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Multifocusing homeomorphic imaging Part 1. Basic concepts and formulas

机译:多聚焦同胚成像第1部分。基本概念和公式

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The decomposition of a total wave field recorded on a set of seismic traces on parts corresponding to different body waves is one of the fundamental problems of data processing. The central point of this problem is the correlation procedure for a seismic event (wave) on a set of recorded traces. in order to implement this procedure, it is necessary to have a local time correction formula for a family of source-receiver pairs arbitrarily distributed around a chosen central pair. This formula is derived in the work for a 2D seismic medium of arbitrary structure using a new homeomorphic imaging method called multifocusing. The presentation of multifocusing is divided into two parts: the basic ideas and concepts of the method, the time correction formula and associated geometrical relationships form Part 1. The main characteristic of the multifocusing approach is the consideration of the geometry of all possible wave fronts, which could be formed in the vicinity of a chosen central source-receiver pair. Provided that a target wave exists on a chosen central trace, then there is also a corresponding central ray and an infinite family of surrounding wave tubes. The basic idea of the multifocusing technique is based on the association of any pair of traces recorded in the vicinity of the central trace with certain ray tube belonging to the family. This association can be always found. Considering this ray tube, the local time correction formula is obtained, assuming a spherical approximation of two tube cross sections at the end points of central ray. In the case of a central ray with non-zero offset, the formula consists of the following parameters: two velocities near the source and receiver locations, two angles (departure and arrival) and two pairs of dual curvatures of tube cross-sections at the ray end points. The first four parameters are common for all traces, the pairs of dual curvatures are, as a rule, specific for the chosen pair of traces; the formula thus obtained could not be directly used in practice. The essential part of the first paper is devoted to the parameterization of the family of dual curvatures. The exact formulas derived for these curvatures include as parameters, a pair of dual curvatures of two chosen fundamental ray tubes. Different choices for the fundamental ray tubes are considered and important relationships between the dual curvatures and spreading functions for these tubes are established. They are the generalization of the Hubral formula [Hubral, P., 1983. Computing true amplitude reflections in a laterally inhomogeneous earth. Geophysics 48, 1051-1062] and known reciprocity relations. In the case of a zero-offset central ray, most important for reflection shooting, the formulas derived are significantly simplified and involve four parameters only. The results obtained can be used not only in the multifocusing method, but also in migration and forward modeling.
机译:记录在对应于不同体波的部分上的一组地震迹线上的总波场的分解是数据处理的基本问题之一。这个问题的中心点是一组记录的迹线上地震事件(波)的相关过程。为了实施该过程,有必要为围绕所选择的中心对任意分布的源-接收器对系列提供本地时间校正公式。该公式是在工作中使用称为多重聚焦的新同胚成像方法针对任意结构的2D地震介质得出的。多重聚焦的介绍分为两部分:方法的基本思想和概念,时间校正公式以及相关的几何关系,构成第1部分。多重聚焦方法的主要特征是考虑所有可能的波阵面的几何形状,可以在选定的中央源接收器对附近形成。假设目标波存在于选定的中心迹线上,那么还将存在相应的中心射线和无限大的周围波管族。多聚焦技术的基本思想是基于记录在中央迹线附近的任何一对迹线与属于该族的某些射线管的关联。总是可以找到这种关联。考虑到这种射线管,假设中心射线端点处两个射线管截面的球面近似,可以得出局部时间校正公式。对于中心射线具有非零偏移的情况,该公式由以下参数组成:源和接收器位置附近的两个速度,两个角度(离开和到达)以及在处的两对管截面的双曲率射线终点。前四个参数对于所有迹线都是通用的,通常,双曲率对特定于所选的迹线对;这样获得的公式不能直接用于实践中。第一篇论文的关键部分致力于双曲率族的参数化。为这些曲率得出的精确公式包括两个选定的基本射线管的一对双曲率作为参数。考虑基本射线管的不同选择,并为这些射线管建立双曲率和扩散函数之间的重要关系。它们是Hubral公式的概括[Hubral,P.,1983。计算横向不均匀地球中的真实振幅反射。地球物理学48,1051-1062]和已知的互惠关系。在零偏移中心射线的情况下(对于反射射击而言最重要),导出的公式已大大简化,仅包含四个参数。获得的结果不仅可以用于多重聚焦方法,而且可以用于迁移和正向建模。

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