology connected with forecast<strong>in</strong>g can undoubtedly play somepositive role.2. The Initial Concepts <strong>of</strong> <strong>the</strong> Applied Theory <strong>of</strong> <strong>Probability</strong>2.1. R<strong>and</strong>om variables <strong>and</strong> <strong>the</strong>ir moments. Denote <strong>the</strong> controlledconditions <strong>of</strong> trials by U, <strong>the</strong>ir result by V <strong>and</strong> <strong>the</strong> magnitude measured<strong>in</strong> trial s by X(s). The forecast <strong>of</strong> X(s + 1) given X(s) <strong>of</strong>ten fails.Permanence (forecast verified many times) is looked for by averag<strong>in</strong>g<strong>and</strong> obta<strong>in</strong><strong>in</strong>g from <strong>in</strong>itial unpredictable magnitude V 1 = X(s)V = E ( X ) = X ( s)mmwhere E m (X), <strong>in</strong> general also unpredictable, is <strong>the</strong> empirical mean <strong>of</strong> anunpredictable magnitude, <strong>of</strong> a r<strong>and</strong>om variable X(s). It is <strong>of</strong>ten stable:E m (X) ≈ E(X) (1)124
which means that sooner or later <strong>the</strong> scatter <strong>of</strong> <strong>the</strong> values <strong>of</strong> E m (X)ra<strong>the</strong>r <strong>of</strong>ten appreciably dim<strong>in</strong>ishes. The author <strong>in</strong>troduced <strong>the</strong> pattern <strong>of</strong> anextended series <strong>of</strong> trials. Bear<strong>in</strong>g <strong>in</strong> m<strong>in</strong>d his statements made <strong>in</strong> <strong>the</strong> sequel, it meansthat <strong>the</strong> behaviour <strong>of</strong> E m (X) is studied throughout <strong>the</strong> series ra<strong>the</strong>r than appreciatedby <strong>the</strong> result <strong>of</strong> <strong>the</strong> last trial. This latter method is called <strong>the</strong> pattern <strong>of</strong> a fixed series.For a predictable permanence it is supposed that (1) persists when <strong>the</strong> series isextended <strong>and</strong> E(X) is <strong>the</strong> predictable rough estimate <strong>of</strong> <strong>the</strong> empirical mean.Expectation <strong>of</strong> a separate measurement is mean<strong>in</strong>gless.The author <strong>in</strong>troduces moments but barely applies <strong>the</strong>m.2.2. Statistical stability. It is <strong>of</strong>ten alleged that homogeneity <strong>of</strong>trials leads to statistical stability. Only controlled conditions <strong>of</strong> trialsare meant <strong>and</strong> <strong>the</strong>refore, on <strong>the</strong> contrary, statistical stability means that<strong>the</strong> trials were homogeneous. Statistical stability is best justified byempirical <strong>in</strong>duction. Without stability E(X) does not exist.R<strong>and</strong>omness (<strong>in</strong> <strong>the</strong> general sense) is identified withunpredictability. It became usual to underst<strong>and</strong> r<strong>and</strong>om variables <strong>in</strong> <strong>the</strong>ma<strong>the</strong>matical sense only as statistically stable unpredictablemagnitudes, <strong>and</strong> even such for which <strong>the</strong> notion <strong>of</strong> distribution <strong>of</strong>probabilities is applicable.This narrow specialized <strong>in</strong>terpretation <strong>of</strong> r<strong>and</strong>om variable is stillbe<strong>in</strong>g willy-nilly confused with its wide general mean<strong>in</strong>g <strong>and</strong> leads toa mistaken belief that <strong>the</strong> applied <strong>the</strong>ory <strong>of</strong> probability <strong>and</strong>ma<strong>the</strong>matical statistics are applicable to any r<strong>and</strong>om variableunderstood <strong>in</strong> <strong>the</strong> general sense, i. e., to unpredictable magnitudes.On <strong>the</strong> o<strong>the</strong>r h<strong>and</strong>, <strong>the</strong> reader beg<strong>in</strong>s to believe that <strong>the</strong>ma<strong>the</strong>matical propositions <strong>of</strong> <strong>the</strong> <strong>the</strong>ory <strong>of</strong> probability somehowdirectly concern only such magnitudes. Actually, <strong>the</strong>ir unpredictabilityis not at all a necessary condition for apply<strong>in</strong>g to <strong>the</strong>m <strong>the</strong> <strong>the</strong>ory <strong>of</strong>probability. It is important that when measur<strong>in</strong>g a magnitude manytimes it <strong>in</strong>dicates statistical stability. An artificial <strong>in</strong>troduction <strong>of</strong>unpredictability <strong>in</strong> an experiment by <strong>the</strong> so-called r<strong>and</strong>omization asalso <strong>in</strong> some calculations by <strong>the</strong> Monte Carlo method can be thought tomean an excessively brave challenge to <strong>the</strong> natural scientific tradition 1 .2.3. <strong>Probability</strong> <strong>of</strong> an event. An event A is r<strong>and</strong>om <strong>in</strong> both senses if X A (s)is r<strong>and</strong>om. Stability <strong>of</strong> frequency is established by empirical <strong>in</strong>duction accord<strong>in</strong>g to<strong>the</strong> pattern <strong>of</strong> an extended series. If frequency is stable, E(X), <strong>the</strong> probability <strong>of</strong> anevent, is its predictable rough estimate. If <strong>the</strong> behaviour <strong>of</strong> <strong>the</strong> series is not studied,<strong>and</strong> <strong>the</strong> probability only determ<strong>in</strong>ed by its outcome, <strong>the</strong> statistical stability is not<strong>in</strong>vestigated.Statistical probability is not applicable to <strong>in</strong>dividual trials. For estimat<strong>in</strong>g <strong>the</strong>probability <strong>of</strong> a rare event <strong>of</strong> <strong>the</strong> order <strong>of</strong> 10 −4 , sometimes encountered <strong>in</strong> <strong>the</strong>reliability <strong>the</strong>ory, 10 5 measurements are required.2.4. Distribution <strong>of</strong> probabilities. It is measured for a series <strong>of</strong> an<strong>in</strong>creas<strong>in</strong>g number <strong>of</strong> trials. If <strong>the</strong> empirical distributions are stabilized, F(X) isdeterm<strong>in</strong>ed. This is empirical <strong>in</strong>duction for <strong>the</strong> pattern <strong>of</strong> an extended series. Lack <strong>of</strong>stability <strong>of</strong> <strong>the</strong> empirical distributions means that <strong>the</strong> notion <strong>of</strong> F(X) is not applicable.Often recommended is <strong>the</strong> measurement <strong>of</strong> those F m (X) because <strong>the</strong>ir stability ismore noticeable, ra<strong>the</strong>r than <strong>the</strong> histograms, but this is ak<strong>in</strong> to stat<strong>in</strong>g that an<strong>in</strong>sensitive device is better than a sensitive histogram (<strong>in</strong>dicat<strong>in</strong>g a greater scatter, alack <strong>of</strong> stability).2.5. Statistical <strong>in</strong>dependence. Lack <strong>of</strong> correlation. A necessary<strong>and</strong> sufficient condition <strong>of</strong> <strong>in</strong>dependence isF(X 1 , X 2 , ..., X n ) = F 1 (X 1 ) F 2 (X 2 ) ... F n (X n ).125
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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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structure of statistical methods, d
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Suppose that we have adopted the pa
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and the variances are inversely pro
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It is interesting therefore to see
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is applied with P(t) being a polyno
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ut some mathematical tricks describ
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of various groups of machines, and
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nnA(λ) x sin λ t, B(λ) = x cosλ
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of the mathematical model of the Br
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dF(λ) = f (λ) dλ, so that B( t
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usually very little of them. Indeed
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