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$ f-x$ EMD

$ f-x$ EMD was proposed by Bekara and van der Baan (2009) to attenuate random noise. They applied EMD on each frequency slice in the $ f-x$ domain, and remove the first IMF, which mainly represent the higher wavenumber components. The methodology can be summarized as:

\begin{displaymath}\begin{split}\hat{s}(m,t) &= \mathcal{F}^{-1}\left(\sum_{n=2}...
..., \\ \mathcal{F} d(m,t) &= \sum_{n=1}^{N} C_n(m,w), \end{split}\end{displaymath} (2)

where $ \hat{s}(m,t)$ and $ d(m,t)$ denote the estimated signal and acquired noisy signal, respectively. $ \mathcal{F}$ and $ \mathcal{F}^{-1}$ denote the forward and inverse Fourier transforms along the time axis, respectively. $ C_n$ denotes the $ n$ th EMD decomposed component. $ w$ denotes frequency. However, a problem occurs when applying $ f-x$ EMD, because the dipping events will also be removed. This problem occurs because, for many data sets, the random noise and any steeply dipping coherent energy make a significantly larger contribution to the high-wavenumber energy in the $ f-x$ domain than any desired signal (Bekara and van der Baan, 2009).


next up previous [pdf]

Next: SSA Up: Background theory Previous: EMD

2015-11-23