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    青藏高原东南缘PmP波数据集构建及识别模型训练

    李澍辰 孙安辉 李天觉 童平 房立华 安艳茹 张莹莹 赵盼盼 杨峰

    李澍辰, 孙安辉, 李天觉, 童平, 房立华, 安艳茹, 张莹莹, 赵盼盼, 杨峰, 2026. 青藏高原东南缘PmP波数据集构建及识别模型训练. 地球科学, 51(3): 1169-1181. doi: 10.3799/dqkx.2025.128
    引用本文: 李澍辰, 孙安辉, 李天觉, 童平, 房立华, 安艳茹, 张莹莹, 赵盼盼, 杨峰, 2026. 青藏高原东南缘PmP波数据集构建及识别模型训练. 地球科学, 51(3): 1169-1181. doi: 10.3799/dqkx.2025.128
    Li Shuchen, Sun Anhui, Li Tianjue, Tong Ping, Fang Lihua, An Yanru, Zhang Yingying, Zhao Panpan, Yang Feng, 2026. Constructing and Training of a Deep Learning Dataset for PmP Waves in the Southeastern Tibetan Plateau. Earth Science, 51(3): 1169-1181. doi: 10.3799/dqkx.2025.128
    Citation: Li Shuchen, Sun Anhui, Li Tianjue, Tong Ping, Fang Lihua, An Yanru, Zhang Yingying, Zhao Panpan, Yang Feng, 2026. Constructing and Training of a Deep Learning Dataset for PmP Waves in the Southeastern Tibetan Plateau. Earth Science, 51(3): 1169-1181. doi: 10.3799/dqkx.2025.128

    青藏高原东南缘PmP波数据集构建及识别模型训练

    doi: 10.3799/dqkx.2025.128
    基金项目: 

    中国地震局地震预报重点实验室专项基金项目 2023030104

    国家自然科学基金项目 42474134

    国家自然科学基金项目 41974050

    国家自然科学基金项目 42374081

    详细信息
      作者简介:

      李澍辰(2000-),男,硕士研究生,研究方向为人工智能方法拾取震相.ORCID:0009-0008-8364-7163. E-mail:lishuchen00@163.com

      通讯作者:

      孙安辉,ORCID: 0000-0003-3809-7904. E-mail: sah@ief.ac.cn

    • 中图分类号: P315

    Constructing and Training of a Deep Learning Dataset for PmP Waves in the Southeastern Tibetan Plateau

    • 摘要: 莫霍面反射波PmP的射线路径与初至Pg波、Pn波不同,其传播特性与发震构造环境密切相关,可为研究地壳深部结构与莫霍面不连续性提供关键信息.识别PmP波的主要挑战是它们的稀缺性,且人工拾取需要耗费大量的人力.为改善这一问题,利用青藏高原东南缘的固定台站(2009—2022年)和流动台阵(2011—2013年)记录的波形,通过手动拾取和振幅比值检验得到了1 713个PmP震相,结合半自动拾取流程(基于振幅阈值筛选和质点运动检验)提取1 536个PmP震相,构建了高质量PmP数据集.对基于深度神经网络的PmPNet进行重新训练,构建了适配青藏高原东南缘的新模型PmPNet-SET_V1.0和PmP-traveltime-Net-SET_V1.0,其中PmPNet-SET_V1.0模型的F1分数为0.863 7,精确率为86.6%,召回率为84.8%,并将该区域内高质量PmP波数量增加至6 268个.所有PmP拾取结果通过严格的人工检验并与理论走时对比,确保了可靠性.研究表明,训练参数对采集波形的数量和质量具有显著影响.此外,基于所构建的PmP数据集,本研究初步获得了青藏高原东南缘区域莫霍深度分布,其呈现西北深,东南浅的趋势,与前人反演结果的样式相近.

       

    • 图  1  青藏高原东南缘地区的构造背景

      a. 青藏高原东南部示意图,据Han et al.(2020);黑色线为研究区域的断层,橙色点为2009—2022年间震级大于6.0的地震的位置,每个地震都标注了事件年份和震级;b. 青藏高原东南缘处SWChinaCVM-MOHO-1.0莫霍深度图和台站分布图,据Chen et al.(2021);黑色线为研究区域的断层,红点表示CREDIT-X1local数据集(2011—2013年)中的流动台站,蓝点表示CSNCD数据集(2009—2022年)中的固定台站;c. 局部Pg波、PmP波和Pn波的射线路径;其中的红星表示震源,黑色倒三角形表示地表上的台站,蓝色实线表示P波的射线路径

      Fig.  1.  The tectonic setting of the SE Tibetan Plateau

      图  2  PmP半自动流程的三个步骤,每一步的示例均展示在右侧

      a. 原始波形与其预处理波形的对比;b. 利用振幅比度量自动检测可能的PmP震相的过程;c. 在同一台站记录的垂直分量地震图,以及其对应平面内P波(蓝色曲线)和PmP波(红色曲线)的质点运动,以及它们主要的极化方向

      Fig.  2.  The three-step process is designed to pick local PmP waves with examples for each step shown on the right-hand side

      图  3  CREDIT-X1local中通过PmP半自动流程的PmP数据集

      a. 原始波形和预处理波形的对比示例;b. 所有被拾取到的PmP波的反射点(红点)的空间分布;c. PmP-P到时差与震中距的相关性;d. 单台多事件示例中台站和震源的方位视图;e. 图d中在各台站记录的PmP震相示例,所有波形按初至P波到时(蓝线)对齐,并根据震源深度(evdp)和震中距(dist)进行排序,PmP到时由红线表示;f. PmP波和Pg波的振幅比分布情况

      Fig.  3.  PmP datasets in CREDIT-X1local after PmP-picking workflow

      图  4  PmPNet的训练过程

      当达到预定的最大迭代次数时,PmPNet的训练阶段即为完成

      Fig.  4.  PmPNet training flow

      图  5  当使用不同学习率对数据集进行训练时,PmPNet训练和验证的结果

      a~c. 使用高学习率训练和验证的结果;d~f. 使用低学习率训练和验证的结果;g~i. 联合使用两种学习率训练和验证的结果.a、d、g. 随着迭代次数的增加,总的损失函数减少,F1分数增加,经过足够多的迭代次数训练后变得稳定;b、e、h.验证集上的精度‒召回率曲线(相关数据见附录A);c、f、i. 验证集上预测值和真实值之间的PmP走时残差

      Fig.  5.  Training and validation performance of PmPNet when applied to real data with different learning rates

      图  6  PmP-traveltime-Net训练和验证的结果

      a. 损失函数迭代变化;b. 验证集走时残差分布;c. 震中距与PmP走时关系

      Fig.  6.  Training and validation performance of PmP- traveltime-Net

      图  7  PmPNet-SET_V1.0和PmP-traveltime-Net-SET_V1.0在CREDIT-X1local的PmP波自动拾取结果

      a. 单台多事件示例中震源和台站的分布.PmP震相由同一个台站(黑色方块)记录得到,各个震源由红色星星标记;b. 图a中在各台站记录的PmP震相示例. 所有波形按初至P波到时(蓝线)对齐,并根据震源深度(evdp)和震中距(dist)进行排序.PmP半自动流程拾取的PmP到时由紫线表示,PmPNet-SET_V1.0拾取的PmP到时由红线表示;c~d. 另一组与图a~b相同的示例;e. PmPNet-SET_V1.0拾取的PmP震相与PmP半自动流程选取的震相对比. 它还显示了这两种方法拾取的PmP震相波形一致的数量及其到时差异

      Fig.  7.  CREDIT-X1local's PmP wave automatic picking result of PmPNet-SET_V1.0 and PmP-traveltime-Net-SET_V1.0

      图  8  构建速度模型的两种不同方法

      a. 反射点的一维分层速度模型的示例(表 1);b. 根据反射点的莫霍深度扩张/压缩SWChinaCVM-2.0速度模型的示例(表 2

      Fig.  8.  Two different approaches of constructing the velocity model

      图  9  使用不同的速度模型对CREDIT-X1local的PmP波自动拾取结果

      a. 单台多事件震源和台站的分布;b. 多事件PmP震相示例.所有波形按初至P波到时(蓝线)对齐,并根据震源深度(evdp)和震中距(dist)进行排序.PmP半自动流程拾取的PmP到时由橙线表示,PmPNet拾取的PmP到时由红线表示.先前的速度模型计算的PmP理论到时由绿线表示,新的速度模型计算的PmP理论到时由紫线表示

      Fig.  9.  CREDIT-X1local's PmP wave automatic picking result with different compositions of velocity model

      图  10  在其他条件不变的情况下,震中距与PmP-P理论走时之差之间的相关性

      蓝色区域是初至P波窗区;红色区域是PmP波窗区;绿框中的波段很容易被误认为是PmP波

      Fig.  10.  When other conditions remain unchanged, the correlation between epicentral distance and PmP-P travel time

      图  11  莫霍深度对比

      a. 本研究反演得到的莫霍深度,黑线为研究区域的断层;b. SWChinaCVM-MOHO-1.0模型的莫霍深度

      Fig.  11.  The comparison of Moho depth

      表  1  基于反射点的SWChinaCVM-2.0一维分层速度模型示例

      Table  1.   A sample of choosing the reflection point's 1-D layered velocity model for choosing the reflection point

      模型上边界深度($ \mathrm{k}\mathrm{m} $) P波速度模型($ \mathrm{k}\mathrm{m}\bullet {\mathrm{s}}^{-1} $)
      0 5.26
      2.5 5.32
      5 5.50
      7.5 5.71
      10 5.83
      15 5.95
      20 5.97
      30 6.03
      40 6.19
      50 6.52
      60 6.81
      70 7.28
      80 7.65
      下载: 导出CSV

      表  2  基于反射点的莫霍深度压缩/扩张后的SWChi naCVM-2.0一维分层速度模型示例

      Table  2.   A sample of compressing the reflection point's model of SWChinaCVM-2.0 according to the reflection point's Moho depth

      模型上边界深度($ \mathrm{k}\mathrm{m} $) P波速度模型($ \mathrm{k}\mathrm{m}\bullet {\mathrm{s}}^{-1} $)
      0 5.26
      1.97 5.32
      3.94 5.50
      5.91 5.71
      7.88 5.83
      11.82 5.95
      15.76 5.97
      19.7 6.03
      23.64 6.19
      27.58 6.52
      31.52 6.81
      39.4 7.28
      47.28 7.65
      下载: 导出CSV
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