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The inverse problem for imaging multiples using up- and down-going data

The inverse problem for imaging multiples using up- and down-going data can be fomulated as follow. We first break down the recorded data as the superposition of up- $ \bold d_{\uparrow}$ and down-going $ \bold d_{\downarrow}$ signals at the receivers. This can be done by using PZ data to give up-going and down-going data as discussed in the PZ summation section above.

$\displaystyle \left[ \begin{array}{c}
\bold d_{\uparrow} \\
\bold d_{\downarro...
..._{pz} \left[
\begin{array}{c}
\bold d_{p} \\
\bold d_{z} \end{array}
\right]
$

The above construction assumes that the vertical particle velocity $ d_z$ contains mostly pressure ($ \bold P$) waves. A pre-processing step can be included into $ \bold S_{pz}$ to separate the $ \bold P-$ and converted $ \bold S-$wave arrivals (Helbig and Mesdag, 1982; Dankbaar, 1985). Next, we denote the modelling operator for up-going signals at the receivers as $ \bold L_{\uparrow}$. Similarily, denote the modeling operator for down-going signals at the receivers as $ \bold L_{\downarrow}$. The two modeling operators provide the up- and down-going modeled data, denoted as $ \bold d^{mod}_{\uparrow}$ and $ \bold d^{mod}_{\downarrow}$;


$\displaystyle \bold d^{mod}_{\uparrow}$ $\displaystyle =$ $\displaystyle \bold L_{\uparrow} \bold m ,$  
$\displaystyle \bold d^{mod}_{\downarrow}$ $\displaystyle =$ $\displaystyle \bold L_{\downarrow} \bold m .$ (5)

The inverse problem is defined as minimizing the $ L_2$ norm of the two data residuals $ \bold r_{\uparrow}$ and $ \bold r_{\downarrow}$ , with respect to a single model $ \bold m$. The data residuals are defined as the difference between the recorded data and the modelled data,


$\displaystyle \bold r_{\uparrow}$ $\displaystyle =$ $\displaystyle \bold d_{\uparrow} - \bold d^{mod}_{\uparrow} = \bold d_{\uparrow} - \bold L_{\uparrow} \bold m ,$  
$\displaystyle \bold r_{\downarrow}$ $\displaystyle =$ $\displaystyle \bold d_{\downarrow} - \bold d^{mod}_{\downarrow} = \bold d_{\downarrow} - \bold L_{\downarrow} \bold m ,$ (6)

$\displaystyle min \left( \Vert \bold L_{\uparrow} \bold m - \bold d_{\uparrow} ...
...+ \Vert \bold L_{\downarrow} \bold m - \bold d_{\downarrow} \Vert _2^2 \right),$ (7)

where $ \Vert . \Vert _{2}$ represents the $ L_2$ norm. In matrix form, the fitting goal can be written as

$\displaystyle 0 \approx \left[ \begin{array}{c}
\bold L_{\uparrow} \\
\bold L_...
...in{array}{c}
\bold d_{\uparrow} \\
\bold d_{\downarrow} \end{array}
\right].
$

With the conjugate gradient method, the model update $ \Delta \bold m$ at each iteration has contributions from both the up-going and down-going parts of the inversion;

$\displaystyle \Delta \bold m = \bold L'_{\uparrow} \bold r_{\uparrow} + \bold L'_{\downarrow} \bold r_{\downarrow}.$ (8)

where $ \bold r_{\uparrow} = \bold L_{\uparrow} \bold m - \bold d_{\uparrow} $ and $ \bold r_{\downarrow} = \bold L_{\downarrow} \bold m - \bold d_{\downarrow}$ is the up- and down-going part of the residual, respectively.

The justification for this inverse problem is to reduce the wrong placement of image point with the use of both $ \bold d_{\uparrow}$ and $ \bold d_{\downarrow}$ signals. Traditional migration scheme only uses $ d_{\uparrow}$ to determine the image since all primary signal can be found in $ \bold d_{\uparrow}$. However, migration of primaries can give incorrect image point as well. In Figure 4, a primary event with a given travel time can indicate a correct image point at A and an incorrect image point at B. If we include the previously ignored information $ \bold d_{\downarrow}$ into a joint inversion, some wrongly placed image point can be refuted. Joint imaging allow us to use both primaries and multiples to estimate the image. This can be a distinct advantage because multiples and primaries illuminate different parts of the sub-surface. For ocean bottom data with sparse receiver spacing, multiples illuminate more than primaries.

whyupdown
whyupdown
Figure 4.
An up-going signal with a given travel time can indicate a correctly placed reflector at A and an incorrectly placed reflector at B. Reflector A will be supported by down-going data while reflector B will be refuted. [NR]
[pdf] [png]

The quality of the inverse problem would depend on the implemetation of the modeling operator. The next section will discuss how to approximate the modeling operator.


next up previous [pdf]

Next: Modelling Operators Up: Wong et al.: Up-down Previous: Separation using over-under recordings

2009-05-05