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地震 ›› 2023, Vol. 43 ›› Issue (4): 76-100.doi: 10.12196/j.issn.1000-3274.2023.04.006

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基于模式和广义射线理论研究水平层状介质中面波模式的接触现象

王少曈, 鲁来玉   

  1. 中国地震局地球物理研究所, 北京 100081
  • 收稿日期:2023-06-05 修回日期:2023-06-28 出版日期:2023-10-31 发布日期:2023-12-29
  • 通讯作者: 鲁来玉, 研究员。 E-mail: laiyulu@cea-igp.ac.cn
  • 作者简介:王少曈(1993-), 男, 北京市人, 博士研究生, 主要从事理论地震学研究。
  • 基金资助:
    国家自然科学基金地震联合基金资助项目(U1839209)

Study on the Mode-kissing of Surface Waves Based on the Theory of the Mode and Generalized Ray

WANG Shao-tong, LU Lai-yu   

  1. Institute of Geophysics, China Earthquake Administration, Beijing 100081, China
  • Received:2023-06-05 Revised:2023-06-28 Online:2023-10-31 Published:2023-12-29

摘要: 在近地表面波勘探中, 尤其对于典型沉积盆地的探测, 基于观测数据得到的频率-相速度域的能谱中, 通常可以观察到基阶和一阶模式的模式接触现象(Mode-kissing)。 基于模式理论, 频率域中面波模式对应由频散方程的根给出的一系列极点。 基于广义射线理论, 时空域的多径, 造成了频率域中的多模。 本文结合广义射线理论和简正模理论研究广义射线理论中极和极两个表面波极点贡献对频散曲线的影响, 解释实际观测的模式接触现象。 基于两层介质模型, 分析下层半空间S波速度β(2)变化时, 随极点在复射线参数平面变化, 引起的基阶和一阶模式的频散曲线、 本征位移和质点偏振的变化特征。 研究发现, 模式接触现象出现在复射线参数平面内, 极越过1/β(2)表示的支点, 基本进入简正模区域时。 与该极点对应的一阶露能模式, 其地表质点轨迹为顺进椭圆, 但本征位移随深度的变换表现出经典表面波特征, 能量主要集中在地表。

关键词: 广义射线, 本征值, 频散曲线, Cagniard-de Hoop方法, 广义反、 透射系数, 自由表面波, 能陷波

Abstract: In near-surface surface wave exploration, especially in typical sedimentary basins, mode-kissing of the fundamental and first-order modes is often observed for the dispersion image in the frequency-phase velocity domain. In the mode theory of waves, surface wave mode in the frequency domain is associated with a series of poles determined by the dispersion equation. In the generalized ray theory, the multipath in the spatial-temporal domain gives rise to the multimode in the frequency domain. Combined with the generalized theory and the mode theory, the influence of the $\bar{P}$ pole and the $\bar{S}$ pole on dispersion curves is studied to explain the mode-kissing phenomenon. For a two-layer model, the characteristics of the dispersion curves, eigen displacement, and polarization of the particle, which varies with the moving of $\bar{P}$ pole in the complex ray parameter plane, are studied by changing the S wave velocity β(2) of the bottom half space, both for the fundamental and the first overtone. It is found that mode-kissing appears when the $\bar{P}$ pole passes through the branch point 1/β(2) in the complex ray parameter plane and just enter the area belongs to the normal mode. The particle motion of the first leaky mode corresponding to the $\bar{P}$ pole is a prograde ellipse, but the eigen displacement shows the characteristic of the classical surface wave, i.e., the displacement mainly concentrates near the surface and decays rapidly with depth.

Key words: Generalized ray, Eigenvalue, Dispersion curve, Cagniard-de Hoop method, Generalized reflection-transmission coefficient, Free surface wave, Trapped wave

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