地震作用下横断层地质金属成矿带电法找矿成果研究

深部矿产资源勘探是未来勘探的必然趋势.地震作用下的横断层地质构造对金属矿、 能源矿等矿产资源的分布具有重要影响,拥有较大的找矿潜力.对于地震作用下横断层地质等条件复杂的场合,采用高密度电阻率法、 激发极化法和可控源音频大地电磁法等单一电法勘探可能存在找矿效果不佳的问题,有必要研究更为有效的找矿技术方法.首先阐述了激发极化法、CSAMT法等电法勘探的基本内容和各自优缺点;然后,在分析地震作用下横断层地质特征的基础上,研究并提出了基于激发极化法和CSAMT的综合找矿法.基于激发极化法和CSAMT的综合找矿法能有效反映地下地电差异,在大深度范围有效反应地电断面电阻、 极化率参数,互相校正验证;结合已有地质物探资料,推断地下异常,提高横断层的金属矿产勘探效率和效果.将本文的研究成果应用于某横断层地质区域的金属矿勘探实践,取得了良好的勘探效果.实践表明本文所提方法有效、 可行.     

宁河-昌黎断裂基于浅层地震勘探资料研究

宁河—昌黎断裂长约170 km,为燕山隆起、山海关隆起与黄骅拗陷的分界断裂,断裂西南起自宁河,向东北经南套南、大夫庄南、杨家坨,过昌黎转向东入海,断裂走向NE50°~70°,倾向SE,为上陡下缓的铲形正断层,该断裂为一条地壳基底深断裂,控制了南侧黄骅坳陷北段中、新生代沉积。河北省工程地震勘察研究院于2007年、2014年先后在昌黎、滦南、唐海、丰南布设了4条浅层地震勘探测线对宁河—昌黎断裂进行了探测,浅层地震勘探应用美国GEOMETRICS公司STRATAVISOR NX96高分辨数字地震勘探系统,采用70 kg冲击震源,单边激发多次覆盖观测系统,覆盖次数12次。应用Vista地震处理软件系统,通过对数据进行真振幅恢复、地表一致性振幅补偿等处理方法,获得高质量的地震勘探时间剖面。为获得断裂活动时代的重要信息,通过浅层地震勘探处理过程中的中间数据获得地震剖面时—深转换速度参数,从而获得地震勘探深度剖面,结合测线附近地层层序资料,与地震勘探深度剖面进行对比分析,从而获得断裂的上断点埋深和最新活动时代认识。浅层地震勘探剖面揭示,宁河—昌黎断裂浅部由一条主断层和一条次级断层组成;断层上断点埋深40~110 m,断裂活动时代具有分段活动特征,断裂北段活动时代为晚更新世早期,南段为晚更新世中期;断裂走向为北东的段落,为正断层,走向为北西的段落,以走滑运动为主。     

A Preliminary Analysis of the Seismogenic Structure of the Akto MS6.7 Earthquake Sequence on November 25, 2016

In this study,data from the Xinjiang regional network and IRIS shared global stations are used to relocate the Akto M_S6. 7 earthquake sequence on November 25,2016 by using double difference location method. Three earthquakes of M_S4. 8,M_S6. 7 and M_S5. 0 are inverted by using the g CAP method,and the focal mechanism solutions are obtained.According to the results of relocating,the location of the main shock is 39. 22°N,73. 98°E,the distribution of the earthquake sequence is about 70 km in length,and the focal depth is mainly within the range of 5-20 km. The plane and depth profiles of the earthquake sequence show that aftershocks extended in SEE direction after the main shock and the dip angle of fault plane is steep. Focal mechanism results show that the three earthquakes are characterized by strike-slip movement. Based on the results of field geological investigation,it is inferred that the seismogenic fault of the Akto earthquake is Muji fault,which is located at the northernmost end of the Kongur extensional system.The possible cause of this earthquake is that the Indian Plate continues to push northward,and during this compression process,the Indian Plate is affected by the clockwise rotation of the Tarim basin,which causes the accumulation of right-lateral action of the Muji fault,resulting in this earthquake.     

Monitoring Contact State of Laboratory Fault with Coda Transmission Waves

We monitored the amplitude changes of coda transmission waves around 500kHz across the frictional interface of a simulated 1.5-meter-long fault during normal stress holding test. We find that the amplitude of coda transmission waves increases with the logarithm of stationary contact time. Localized increase amounted to a level ranging from 4% to 16% along the fault is observed during the 1-hour experiment. We discuss that the frictional strength at mesoscopic scale, which is related to the amplitude of coda transmission waves, is responsible for the phenomenon. Combining the reported method with other complementary approaches will enhance the understanding of fault mechanism either at laboratory or on-site applications.     

断裂带首波研究进展

断裂带首波是沿着存在物性差异界面传播的一种地震折射波,在传播过程中携带了断裂带的重要信息,对分析和研究断裂带以及附近区域的精细结构提供了一种新的分析方法。本文主要阐述断裂带首波的产生原理、波形特征、识别及分析方法等,介绍目前国际上识别及利用断裂带首波开展断裂带特征方面的研究现状,并针对地震危险区域存在物性差异的断裂带,提出可结合密集台阵观测技术,利用断裂带首波进行断裂带精细结构探测及其变化监测研究,提高潜在孕震环境及发生机理的认识水平。     

2013年芦山地震震源区地壳介质地震波速变化的特征分析

为探究芦山M7.0级地震后5年多来,震源区龙门山断裂带西南段介质波速的变化规律,本文基于2012年4月至2018年4月共6年的连续波形数据,运用移动窗互谱与频域偏振等分析方法,结合背景噪声源的特性,对不同深度范围内的相对波速变化以及震后的恢复过程与机制进行了研究.获得的主要认识包括：（1）年尺度而言,震源区周期为1~20 s的背景噪声场相对稳定,但成分复杂、2~10 s频带内至少存在2个能量相对稳定的噪声源;不同周期噪声的能量,在月变与季节性上的变化特征差异明显.（2）获得了长时间尺度、不同频带内介质相对波速的背景变化水平,1~2 s、2~4 s的波动幅度（约为±0.04%）与季节性变化规律强于4~10 s、10~20 s的,结合与降雨量相关的地下水位模型能很好地解释其变化规律.（3）震源区的同震波速降低现象清晰,降幅约为0.08%~0.1%;空间上,波速下降最为显著的区域主要集中在龙门山断裂带两侧约70 km范围内,其中四川盆地一侧平均约为0.1%,略高于青藏高原（0.08%）一侧;在断裂带内的降速不显著.对不同子频带进行测量的结果显示,震后除10~20 s外,其余3个子频带的相对波速在震后较短时间内（约20天左右）均出现较大幅度的波速降低现象,其中4~10 s的平均降速最大（约为0.08%）,分析认为主震及大量余震的松弛效应是引起介质波速下降的主要原因.（4）震后大约1年左右,波速变化基本恢复到震前水平,且至2018年4月前未观察到大幅的波速变化现象,总体上各频带内的结果均沿零线小幅波动.     

郯庐断裂带中南段及邻区基于背景噪声的瑞利波群速度层析成像

本文收集了郯庐断裂带中南段及邻区省属和市县地震台网共261个宽频带地震台站2015年1月至2016年12月间的垂直向连续波形资料,利用长时间序列背景噪声互相关法提取台站对之间的经验格林函数,采用时频分析法提取瑞利面波混合路径频散曲线.通过质量控制和严格筛选后得到了15627条路径上的群速度频散曲线,重新构建了郯庐断裂带中南段及邻区瑞利波5～50s、分辨率为0.75°×0.75°的群速度分布图像.分析研究了6个周期的群速度分布图像和3条不同方向的纵向周期剖面,这些图像揭示了郯庐断裂带中南段及邻区地壳上地幔速度结构具有横向分块和纵向成层的非均匀性特征.结果表明,短周期(6s、10s)的群速度分布与地表地质和构造特征密切相关.拥有较厚沉积层的苏北盆地、合肥盆地及河淮盆地等显示为低速,而基岩广泛出露的鲁西隆起、大别—苏鲁造山带、扬子克拉通及华南褶皱系则呈现出大面积的高速异常.随着周期的递增(15s、20s),群速度分布受地表地质构造的影响逐渐弱化.受地壳厚度和莫霍面附近的速度差异影响,大别和苏鲁地区在较长周期(25s、30s)群速度图上表现出相对较低的速度,这可能与这些地方Moho面埋藏较深有关.纵向剖面显示,苏鲁—大别造山带及其高压、超高压变质带不仅在浅地表具有基本相同的地形地貌和构造特征,地壳内也有着极为相似的Rayleigh波群速度分布特征.壳内群速度分布总体上表现为上凸下凹状,形状似一"哑铃".上地壳具有上凸下凹的形态、相比邻区具有较高的群速度值;中地壳低速;下地壳上凸下凹且埋藏较深,反映出具有陆陆碰撞造山的残留山根特征.苏鲁及大别两地自浅地表至上地幔具有相似的Rayleigh波群速度分布不仅为二者被左旋走滑的郯庐带平移错开提供了佐证资料,同时也为郯庐带的形成与演化提供了地震学依据.     

利用模板匹配技术检测米尺度岩石断层黏滑实验中的声发射事件

声发射观测是岩石摩擦实验中研究强震孕育机制的重要观测手段之一.传统的声发射观测以触发记录为主,难以捕捉并提取微弱的声发射信号.近年来天然地震学中发展的模板匹配技术可以在连续波形记录中识别出微弱的事件,大大提升事件检测能力.本文发展了适用于多通道连续记录的声发射信号的模板匹配技术,并将该技术应用于分析米尺度岩石断层黏滑失稳过程.研究结果显示:模板匹配技术识别出的声发射数量约为传统方法识别的5倍,相对完备震级降低约0.3.临近失稳,检测目录完备震级以上声发射率表现出幂律增加的特征,且声发射事件聚集在失稳破裂起始点附近.失稳后,检测目录完备震级以上声发射率表现出幂律衰减,其中失稳后早期表现出较慢的衰减速度.另外,失稳后早期声发射事件表现出随对数时间沿断层迁移的趋势.最后,通过与天然地震学观测的结果对比表明,声发射模板匹配识别技术是研究大尺度岩石摩擦滑动失稳过程中前震和余震时空演化规律的有效手段,该技术助于在方法上为室内实验和野外观测进行融合研究提供思路.     

CHARACTERISTICS OF SATELLITE GRAVITY FIELD AND SEISMOGENIC MECHANISM IN THE LONGMENSHAN FAULT ZONE

Longmenshan fault zone is a famous orogenic belt and seismic zone in the southeastern Tibetan plateau of China. The Wenchuan M_S8.0 earthquake on May 12, 2008 and the Ya'an M_S7.0 earthquake on April 20, 2013 occurred in the central-southern part of Longmenshan fault zone. Because of its complex geological structures, frequent earthquakes and special geographical locations, it has attracted the attention of many scholars around the world. Satellite gravity field has advantages in studying gravity field and gravity anomaly changes before and after earthquake. It covers wide range, can be updated regularly, without difficulty in terms of geographical restrictions, and is not affected by environmental factors such as weather, terrain and traffic. Therefore, the use of high-precision Earth satellite gravity field data inversion and interpretation of seismic phenomena has become a hot topic in earth science research. In order to understand satellite gravity field characteristics of the Longmenshan earthquake zone in the southeastern Tibetan plateau and its seismogenic mechanism of earthquake disasters, the satellite gravity data was used to present the terrain information of the study area. Then, by solving the regional gravity anomaly of the Moho surface, the crustal thickness of the study area was inverted, and the GPS velocity field data was used to detect the crustal deformation rate and direction of the study area. Combining the tectonic setting of the Longmenshan fault zone and the existing deep seismic sounding results of the previous researchers, the dynamic characteristics of the gravity time-varying field after the earthquake in the Longmenshan earthquake zone was analyzed and the mechanism of the earthquake was explored. The results show that the eastward flow of deep materials in the eastern Tibetan plateau is strongly blocked at the Longmenshan fault zone. The continuous collision and extrusion process result in a "deep drop zone" in the Moho surface, and the long-term stress effect is conducive to the formation of thrust-nappe and strike-slip structures. The Longmenshan earthquake zone was in the large-scale gradient zone of gravity change before the earthquake, the deep plastic fluid material transport velocity differed greatly, the fluid pressure was enhanced, and the rock mechanical strength in the seismic source region was weakened, which contributed to the intrusion of crustal fluid and the upwelling of the asthenosphere. As a result, the continuous accumulation of material and energy eventually led to continuous stress imbalance in the deep part and shear rupture of the deep weak structure, causing the occurrence of the thrust-nappe and strike-slip earthquake.