For a centered record of length , the periodogram is the squared modulus of its discrete Fourier transform, with normalization
Under suitable short-memory assumptions its expectation approaches the spectral density of a stationary process, but its variance generally does not vanish. Smoothing nearby frequencies can provide an estimate with statistical consistency.
Let be a centered real stationary Gaussian time series with absolutely summable autocovariances and two-sided angular-frequency spectral density . The parent periodogram uses . At an interior positive frequency define the one-sided quantities
Thus the doubling applies to both the statistic and its target spectral density.
For Fourier-grid frequencies with , set
Then . Summability makes their variances tend to and their covariance tend to zero. Joint Gaussianity therefore gives
Under these Gaussian assumptions the fourth moments also converge, so . An unsmoothed periodogram is therefore not a consistent estimator of a positive spectral density. At zero and the Nyquist frequency , the sine coordinate vanishes and the real-only calibration differs; the interior doubling and two-coordinate argument do not apply there.[ref]
For a centered stationary real Gaussian sequence, let and be its cosine and sine coefficients with normalization at a nonzero Fourier frequency. Grouping the double covariance sum by lag and extending each lag sum to a whole record leaves at most omitted bounded products. The full cosine-sine sum is zero, giving the bound. If , the two coefficients become asymptotically uncorrelated, and their limiting joint normal distribution consequently has independent components.
Average neighboring periodogram ordinates with nonnegative weights summing to one. Let the number of averaged ordinates tend to infinity while their frequency span, of order , tends to zero. For a smooth spectral density and suitable short-memory or fourth-order dependence conditions, the bias tends to zero and variance is of order . Smooth second-order spectral density alone does not ensure this: a time-constant random scale multiplying independent white noise has a smooth unconditional spectrum but a nonergodic random limiting local power.

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