cross-spectrum

{{Technical|date=April 2011}}

In time series analysis, the cross-spectrum is used as part of a frequency domain analysis of the cross-correlation or cross-covariance between two time series.

Definition

Let (X_t,Y_t) represent a pair of stochastic processes that are jointly wide sense stationary with autocovariance functions \gamma_{xx} and \gamma_{yy} and cross-covariance function \gamma_{xy}. Then the cross-spectrum \Gamma_{xy} is defined as the Fourier transform of \gamma_{xy} {{Cite book

| publisher = Cambridge Univ Pr

| isbn = 0-521-01230-9

| last = von Storch

| first = H.

|author2=F. W Zwiers

| title = Statistical analysis in climate research

| year = 2001

}}

:

\Gamma_{xy}(f)= \mathcal{F}\{\gamma_{xy}\}(f) = \sum_{\tau=-\infty}^\infty \,\gamma_{xy}(\tau) \,e^{-2\,\pi\,i\,\tau\,f} ,

where

: \gamma_{xy}(\tau) = \operatorname{E}[(x_t - \mu_x)(y_{t+\tau} - \mu_y)] .

The cross-spectrum has representations as a decomposition into (i) its real part (co-spectrum) and (ii) its imaginary part (quadrature spectrum)

:

\Gamma_{xy}(f)= \Lambda_{xy}(f) - i \Psi_{xy}(f) ,

and (ii) in polar coordinates

:

\Gamma_{xy}(f)= A_{xy}(f) \,e^{i \phi_{xy}(f) } .

Here, the amplitude spectrum A_{xy} is given by

: A_{xy}(f)= (\Lambda_{xy}(f)^2 + \Psi_{xy}(f)^2)^\frac{1}{2} ,

and the phase spectrum \Phi_{xy} is given by

: \begin{cases}

\tan^{-1} ( \Psi_{xy}(f) / \Lambda_{xy}(f) ) & \text{if } \Psi_{xy}(f) \ne 0 \text{ and } \Lambda_{xy}(f) \ne 0 \\

0 & \text{if } \Psi_{xy}(f) = 0 \text{ and } \Lambda_{xy}(f) > 0 \\

\pm \pi & \text{if } \Psi_{xy}(f) = 0 \text{ and } \Lambda_{xy}(f) < 0 \\

\pi/2 & \text{if } \Psi_{xy}(f) > 0 \text{ and } \Lambda_{xy}(f) = 0 \\

-\pi/2 & \text{if } \Psi_{xy}(f) < 0 \text{ and } \Lambda_{xy}(f) = 0 \\

\end{cases}

Squared coherency spectrum

The squared coherency spectrum is given by

:

\kappa_{xy}(f)= \frac{A_{xy}^2}{ \Gamma_{xx}(f) \Gamma_{yy}(f)} ,

which expresses the amplitude spectrum in dimensionless units.

See also

References