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1 Studies in the History of Statistics and Probability ... - Sheynin, Oscar

1 Studies in the History of Statistics and Probability ... - Sheynin, Oscar

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dF(λ) = f (λ) dλ, so that B( t − s) = cosλ( t − s) f (λ) dλ.π∫−πSpectral analysis, that is, an experimental determ<strong>in</strong>ation <strong>of</strong> <strong>the</strong>spectral density f(λ), is <strong>the</strong>refore sometimes expla<strong>in</strong>ed as <strong>the</strong>determ<strong>in</strong>ation <strong>of</strong> <strong>the</strong> variances <strong>of</strong> <strong>the</strong> separate r<strong>and</strong>om components <strong>of</strong><strong>the</strong> process. For practically apply<strong>in</strong>g <strong>the</strong> correlation or spectral <strong>the</strong>oryit is necessary, first, to f<strong>in</strong>d out <strong>the</strong> practical conclusions possible from<strong>the</strong> correlation function or spectrum (spectral density); <strong>and</strong>, second, tobe able to estimate <strong>the</strong> correlation function (or spectral density) byobservations.That correlation function is normally applied <strong>in</strong> statistical problems.For example, <strong>the</strong> variance <strong>of</strong> <strong>the</strong> arithmetic mean ξ is expressedthrough <strong>the</strong> sum <strong>of</strong> paired covariations, i. e., through a correlationfunction. It can also be expressed through <strong>the</strong> spectral density.However, an estimate <strong>of</strong> a spectrum, or <strong>of</strong> a correlation function, issometimes applied as a magic remedy allegedly mak<strong>in</strong>g it possible topenetrate <strong>the</strong> essence <strong>of</strong> <strong>the</strong> observed process. It should be clearlyimag<strong>in</strong>ed that <strong>the</strong> correlation <strong>the</strong>ory generally deals with suchcharacteristics that are far from determ<strong>in</strong><strong>in</strong>g <strong>the</strong> process as a whole <strong>and</strong><strong>of</strong>ten only provides a superficial <strong>in</strong>formation about it. If we are<strong>in</strong>terested <strong>in</strong> some problem <strong>of</strong> its structure, we must be able t<strong>of</strong>ormulate it <strong>in</strong> terms <strong>of</strong> <strong>the</strong> correlation <strong>the</strong>ory while bear<strong>in</strong>g <strong>in</strong> m<strong>in</strong>dthat usually we do not know precisely ei<strong>the</strong>r <strong>the</strong> correlation function or<strong>the</strong> spectral density but estimate <strong>the</strong>m by observations. We should thusconsider comparatively rough characteristics determ<strong>in</strong>able by issu<strong>in</strong>gfrom non-precise data.For example, <strong>the</strong>re exists <strong>the</strong> so-called method <strong>of</strong> canonicalexpansion whose application dem<strong>and</strong>s <strong>the</strong> knowledge <strong>of</strong> <strong>the</strong>eigenfunctions <strong>of</strong> an <strong>in</strong>tegral equation <strong>in</strong> which a correlation function<strong>of</strong> a process is <strong>in</strong>cluded as a series. This method ought to berecognized as practically hopeless because <strong>the</strong> <strong>in</strong>accuracy <strong>of</strong> <strong>the</strong>equation’s kernel very essentially <strong>in</strong>fluences <strong>the</strong> eigenfunctions. I donot know about any practical application <strong>of</strong> that method. All so-calledapplications issue from arbitrarily given correlation functions <strong>and</strong> donot deal with statistical material.The estimation <strong>of</strong> <strong>the</strong> correlation function <strong>and</strong> spectrum is ra<strong>the</strong>rcomplicated. At first you should estimate <strong>and</strong> subtract <strong>the</strong> mean valuem <strong>of</strong> <strong>the</strong> process. Its estimate is <strong>the</strong> arithmetic mean mˆ = ξ . Theestimate <strong>of</strong>B(u) = Eξ t ξ t+n – m 2will beˆ 1B u m u nn−u2( ) = ∑ ξ ξ ˆt t+u− , = 0, 1, ..., −1.n − u t=169

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