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The up-down separation operator

The derivation for decomposing over/under pressure waves into up-going and down-going signals is best done in the Fourier domain. For a thorough review of this method, please refer to Sonneland et al. (1986). Denote $ P_1(\omega, k_x)$ and $ P_2(\omega,k_x)$ to be the Fourier-transformed measurements of compressional waves at depths $ z_1$ (over) and $ z_2$ (under). Theoretically, $ P_1(\omega, k_x)$ is a sum of the up-going $ U_1(\omega, k_x)$ and down-going $ D_1(\omega, k_x)$ components. Likewise for $ P_2(\omega,k_x)$:


$\displaystyle P_1(\omega,k_x)$ $\displaystyle =$ $\displaystyle U_1(\omega,k_x) + D_1(\omega,k_x),$  
$\displaystyle P_2(\omega,k_x)$ $\displaystyle =$ $\displaystyle U_2(\omega,k_x) + D_2(\omega,k_x).$ (5)

Down-going waves arrive at the under array ($ D_2$) before the over ($ D_1$) array. Therefore, shifting $ D_2$ forward in time would match the signal $ D_1$. Similarly, up-going waves visit the over array first. Therefore, shifting $ U_1$ forward in time would match the signal $ U_2$. This relationship is equivalent to a phase-shift in the Fourier domain:


$\displaystyle e^{i k_z \Delta z } D_2$ $\displaystyle =$ $\displaystyle D_1 ,$  
$\displaystyle U_2$ $\displaystyle =$ $\displaystyle e^{i k_z \Delta z } U_1 ,$ (6)

where $ \Delta z = z_2 - z_1$, and $ k_z$ is the usual dispersion relation. Finally, substituting equation 6 into equation 5 yields the formula for the up-going and down-going waves at the receivers:


$\displaystyle U_2$ $\displaystyle =$ $\displaystyle \frac{P_2 - e^{i k_z \Delta z } P_1}{1 - e^{2 i k_z \Delta z }},$  
$\displaystyle D_2$ $\displaystyle =$ $\displaystyle \frac{e^{i k_z \Delta z } P_1 - e^{2 i k_z \Delta z } P_2}{1 - e^{2 i k_z \Delta z }}.$ (7)

Over/under acquisition is used to eliminate receiver ghosting and water reverberation. Although over/under arrays are rarely placed on the sea floor in real seismic surveys, this technique allows easy generation of up-going and down-going waves at the sea bottom for synthetic examples or modeling. For the remaining of this paper, we will denote the operation that separates over/under data into up-down data in equation 7 as $ \bold S$.


next up previous [pdf]

Next: Synthetic ocean-bottom data Up: The RTM and the Previous: The RTM operator

2009-10-19