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Elastic Wave Diffraction Fields Generated by Surface Excitation of a Crystal

机译:晶体表面激发产生的弹性波衍射场

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The angular spectrum theory is currently used to analyse the diffraction fields generated by a finite aperture source on surface of the anisotropic medium. Only is the anisotropy of the propagation velocity regarded in such a sclar theory. So this theory is insufficient and exists many shortcomings. Since the elastic wave in solid is the vector field, the diffraction patterns for various wave modes, various components of each mode and various excitated sources are different generally. The angular spectrum theory neglected actual physical field can only give a relative distribution of phenomenological field. According to the generalized excitation theory in our previous works, the diffraction elastic wave fields excitated by the surface finite-aperture source are obtained in this paper. As an example, the calculation results of the diffraction fields for YZ quartz are given and compared with that of the angular spectrum theory.
机译:目前,角谱理论用于分析由各向异性介质表面上的有限孔径源产生的衍射场。在这样的理论中只考虑了传播速度的各向异性。因此,该理论是不足的,并且存在许多缺点。由于固体中的弹性波是矢量场,因此各种波模式,每种模式的各个成分以及各种激发源的衍射图样通常是不同的。忽略实际物理场的角谱理论只能给出现象学场的相对分布。根据我们以前工作中的广义激励理论,得到了表面有限孔径源激发的衍射弹性波场。例如,给出了YZ石英衍射场的计算结果,并将其与角谱理论的计算结果进行了比较。

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