Autocorrelation
Part of a series on Statistics 
Correlation and covariance 

Correlation and covariance of random vectors 
Correlation and covariance of stochastic processes 
Correlation and covariance of deterministic signals

Autocorrelation, sometimes known as serial correlation in the discrete time case, is the correlation of a signal with a delayed copy of itself as a function of delay. Informally, it is the similarity between observations of a random variable as a function of the time lag between them. The analysis of autocorrelation is a mathematical tool for finding repeating patterns, such as the presence of a periodic signal obscured by noise, or identifying the missing fundamental frequency in a signal implied by its harmonic frequencies. It is often used in signal processing for analyzing functions or series of values, such as time domain signals.
Different fields of study define autocorrelation differently, and not all of these definitions are equivalent. In some fields, the term is used interchangeably with autocovariance.
Unit root processes, trendstationary processes, autoregressive processes, and moving average processes are specific forms of processes with autocorrelation.
Autocorrelation of stochastic processes
In statistics, the autocorrelation of a real or complex random process is the Pearson correlation between values of the process at different times, as a function of the two times or of the time lag. Let [math]\displaystyle{ \left\{ X_t \right\} }[/math] be a random process, and [math]\displaystyle{ t }[/math] be any point in time ([math]\displaystyle{ t }[/math] may be an integer for a discretetime process or a real number for a continuoustime process). Then [math]\displaystyle{ X_t }[/math] is the value (or realization) produced by a given run of the process at time [math]\displaystyle{ t }[/math]. Suppose that the process has mean [math]\displaystyle{ \mu_t }[/math] and variance [math]\displaystyle{ \sigma_t^2 }[/math] at time [math]\displaystyle{ t }[/math], for each [math]\displaystyle{ t }[/math]. Then the definition of the autocorrelation function between times [math]\displaystyle{ t_1 }[/math] and [math]\displaystyle{ t_2 }[/math] is^{[1]}^{:p.388}^{[2]}^{:p.165}
[math]\displaystyle{ \operatorname{R}_{XX}(t_1,t_2) = \operatorname{E} \left[ X_{t_1} \overline{X}_{t_2}\right] }[/math] 

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where [math]\displaystyle{ \operatorname{E} }[/math] is the expected value operator and the bar represents complex conjugation. Note that the expectation may not be well defined.
Subtracting the mean before multiplication yields the autocovariance function between times [math]\displaystyle{ t_1 }[/math] and [math]\displaystyle{ t_2 }[/math]:^{[1]}^{:p.392}^{[2]}^{:p.168}
[math]\displaystyle{ \operatorname{K}_{XX}(t_1,t_2) = \operatorname{E} \left[ (X_{t_1}  \mu_{t_1})\overline{(X_{t_2}  \mu_{t_2})} \right] = \operatorname{E}\left[X_{t_1} \overline{X}_{t_2} \right]  \mu_{t_1}\overline{\mu}_{t_2} }[/math] 

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Note that this expression is not well defined for all time series or processes, because the mean may not exist, or the variance may be zero (for a constant process) or infinite (for processes with distribution lacking wellbehaved moments, such as certain types of power law).
Definition for widesense stationary stochastic process
If [math]\displaystyle{ \left\{ X_t \right\} }[/math] is a widesense stationary process then the mean [math]\displaystyle{ \mu }[/math] and the variance [math]\displaystyle{ \sigma^2 }[/math] are timeindependent, and further the autocovariance function depends only on the lag between [math]\displaystyle{ t_1 }[/math] and [math]\displaystyle{ t_2 }[/math]: the autocovariance depends only on the timedistance between the pair of values but not on their position in time. This further implies that the autocovariance and autocorrelation can be expressed as a function of the timelag, and that this would be an even function of the lag [math]\displaystyle{ \tau=t_2t_1 }[/math]. This gives the more familiar forms for the autocorrelation function^{[1]}^{:p.395}
[math]\displaystyle{ \operatorname{R}_{XX}(\tau) = \operatorname{E}\left[X_{t+\tau} \overline{X}_{t} \right] }[/math] 

( ) 
and the autocovariance function:
[math]\displaystyle{ \operatorname{K}_{XX}(\tau) = \operatorname{E}\left[ (X_{t+\tau}  \mu)\overline{(X_{t}  \mu)} \right] = \operatorname{E} \left[ X_{t+\tau} \overline{X}_{t} \right]  \mu\overline{\mu} }[/math] 

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In particular, note that
[math]\displaystyle{ \operatorname{K}_{XX}(0) = \sigma^2 . }[/math]
Normalization
It is common practice in some disciplines (e.g. statistics and time series analysis) to normalize the autocovariance function to get a timedependent Pearson correlation coefficient. However, in other disciplines (e.g. engineering) the normalization is usually dropped and the terms "autocorrelation" and "autocovariance" are used interchangeably.
The definition of the autocorrelation coefficient of a stochastic process is^{[2]}^{:p.169}
[math]\displaystyle{ \rho_{XX}(t_1,t_2) = \frac{\operatorname{K}_{XX}(t_1,t_2)}{\sigma_{t_1}\sigma_{t_2}} = \frac{\operatorname{E}\left[(X_{t_1}  \mu_{t_1}) \overline{(X_{t_2}  \mu_{t_2})} \right]}{\sigma_{t_1}\sigma_{t_2}} . }[/math]
If the function [math]\displaystyle{ \rho_{XX} }[/math] is well defined, its value must lie in the range [math]\displaystyle{ [1,1] }[/math], with 1 indicating perfect correlation and −1 indicating perfect anticorrelation.
For a widesense stationary (WSS) process, the definition is
[math]\displaystyle{ \rho_{XX}(\tau) = \frac{\operatorname{K}_{XX}(\tau)}{\sigma^2} = \frac{\operatorname{E} \left[(X_{t+\tau}  \mu)\overline{(X_{t}  \mu)}\right]}{\sigma^2} }[/math].
The normalization is important both because the interpretation of the autocorrelation as a correlation provides a scalefree measure of the strength of statistical dependence, and because the normalization has an effect on the statistical properties of the estimated autocorrelations.
Properties
Symmetry property
The fact that the autocorrelation function [math]\displaystyle{ \operatorname{R}_{XX} }[/math] is an even function can be stated as^{[2]}^{:p.171} [math]\displaystyle{ \operatorname{R}_{XX}(t_1,t_2) = \overline{\operatorname{R}_{XX}(t_2,t_1)} }[/math] respectively for a WSS process:^{[2]}^{:p.173} [math]\displaystyle{ \operatorname{R}_{XX}(\tau) = \overline{\operatorname{R}_{XX}(\tau)} . }[/math]
Maximum at zero
For a WSS process:^{[2]}^{:p.174} [math]\displaystyle{ \left\operatorname{R}_{XX}(\tau)\right \leq \operatorname{R}_{XX}(0) }[/math] Notice that [math]\displaystyle{ \operatorname{R}_{XX}(0) }[/math] is always real.
Cauchy–Schwarz inequality
The Cauchy–Schwarz inequality, inequality for stochastic processes:^{[1]}^{:p.392} [math]\displaystyle{ \left\operatorname{R}_{XX}(t_1,t_2)\right^2 \leq \operatorname{E}\left[ X_{t_1}^2\right] \operatorname{E}\left[X_{t_2}^2\right] }[/math]
Autocorrelation of white noise
The autocorrelation of a continuoustime white noise signal will have a strong peak (represented by a Dirac delta function) at [math]\displaystyle{ \tau=0 }[/math] and will be exactly [math]\displaystyle{ 0 }[/math] for all other [math]\displaystyle{ \tau }[/math].
Wiener–Khinchin theorem
The Wiener–Khinchin theorem relates the autocorrelation function [math]\displaystyle{ \operatorname{R}_{XX} }[/math] to the power spectral density [math]\displaystyle{ S_{XX} }[/math] via the Fourier transform:
[math]\displaystyle{ \operatorname{R}_{XX}(\tau) = \int_{\infty}^\infty S_{XX}(f) e^{i 2 \pi f \tau} \, {\rm d}f }[/math]
[math]\displaystyle{ S_{XX}(f) = \int_{\infty}^\infty \operatorname{R}_{XX}(\tau) e^{ i 2 \pi f \tau} \, {\rm d}\tau . }[/math]
For realvalued functions, the symmetric autocorrelation function has a real symmetric transform, so the Wiener–Khinchin theorem can be reexpressed in terms of real cosines only:
[math]\displaystyle{ \operatorname{R}_{XX}(\tau) = \int_{\infty}^\infty S_{XX}(f) \cos(2 \pi f \tau) \, {\rm d}f }[/math]
[math]\displaystyle{ S_{XX}(f) = \int_{\infty}^\infty \operatorname{R}_{XX}(\tau) \cos(2 \pi f \tau) \, {\rm d}\tau . }[/math]
Autocorrelation of random vectors
The (potentially timedependent) autocorrelation matrix (also called second moment) of a (potentially timedependent) random vector [math]\displaystyle{ \mathbf{X} = (X_1,\ldots,X_n)^{\rm T} }[/math] is an [math]\displaystyle{ n \times n }[/math] matrix containing as elements the autocorrelations of all pairs of elements of the random vector [math]\displaystyle{ \mathbf{X} }[/math]. The autocorrelation matrix is used in various digital signal processing algorithms.
For a random vector [math]\displaystyle{ \mathbf{X} = (X_1,\ldots,X_n)^{\rm T} }[/math] containing random elements whose expected value and variance exist, the autocorrelation matrix is defined by^{[3]}^{:p.190}^{[1]}^{:p.334}
[math]\displaystyle{ \operatorname{R}_{\mathbf{X}\mathbf{X}} \triangleq\ \operatorname{E} \left[ \mathbf{X} \mathbf{X}^{\rm T} \right] }[/math] 

( ) 
where [math]\displaystyle{ {}^{\rm T} }[/math] denotes the transposed matrix of dimensions [math]\displaystyle{ n \times n }[/math].
Written componentwise:
[math]\displaystyle{ \operatorname{R}_{\mathbf{X}\mathbf{X}} = \begin{bmatrix} \operatorname{E}[X_1 X_1] & \operatorname{E}[X_1 X_2] & \cdots & \operatorname{E}[X_1 X_n] \\ \\ \operatorname{E}[X_2 X_1] & \operatorname{E}[X_2 X_2] & \cdots & \operatorname{E}[X_2 X_n] \\ \\ \vdots & \vdots & \ddots & \vdots \\ \\ \operatorname{E}[X_n X_1] & \operatorname{E}[X_n X_2] & \cdots & \operatorname{E}[X_n X_n] \\ \\ \end{bmatrix} }[/math]
If [math]\displaystyle{ \mathbf{Z} }[/math] is a complex random vector, the autocorrelation matrix is instead defined by
[math]\displaystyle{ \operatorname{R}_{\mathbf{Z}\mathbf{Z}} \triangleq\ \operatorname{E}[\mathbf{Z} \mathbf{Z}^{\rm H}] . }[/math]
Here [math]\displaystyle{ {}^{\rm H} }[/math] denotes Hermitian transpose.
For example, if [math]\displaystyle{ \mathbf{X} = \left( X_1,X_2,X_3 \right)^{\rm T} }[/math] is a random vector, then [math]\displaystyle{ \operatorname{R}_{\mathbf{X}\mathbf{X}} }[/math] is a [math]\displaystyle{ 3 \times 3 }[/math] matrix whose [math]\displaystyle{ (i,j) }[/math]th entry is [math]\displaystyle{ \operatorname{E}[X_i X_j] }[/math].
Properties of the autocorrelation matrix
 The autocorrelation matrix is a Hermitian matrix for complex random vectors and a symmetric matrix for real random vectors.^{[3]}^{:p.190}
 The autocorrelation matrix is a positive semidefinite matrix,^{[3]}^{:p.190} i.e. [math]\displaystyle{ \mathbf{a}^{\mathrm T} \operatorname{R}_{\mathbf{X}\mathbf{X}} \mathbf{a} \ge 0 \quad \text{for all } \mathbf{a} \in \mathbb{R}^n }[/math] for a real random vector, and respectively [math]\displaystyle{ \mathbf{a}^{\mathrm H} \operatorname{R}_{\mathbf{Z}\mathbf{Z}} \mathbf{a} \ge 0 \quad \text{for all } \mathbf{a} \in \mathbb{C}^n }[/math] in case of a complex random vector.
 All eigenvalues of the autocorrelation matrix are real and nonnegative.
 The autocovariance matrix is related to the autocorrelation matrix as follows:[math]\displaystyle{ \operatorname{K}_{\mathbf{X}\mathbf{X}} = \operatorname{E}[(\mathbf{X}  \operatorname{E}[\mathbf{X}])(\mathbf{X}  \operatorname{E}[\mathbf{X}])^{\rm T}] = \operatorname{R}_{\mathbf{X}\mathbf{X}}  \operatorname{E}[\mathbf{X}] \operatorname{E}[\mathbf{X}]^{\rm T} }[/math]Respectively for complex random vectors:[math]\displaystyle{ \operatorname{K}_{\mathbf{Z}\mathbf{Z}} = \operatorname{E}[(\mathbf{Z}  \operatorname{E}[\mathbf{Z}])(\mathbf{Z}  \operatorname{E}[\mathbf{Z}])^{\rm H}] = \operatorname{R}_{\mathbf{Z}\mathbf{Z}}  \operatorname{E}[\mathbf{Z}] \operatorname{E}[\mathbf{Z}]^{\rm H} }[/math]
Autocorrelation of deterministic signals
In signal processing, the above definition is often used without the normalization, that is, without subtracting the mean and dividing by the variance. When the autocorrelation function is normalized by mean and variance, it is sometimes referred to as the autocorrelation coefficient^{[4]} or autocovariance function.
Autocorrelation of continuoustime signal
Given a signal [math]\displaystyle{ f(t) }[/math], the continuous autocorrelation [math]\displaystyle{ R_{ff}(\tau) }[/math] is most often defined as the continuous crosscorrelation integral of [math]\displaystyle{ f(t) }[/math] with itself, at lag [math]\displaystyle{ \tau }[/math].^{[1]}^{:p.411}
[math]\displaystyle{ R_{ff}(\tau) = \int_{\infty}^\infty f(t+\tau)\overline{f(t)}\, {\rm d}t = \int_{\infty}^\infty f(t) \overline{f(t\tau)}\, {\rm d}t }[/math] 

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where [math]\displaystyle{ \overline{f(t)} }[/math] represents the complex conjugate of [math]\displaystyle{ f(t) }[/math]. Note that the parameter [math]\displaystyle{ t }[/math] in the integral is a dummy variable and is only necessary to calculate the integral. It has no specific meaning.
Autocorrelation of discretetime signal
The discrete autocorrelation [math]\displaystyle{ R }[/math] at lag [math]\displaystyle{ \ell }[/math] for a discretetime signal [math]\displaystyle{ y(n) }[/math] is
[math]\displaystyle{ R_{yy}(\ell) = \sum_{n \in Z} y(n)\,\overline{y(n\ell)} }[/math] 

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The above definitions work for signals that are square integrable, or square summable, that is, of finite energy. Signals that "last forever" are treated instead as random processes, in which case different definitions are needed, based on expected values. For widesensestationary random processes, the autocorrelations are defined as
[math]\displaystyle{ \begin{align} R_{ff}(\tau) &= \operatorname{E}\left[f(t)\overline{f(t\tau)}\right] \\ R_{yy}(\ell) &= \operatorname{E}\left[y(n)\,\overline{y(n\ell)}\right] . \end{align} }[/math]
For processes that are not stationary, these will also be functions of [math]\displaystyle{ t }[/math], or [math]\displaystyle{ n }[/math].
For processes that are also ergodic, the expectation can be replaced by the limit of a time average. The autocorrelation of an ergodic process is sometimes defined as or equated to^{[4]}
[math]\displaystyle{ \begin{align} R_{ff}(\tau) &= \lim_{T \rightarrow \infty} \frac 1 T \int_0^T f(t+\tau)\overline{f(t)}\, {\rm d}t \\ R_{yy}(\ell) &= \lim_{N \rightarrow \infty} \frac 1 N \sum_{n=0}^{N1} y(n)\,\overline{y(n\ell)} . \end{align} }[/math]
These definitions have the advantage that they give sensible welldefined singleparameter results for periodic functions, even when those functions are not the output of stationary ergodic processes.
Alternatively, signals that last forever can be treated by a shorttime autocorrelation function analysis, using finite time integrals. (See shorttime Fourier transform for a related process.)
Definition for periodic signals
If [math]\displaystyle{ f }[/math] is a continuous periodic function of period [math]\displaystyle{ T }[/math], the integration from [math]\displaystyle{ \infty }[/math] to [math]\displaystyle{ \infty }[/math] is replaced by integration over any interval [math]\displaystyle{ [t_0,t_0+T] }[/math] of length [math]\displaystyle{ T }[/math]:
[math]\displaystyle{ R_{ff}(\tau) \triangleq \int_{t_0}^{t_0+T} f(t+\tau) \overline{f(t)} \,dt }[/math]
which is equivalent to
[math]\displaystyle{ R_{ff}(\tau) \triangleq \int_{t_0}^{t_0+T} f(t) \overline{f(t\tau)} \,dt }[/math]
Properties
In the following, we will describe properties of onedimensional autocorrelations only, since most properties are easily transferred from the onedimensional case to the multidimensional cases. These properties hold for widesense stationary processes.^{[5]}
 A fundamental property of the autocorrelation is symmetry, [math]\displaystyle{ R_{ff}(\tau) = R_{ff}(\tau) }[/math], which is easy to prove from the definition. In the continuous case,
 the autocorrelation is an even function [math]\displaystyle{ R_{ff}(\tau) = R_{ff}(\tau) }[/math] when [math]\displaystyle{ f }[/math] is a real function, and
 the autocorrelation is a Hermitian function [math]\displaystyle{ R_{ff}(\tau) = R_{ff}^*(\tau) }[/math] when [math]\displaystyle{ f }[/math] is a complex function.
 The continuous autocorrelation function reaches its peak at the origin, where it takes a real value, i.e. for any delay [math]\displaystyle{ \tau }[/math], [math]\displaystyle{ R_{ff}(\tau) \leq R_{ff}(0) }[/math].^{[1]}^{:p.410} This is a consequence of the rearrangement inequality. The same result holds in the discrete case.
 The autocorrelation of a periodic function is, itself, periodic with the same period.
 The autocorrelation of the sum of two completely uncorrelated functions (the crosscorrelation is zero for all [math]\displaystyle{ \tau }[/math]) is the sum of the autocorrelations of each function separately.
 Since autocorrelation is a specific type of crosscorrelation, it maintains all the properties of crosscorrelation.
 By using the symbol [math]\displaystyle{ * }[/math] to represent convolution and [math]\displaystyle{ g_{1} }[/math] is a function which manipulates the function [math]\displaystyle{ f }[/math] and is defined as [math]\displaystyle{ g_{1}(f)(t)=f(t) }[/math], the definition for [math]\displaystyle{ R_{ff}(\tau) }[/math] may be written as:[math]\displaystyle{ R_{ff}(\tau) = (f * g_{1}(\overline{f}))(\tau) }[/math]
Multidimensional autocorrelation
Multidimensional autocorrelation is defined similarly. For example, in three dimensions the autocorrelation of a squaresummable discrete signal would be
[math]\displaystyle{ R(j,k,\ell) = \sum_{n,q,r} x_{n,q,r}\,\overline{x}_{nj,qk,r\ell} . }[/math]
When mean values are subtracted from signals before computing an autocorrelation function, the resulting function is usually called an autocovariance function.
Efficient computation
For data expressed as a discrete sequence, it is frequently necessary to compute the autocorrelation with high computational efficiency. A brute force method based on the signal processing definition [math]\displaystyle{ R_{xx}(j) = \sum_n x_n\,\overline{x}_{nj} }[/math] can be used when the signal size is small. For example, to calculate the autocorrelation of the real signal sequence [math]\displaystyle{ x = (2,3,1) }[/math] (i.e. [math]\displaystyle{ x_0=2, x_1=3, x_2=1 }[/math], and [math]\displaystyle{ x_i = 0 }[/math] for all other values of i) by hand, we first recognize that the definition just given is the same as the "usual" multiplication, but with right shifts, where each vertical addition gives the autocorrelation for particular lag values: [math]\displaystyle{ \begin{array}{rrrrrr} & 2 & 3 & 1 \\ \times & 2 & 3 & 1 \\ \hline &2 &3 & 1 \\ & & 6 & 9 & 3 \\ + & & & 4 & 6 & 2 \\ \hline & 2 & 3 &14 & 3 & 2 \end{array} }[/math]
Thus the required autocorrelation sequence is [math]\displaystyle{ R_{xx}=(2,3,14,3,2) }[/math], where [math]\displaystyle{ R_{xx}(0)=14, }[/math] [math]\displaystyle{ R_{xx}(1)= R_{xx}(1)=3, }[/math] and [math]\displaystyle{ R_{xx}(2)= R_{xx}(2) = 2, }[/math] the autocorrelation for other lag values being zero. In this calculation we do not perform the carryover operation during addition as is usual in normal multiplication. Note that we can halve the number of operations required by exploiting the inherent symmetry of the autocorrelation. If the signal happens to be periodic, i.e. [math]\displaystyle{ x=(\ldots,2,3,1,2,3,1,\ldots), }[/math] then we get a circular autocorrelation (similar to circular convolution) where the left and right tails of the previous autocorrelation sequence will overlap and give [math]\displaystyle{ R_{xx}=(\ldots,14,1,1,14,1,1,\ldots) }[/math] which has the same period as the signal sequence [math]\displaystyle{ x. }[/math] The procedure can be regarded as an application of the convolution property of Ztransform of a discrete signal.
While the brute force algorithm is order n^{2}, several efficient algorithms exist which can compute the autocorrelation in order n log(n). For example, the Wiener–Khinchin theorem allows computing the autocorrelation from the raw data X(t) with two fast Fourier transforms (FFT):^{[6]}^{[page needed]}
[math]\displaystyle{ \begin{align} F_R(f) &= \operatorname{FFT}[X(t)] \\ S(f) &= F_R(f) F^*_R(f) \\ R(\tau) &= \operatorname{IFFT}[S(f)] \end{align} }[/math]
where IFFT denotes the inverse fast Fourier transform. The asterisk denotes complex conjugate.
Alternatively, a multiple τ correlation can be performed by using brute force calculation for low τ values, and then progressively binning the X(t) data with a logarithmic density to compute higher values, resulting in the same n log(n) efficiency, but with lower memory requirements.^{[7]}^{[8]}
Estimation
For a discrete process with known mean and variance for which we observe [math]\displaystyle{ n }[/math] observations [math]\displaystyle{ \{X_1,\,X_2,\,\ldots,\,X_n\} }[/math], an estimate of the autocorrelation coefficient may be obtained as
[math]\displaystyle{ \hat{R}(k)=\frac{1}{(nk) \sigma^2} \sum_{t=1}^{nk} (X_t\mu)(X_{t+k}\mu) }[/math]
for any positive integer [math]\displaystyle{ k\lt n }[/math]. When the true mean [math]\displaystyle{ \mu }[/math] and variance [math]\displaystyle{ \sigma^2 }[/math] are known, this estimate is unbiased. If the true mean and variance of the process are not known there are several possibilities:
 If [math]\displaystyle{ \mu }[/math] and [math]\displaystyle{ \sigma^2 }[/math] are replaced by the standard formulae for sample mean and sample variance, then this is a biased estimate.
 A periodogrambased estimate replaces [math]\displaystyle{ nk }[/math] in the above formula with [math]\displaystyle{ n }[/math]. This estimate is always biased; however, it usually has a smaller mean squared error.^{[9]}^{[10]}
 Other possibilities derive from treating the two portions of data [math]\displaystyle{ \{X_1,\,X_2,\,\ldots,\,X_{nk}\} }[/math] and [math]\displaystyle{ \{X_{k+1},\,X_{k+2},\,\ldots,\,X_n\} }[/math] separately and calculating separate sample means and/or sample variances for use in defining the estimate.^{[citation needed]}
The advantage of estimates of the last type is that the set of estimated autocorrelations, as a function of [math]\displaystyle{ k }[/math], then form a function which is a valid autocorrelation in the sense that it is possible to define a theoretical process having exactly that autocorrelation. Other estimates can suffer from the problem that, if they are used to calculate the variance of a linear combination of the [math]\displaystyle{ X }[/math]'s, the variance calculated may turn out to be negative.^{[11]}
Regression analysis
In regression analysis using time series data, autocorrelation in a variable of interest is typically modeled either with an autoregressive model (AR), a moving average model (MA), their combination as an autoregressivemovingaverage model (ARMA), or an extension of the latter called an autoregressive integrated moving average model (ARIMA). With multiple interrelated data series, vector autoregression (VAR) or its extensions are used.
In ordinary least squares (OLS), the adequacy of a model specification can be checked in part by establishing whether there is autocorrelation of the regression residuals. Problematic autocorrelation of the errors, which themselves are unobserved, can generally be detected because it produces autocorrelation in the observable residuals. (Errors are also known as "error terms" in econometrics.) Autocorrelation of the errors violates the ordinary least squares assumption that the error terms are uncorrelated, meaning that the Gauss Markov theorem does not apply, and that OLS estimators are no longer the Best Linear Unbiased Estimators (BLUE). While it does not bias the OLS coefficient estimates, the standard errors tend to be underestimated (and the tscores overestimated) when the autocorrelations of the errors at low lags are positive.
The traditional test for the presence of firstorder autocorrelation is the Durbin–Watson statistic or, if the explanatory variables include a lagged dependent variable, Durbin's h statistic. The DurbinWatson can be linearly mapped however to the Pearson correlation between values and their lags.^{[12]} A more flexible test, covering autocorrelation of higher orders and applicable whether or not the regressors include lags of the dependent variable, is the Breusch–Godfrey test. This involves an auxiliary regression, wherein the residuals obtained from estimating the model of interest are regressed on (a) the original regressors and (b) k lags of the residuals, where 'k' is the order of the test. The simplest version of the test statistic from this auxiliary regression is TR^{2}, where T is the sample size and R^{2} is the coefficient of determination. Under the null hypothesis of no autocorrelation, this statistic is asymptotically distributed as [math]\displaystyle{ \chi^2 }[/math] with k degrees of freedom.
Responses to nonzero autocorrelation include generalized least squares and the Newey–West HAC estimator (Heteroskedasticity and Autocorrelation Consistent).^{[13]}
In the estimation of a moving average model (MA), the autocorrelation function is used to determine the appropriate number of lagged error terms to be included. This is based on the fact that for an MA process of order q, we have [math]\displaystyle{ R(\tau) \neq 0 }[/math], for [math]\displaystyle{ \tau = 0,1, \ldots , q }[/math], and [math]\displaystyle{ R(\tau) = 0 }[/math], for [math]\displaystyle{ \tau \gt q }[/math].
Applications
 Autocorrelation analysis is used heavily in fluorescence correlation spectroscopy^{[14]} to provide quantitative insight into molecularlevel diffusion and chemical reactions.^{[15]}
 Another application of autocorrelation is the measurement of optical spectra and the measurement of veryshortduration light pulses produced by lasers, both using optical autocorrelators.
 Autocorrelation is used to analyze dynamic light scattering data, which notably enables determination of the particle size distributions of nanometersized particles or micelles suspended in a fluid. A laser shining into the mixture produces a speckle pattern that results from the motion of the particles. Autocorrelation of the signal can be analyzed in terms of the diffusion of the particles. From this, knowing the viscosity of the fluid, the sizes of the particles can be calculated.
 Utilized in the GPS system to correct for the propagation delay, or time shift, between the point of time at the transmission of the carrier signal at the satellites, and the point of time at the receiver on the ground. This is done by the receiver generating a replica signal of the 1,023bit C/A (Coarse/Acquisition) code, and generating lines of code chips [1,1] in packets of ten at a time, or 10,230 chips (1,023 × 10), shifting slightly as it goes along in order to accommodate for the doppler shift in the incoming satellite signal, until the receiver replica signal and the satellite signal codes match up.^{[16]}
 The smallangle Xray scattering intensity of a nanostructured system is the Fourier transform of the spatial autocorrelation function of the electron density.
 In surface science and scanning probe microscopy, autocorrelation is used to establish a link between surface morphology and functional characteristics.^{[17]}
 In optics, normalized autocorrelations and crosscorrelations give the degree of coherence of an electromagnetic field.
 In signal processing, autocorrelation can give information about repeating events like musical beats (for example, to determine tempo) or pulsar frequencies, though it cannot tell the position in time of the beat. It can also be used to estimate the pitch of a musical tone.
 In music recording, autocorrelation is used as a pitch detection algorithm prior to vocal processing, as a distortion effect or to eliminate undesired mistakes and inaccuracies.^{[18]}
 Autocorrelation in space rather than time, via the Patterson function, is used by Xray diffractionists to help recover the "Fourier phase information" on atom positions not available through diffraction alone.
 In statistics, spatial autocorrelation between sample locations also helps one estimate mean value uncertainties when sampling a heterogeneous population.
 The SEQUEST algorithm for analyzing mass spectra makes use of autocorrelation in conjunction with crosscorrelation to score the similarity of an observed spectrum to an idealized spectrum representing a peptide.
 In astrophysics, autocorrelation is used to study and characterize the spatial distribution of galaxies in the universe and in multiwavelength observations of low mass Xray binaries.
 In panel data, spatial autocorrelation refers to correlation of a variable with itself through space.
 In analysis of Markov chain Monte Carlo data, autocorrelation must be taken into account for correct error determination.
 In geosciences (specifically in geophysics) it can be used to compute an autocorrelation seismic attribute, out of a 3D seismic survey of the underground.
 In medical ultrasound imaging, autocorrelation is used to visualize blood flow.
 In intertemporal portfolio choice, the presence or absence of autocorrelation in an asset's rate of return can affect the optimal portion of the portfolio to hold in that asset.
 Autocorrelation has been used to accurately measure power system frequency in numerical relays.^{[19]}
Serial dependence
Serial dependence is closely linked to the notion of autocorrelation, but represents a distinct concept (see Correlation and dependence). In particular, it is possible to have serial dependence but no (linear) correlation. In some fields however, the two terms are used as synonyms.
A time series of a random variable has serial dependence if the value at some time [math]\displaystyle{ t }[/math] in the series is statistically dependent on the value at another time [math]\displaystyle{ s }[/math]. A series is serially independent if there is no dependence between any pair.
If a time series [math]\displaystyle{ \left\{ X_t \right\} }[/math] is stationary, then statistical dependence between the pair [math]\displaystyle{ (X_t,X_s) }[/math] would imply that there is statistical dependence between all pairs of values at the same lag [math]\displaystyle{ \tau=st }[/math].
See also
 Autocorrelation matrix
 Autocorrelation of a formal word
 Autocorrelation technique
 Autocorrelator
 Cochrane–Orcutt estimation (transformation for autocorrelated error terms)
 Correlation function
 Correlogram
 Crosscorrelation
 CUSUM
 Fluorescence correlation spectroscopy
 Optical autocorrelation
 Partial autocorrelation function
 Phylogenetic autocorrelation (Galton's problem}
 Pitch detection algorithm
 Prais–Winsten transformation
 Scaled correlation
 Triple correlation
 Unbiased estimation of standard deviation
References
 ↑ ^{1.0} ^{1.1} ^{1.2} ^{1.3} ^{1.4} ^{1.5} ^{1.6} Gubner, John A. (2006). Probability and Random Processes for Electrical and Computer Engineers. Cambridge University Press. ISBN 9780521864701.
 ↑ ^{2.0} ^{2.1} ^{2.2} ^{2.3} ^{2.4} ^{2.5} Kun Il Park, Fundamentals of Probability and Stochastic Processes with Applications to Communications, Springer, 2018, ISBN:9783319680743
 ↑ ^{3.0} ^{3.1} ^{3.2} Papoulis, Athanasius, Probability, Random variables and Stochastic processes, McGrawHill, 1991
 ↑ ^{4.0} ^{4.1} Dunn, Patrick F. (2005). Measurement and Data Analysis for Engineering and Science. New York: McGraw–Hill. ISBN 9780072825381.
 ↑ Proakis, John (August 31, 2001). Communication Systems Engineering (2nd Edition) (2 ed.). Pearson. p. 168. ISBN 9780130617934.
 ↑ Box, G. E. P.; Jenkins, G. M.; Reinsel, G. C. (1994). Time Series Analysis: Forecasting and Control (3rd ed.). Upper Saddle River, NJ: Prentice–Hall. ISBN 9780130607744.
 ↑ Frenkel, D.; Smit, B. (2002). "chap. 4.4.2". Understanding Molecular Simulation (2nd ed.). London: Academic Press. ISBN 9780122673511.
 ↑ Colberg, P.; Höfling, F. (2011). "Highly accelerated simulations of glassy dynamics using GPUs: caveats on limited floatingpoint precision". Comput. Phys. Commun. 182 (5): 1120–1129. doi:10.1016/j.cpc.2011.01.009. Bibcode: 2011CoPhC.182.1120C.
 ↑ Priestley, M. B. (1982). Spectral Analysis and Time Series. London, New York: Academic Press. ISBN 9780125649018.
 ↑ Percival, Donald B.; Andrew T. Walden (1993). Spectral Analysis for Physical Applications: Multitaper and Conventional Univariate Techniques. Cambridge University Press. pp. 190–195. ISBN 9780521435413. https://archive.org/details/spectralanalysis00perc_105.
 ↑ Percival, Donald B. (1993). "Three Curious Properties of the Sample Variance and Autocovariance for Stationary Processes with Unknown Mean" (in en). The American Statistician 47 (4): 274–276. doi:10.1080/00031305.1993.10475997.
 ↑ "Serial correlation techniques". Statistical Ideas. 26 May 2014. http://statisticalideas.blogspot.com/2014/05/serialcorrelationtechniques.html.
 ↑ Baum, Christopher F. (2006). An Introduction to Modern Econometrics Using Stata. Stata Press. ISBN 9781597180139.
 ↑ Elson, Elliot L. (December 2011). "Fluorescence Correlation Spectroscopy: Past, Present, Future" (in en). Biophysical Journal 101 (12): 2855–2870. doi:10.1016/j.bpj.2011.11.012. PMID 22208184. Bibcode: 2011BpJ...101.2855E.
 ↑ Hołyst, Robert; Poniewierski, Andrzej; Zhang, Xuzhu (2017). "Analytical form of the autocorrelation function for the fluorescence correlation spectroscopy" (in en). Soft Matter 13 (6): 1267–1275. doi:10.1039/C6SM02643E. ISSN 1744683X. PMID 28106203. Bibcode: 2017SMat...13.1267H.
 ↑ Van Sickle, Jan (2008). GPS for Land Surveyors (Third ed.). CRC Press. pp. 18–19. ISBN 9780849391958.
 ↑ Kalvani, Payam Rajabi; Jahangiri, Ali Reza; Shapouri, Samaneh; Sari, Amirhossein; Jalili, Yousef Seyed (August 2019). "Multimode AFM analysis of aluminumdoped zinc oxide thin films sputtered under various substrate temperatures for optoelectronic applications" (in en). Superlattices and Microstructures 132: 106173. doi:10.1016/j.spmi.2019.106173.
 ↑ Tyrangiel, Josh (20090205). "AutoTune: Why Pop Music Sounds Perfect". Time (magazine). http://www.time.com/time/magazine/article/0,9171,1877372,00.html.
 ↑ Kasztenny, Bogdan (March 2016). "A New Method for Fast Frequency Measurement for Protection Applications". Schweitzer Engineering Laboratories. https://cdn.selinc.com/assets/Literature/Publications/Technical%20Papers/6734_NewMethod_BK_20151112_Web.pdf.
Further reading
 Kmenta, Jan (1986). Elements of Econometrics (Second ed.). New York: Macmillan. pp. 298–334. ISBN 9780023650703. https://archive.org/details/elementsofeconom0003kmen/page/298.
 Marno Verbeek (10 August 2017). A Guide to Modern Econometrics. Wiley. ISBN 9781119401100. https://books.google.com/books?id=SQxDDwAAQBAJ.
 Mojtaba Soltanalian, and Petre Stoica. "Computational design of sequences with good correlation properties." IEEE Transactions on Signal Processing, 60.5 (2012): 2180–2193.
 Solomon W. Golomb, and Guang Gong. Signal design for good correlation: for wireless communication, cryptography, and radar. Cambridge University Press, 2005.
 Klapetek, Petr (2018). Quantitative Data Processing in Scanning Probe Microscopy: SPM Applications for Nanometrology (Second ed.). Elsevier. pp. 108–112 ISBN:9780128133477.
 Weisstein, Eric W.. "Autocorrelation". http://mathworld.wolfram.com/Autocorrelation.html.
Original source: https://en.wikipedia.org/wiki/Autocorrelation.
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