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 represent a pair of stochastic processes that are jointly wide sense stationary with autocovariance functions and and cross-covariance function . Then the cross-spectrum is defined as the Fourier transform of {{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
: .
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 is given by
:
and the phase spectrum is given by
:
\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.