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Deblending via shaping regularization

The blending process can be summarized as the following equation:

$\displaystyle \mathbf{d}=\Gamma\mathbf{m},$ (1)

where $ \mathbf{d}$ is the blended data, $ \Gamma$ is the blending operator, and $ \mathbf{m}$ is the unblended data. The formulation of $ \Gamma$ has been introduced in Mahdad (2012) in detail. When considered in time domain, $ \Gamma$ corresponds to blending different shot records onto one receiver record according to the shot schedules of different shots. Deblending amounts to inverting equation 1 and recovering $ \mathbf{m}$ from $ \mathbf{d}$ .

Because of the ill-posed property of this problem, all inversion methods require some constraints.

Chen et al. (2014a) proposed a general iterative deblending framework via shaping regularization Fomel (2007,2008). The iterative deblending is expressed as:

$\displaystyle \mathbf{m}_{n+1} = \mathbf{S}[\mathbf{m}_n+\mathbf{B}[\mathbf{d}-\Gamma\mathbf{m}_n]],$ (2)

where $ \mathbf{S}$ is the shaping operator, which provides some constraints on the model, and $ \mathbf{B}$ is the backward operator, which approximates the inverse of $ \Gamma$ . The shaping regularization framework offers us much freedom in constraining an under-determined problem by allowing different types of constraints. In this paper, the backward operator is simply chosen as $ \lambda\Gamma^*$ , where $ \lambda$ is a scale coefficient closely related with the blending fold, and $ \Gamma^*$ stands for the adjoint operator of $ \Gamma$ (or the pseudo-deblending operator). For example, $ \lambda$ can be optimally chosen as $ 1/2$ in a two-source dithering configuration Chen et al. (2014a); Mahdad (2012). In the next two sections, I will first introduce the conventional way for choosing the $ \mathbf{S}$ and then propose a novel way for designing the $ \mathbf{S}$ .


next up previous [pdf]

Next: Iterative seislet thresholding Up: Method Previous: Method

2015-09-15