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In statistics, **Whittle likelihood** is an approximation to the likelihood function of a stationary Gaussian time series. It is named after the mathematician and statistician Peter Whittle, who introduced it in his PhD thesis in 1951.^{[1]}
It is commonly utilized in time series analysis and signal processing for parameter estimation and signal detection.

In a stationary Gaussian time series model, the likelihood function is (as usual in Gaussian models) a function of the associated mean and covariance parameters. With a large number () of observations, the () covariance matrix may become very large, making computations very costly in practice. However, due to stationarity, the covariance matrix has a rather simple structure, and by using an approximation, computations may be simplified considerably (from to ).^{[2]} The idea effectively boils down to assuming a heteroscedastic zero-mean Gaussian model in Fourier domain; the model formulation is based on the time series' discrete Fourier transform and its power spectral density.^{[3]}^{[4]}^{[5]}

Let be a stationary Gaussian time series with (*one-sided*) power spectral density , where is even and samples are taken at constant sampling intervals .
Let be the (complex-valued) discrete Fourier transform (DFT) of the time series. Then for the Whittle likelihood one effectively assumes independent zero-mean Gaussian distributions for all with variances for the real and imaginary parts given by

where is the th Fourier frequency. This approximate model immediately leads to the (logarithmic) likelihood function

where denotes the absolute value with .^{[3]}^{[4]}^{[6]}

In case the noise spectrum is assumed a-priori *known*, and noise properties are not to be inferred from the data, the likelihood function may be simplified further by ignoring constant terms, leading to the sum-of-squares expression

This expression also is the basis for the common matched filter.

The Whittle likelihood in general is only an approximation, it is only exact if the spectrum is constant, i.e., in the trivial case of white noise.
The efficiency of the Whittle approximation always depends on the particular circumstances.^{[7]}
^{[8]}

Note that due to linearity of the Fourier transform, Gaussianity in Fourier domain implies Gaussianity in time domain and vice versa. What makes the Whittle likelihood only approximately accurate is related to the sampling theorem—the effect of Fourier-transforming only a *finite* number of data points, which also manifests itself as spectral leakage in related problems (and which may be ameliorated using the same methods, namely, windowing). In the present case, the implicit periodicity assumption implies correlation between the first and last samples ( and ), which are effectively treated as "neighbouring" samples (like and ).

Whittle's likelihood is commonly used to estimate signal parameters for signals that are buried in non-white noise. The noise spectrum then may be assumed known,^{[9]}
or it may be inferred along with the signal parameters.^{[4]}^{[6]}

Signal detection is commonly performed utilizing the matched filter, which is based on the Whittle likelihood for the case of a *known* noise power spectral density.^{[10]}^{[11]}
The matched filter effectively does a maximum-likelihood fit of the signal to the noisy data and uses the resulting likelihood ratio as the detection statistic.^{[12]}

The matched filter may be generalized to an analogous procedure based on a Student-t distribution by also considering uncertainty (e.g. estimation uncertainty) in the noise spectrum. On the technical side, this entails repeated or iterative matched-filtering.^{[12]}

The Whittle likelihood is also applicable for estimation of the noise spectrum, either alone or in conjunction with signal parameters.^{[13]}^{[14]}

- Coloured noise
- Discrete Fourier transform
- Likelihood function
- Matched filter
- Power spectral density
- Statistical signal processing
- Weighted least squares

**^**Whittle, P. (1951).*Hypothesis testing in times series analysis*. Uppsala: Almqvist & Wiksells Boktryckeri AB.**^**Hurvich, C. (2002). "Whittle's approximation to the likelihood function" (PDF). NYU Stern.- ^
^{a}^{b}Calder, M.; Davis, R. A. (1997), "An introduction to Whittle (1953) "The analysis of multiple stationary time series"", in Kotz, S.; Johnson, N. L. (eds.),*Breakthroughs in Statistics*, Springer Series in Statistics, New York: Springer-Verlag, pp. 141–169, doi:10.1007/978-1-4612-0667-5_7, ISBN 978-0-387-94989-5

See also: Calder, M.; Davis, R. A. (1996), "An introduction to Whittle (1953) "The analysis of multiple stationary time series"",*Technical report 1996/41*, Department of Statistics, Colorado State University - ^
^{a}^{b}^{c}Hannan, E. J. (1994), "The Whittle likelihood and frequency estimation", in Kelly, F. P. (ed.),*Probability, statistics and optimization; a tribute to Peter Whittle*, Chichester: Wiley **^**Pawitan, Y. (1998), "Whittle likelihood", in Kotz, S.; Read, C. B.; Banks, D. L. (eds.),*Encyclopedia of Statistical Sciences*, Update Volume 2, New York: Wiley & Sons, pp. 708–710, doi:10.1002/0471667196.ess0753, ISBN 978-0471667193- ^
^{a}^{b}Röver, C.; Meyer, R.; Christensen, N. (2011). "Modelling coloured residual noise in gravitational-wave signal processing".*Classical and Quantum Gravity*.**28**(1): 025010. arXiv:0804.3853. Bibcode:2011CQGra..28a5010R. doi:10.1088/0264-9381/28/1/015010. **^**Choudhuri, N.; Ghosal, S.; Roy, A. (2004). "Contiguity of the Whittle measure for a Gaussian time series".*Biometrika*.**91**(4): 211–218. doi:10.1093/biomet/91.1.211.**^**Countreras-Cristán, A.; Gutiérrez-Peña, E.; Walker, S. G. (2006). "A Note on Whittle's Likelihood".*Communications in Statistics – Simulation and Computation*.**35**(4): 857–875. doi:10.1080/03610910600880203.**^**Finn, L. S. (1992). "Detection, measurement and gravitational radiation".*Physical Review D*.**46**(12): 5236–5249. arXiv:gr-qc/9209010. Bibcode:1992PhRvD..46.5236F. doi:10.1103/PhysRevD.46.5236.**^**Turin, G. L. (1960). "An introduction to matched filters".*IRE Transactions on Information Theory*.**6**(3): 311–329. doi:10.1109/TIT.1960.1057571.**^**Wainstein, L. A.; Zubakov, V. D. (1962).*Extraction of signals from noise*. Englewood Cliffs, NJ: Prentice-Hall.- ^
^{a}^{b}Röver, C. (2011). "Student-t-based filter for robust signal detection".*Physical Review D*.**84**(12): 122004. arXiv:1109.0442. Bibcode:2011PhRvD..84l2004R. doi:10.1103/PhysRevD.84.122004. **^**Choudhuri, N.; Ghosal, S.; Roy, A. (2004). "Bayesian estimation of the spectral density of a time series" (PDF).*Journal of the American Statistical Association*.**99**(468): 1050–1059. CiteSeerX 10.1.1.212.2814. doi:10.1198/016214504000000557.**^**Edwards, M. C.; Meyer, R.; Christensen, N. (2015). "Bayesian semiparametric power spectral density estimation in gravitational wave data analysis".*Physical Review D*.**92**(6): 064011. arXiv:1506.00185. Bibcode:2015PhRvD..92f4011E. doi:10.1103/PhysRevD.92.064011.