2019年四川长宁MS6.0地震序列S波分裂变化特征

Variation characteristic of S-wave splitting on the 2019 Changning MS6.0 earthquake sequence,Sichuan

  • 摘要: 本文采用质点运动判别与偏振分析相结合的方法对2019年四川长宁MS6.0地震震源区10个台站于2013年4月25日至2019年7月31日记录到的波形数据进行S波分裂参数测定,其中9个台站获取4条以上有效S波分裂参数。结果表明,震源区各台站的S波分裂参数不仅在空间上存在分区特征,还会随时间发生改变。快波偏振方向在空间上的分区特征大体为:位于震源区东南段的三个台站的快波偏振优势方向主要为NE向,与震源区东南段的主压应力方向基本一致;位于研究区西北段的台站,其快波偏振优势方向为近EW向,与震源区西北段的主压应力方向基本一致。但由于受到震源区地壳应力和复杂构造的共同影响,CJW,GXA和LQS三个台站都有两个快波偏振优势方向。快波偏振方向随时间的变化为:主震后各台站的快波偏振方向都出现离散度增大而后又逐渐趋于一致的现象;CJW台的快波偏振方向在主震前三个月发生了改变,体现了孕震过程中随着应力的不断积累,其各向异性特征由主要受构造控制转变为受应力控制。各台站的归一化慢波时间延迟随台站距主震和余震密集区距离的增加而减小,反映了长宁地震孕震过程中余震密集区的应力积累和释放明显强于周边区域。此外,主震发生前6个月左右CNI台的慢波时间延迟出现明显下降,地震发生后又迅速上升,反映出长宁地震震前的应力积累以及震后应力突然释放使上地壳中微裂隙的几何形态发生了改变。

     

    Abstract: In this paper, the S-wave splitting parameters of the waveform data recorded at 10 stations in the source area of the 2019 Changning MS6.0 earthquake, Sichuan, from April 25, 2013 to July 31, 2019 were measured by the particle motion discriminant method combined with the polarization analysis method. More than four effective S-wave splitting parameters are obtained at nine stations. The results show that the S-wave splitting parameters at the stations in the studied region are characterized by partition in space and variation over time. The characteristics of fast wave polarization direction in space are as follows: the predominant polarization direction of fast S-wave at three stations in the southeastern source area of the Changning earthquake is in the direction of NE, which is consistent with direction of regional principal compressive stress in the southeastern source area. In the northwestern source area, the predominant polarization directions of fast S-wave, nearly EW, is consistent with the directions of regional principal compressive stress in the northwestern source area. Due to the combining effect of crustal stress and complex fault structure, the three stations CJW, GXA and LQS all have two predominant polarization directions of fast S-wave. The polarization directions of fast S-wave change with time as follows: After the main shock, the polarization directions of fast S-wave at each station gradually tended to be convergence after the dispersion increases; the polarization directions of fast S-waves at the station CJW changed three months before the main shock, indicating that with the accumulation of the stress during the seismogenic process, the anisotropic characteristics at the station CJW are controlled mainly by stress instead of structure. As for the temporal distribution, the average normalized delay time of slow S-wave at each station decreased as the distance increasing from the main shock and aftershock dense area to stations, reflecting the stronger accumulation and releasing of stress during seismogenic process in the aftershock dense area. In addition, the normalized delay time of slow S-wave at the station CNI decreased significantly about six months before the main shock, and increased rapidly after the main shock, suggesting the accumulation of stress before the earthquake and the abrupt release of stress after the earthquake lead to the change in geometry of the micro-cracks in upper crust.

     

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