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Review of the Research of the 2011 Mw9.0 Tohoku-Oki Earthquake
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作者 Shao Zhigang Wang Peng Li Haiyan 《Earthquake Research in China》 CSCD 2017年第3期309-333,共25页
On March 11,2011, a M_W9.0 earthquake occurred in the Japan Trench, causing tremendous casualties,and attracting extensive concern. Based on the results of related research,this paper analyzes the observations,phenome... On March 11,2011, a M_W9.0 earthquake occurred in the Japan Trench, causing tremendous casualties,and attracting extensive concern. Based on the results of related research,this paper analyzes the observations,phenomena and understandings of the earthquake from varied aspects,and obtains four main conclusions.(1) The earthquake,occurring in the subduction zone in the Japan Trench located in the northwest boundary of the pacific plate has two zones of concentrated coseismic slip at different depths,and the slip in the deep zone is relatively small. Though there have been many M7. 0 historical earthquakes,slips in the shallow zone are large,but there have been few historical strong earthquakes.(2) Constrained by GPS data,the study of fault movement shows that fault movement in the Japan Trench has a background of widely distributed stability and locking( the locking zone is equivalent that of coseismic rupture zone). Perturbation occurred after the 2008 M8. 0 Hokkaido earthquake,several M7. 0 events had after slips larger than the coseismic slip,and two obvious slow slip events were recorded in 2008 and2011. Eventually,the March 9,2011 M7. 0 foreshock and the March 11,2011 M_W9.0 mainshock occurred. The pre-earthquake changing of the fault movement in the Japan Trench is quite clear.(3) Traditional precursory observation show no obvious anomaly,possibly due to monitoring reason. Anomaly before earthquake consists of high stress state in focal zone reflected by some seismic activity parameters,short period anomaly in regional ground motion,etc.(4) The analysis of physical property in focal zone aroused more scientific issues,for example,is there obvious difference between physical property in focal zone and its vicinity? Does frictional property of fault determine seismogenic ability and rupture process? Whether pre-earthquake fault movement include pre-slips? Could deep fluid affect fault movement in focal zone? Experience is the best teacher,and authors hope this paper could be a modest spur to induce others in basic research in earthquake forecast and prediction. 展开更多
关键词 The 2011 mw9.0 JAPAN earthquake earthquake prediction SEISMIC MONITORING earthquake RESEARCH
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Spatio-temporal characteristics of aftershocks and seismogenic structure of the 2011 Mw9.0 Tohoku earthquake,Japan 被引量:2
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作者 Farah Lazzali 《Earthquake Science》 CSCD 2012年第3期219-227,共9页
The Tohoku megathrust earthquake, which occurred on March 11, 2011 and had an epicenter that was 70 km east of Tohoku, Japan, resulted in an estimated ten′s of billions of dollars in damage and a death toll of more t... The Tohoku megathrust earthquake, which occurred on March 11, 2011 and had an epicenter that was 70 km east of Tohoku, Japan, resulted in an estimated ten′s of billions of dollars in damage and a death toll of more than 15 thousand lives, yet few studies have documented key spatio-temporal seismogenic characteristics. Specifically, the temporal decay of aftershock activity, the number of strong aftershocks (with magnitudes greater than or equal to 7.0), the magnitude of the greatest aftershock, and area of possible aftershocks. Forecasted results from this study are based on Gutenberg-Richter’s relation, Bath’s law, Omori’s law, and Well’s relation of rupture scale utilizing the magnitude and statistical parameters of earthquakes in USA and China (Landers, Northridge, Hector Mine, San Simeon and Wenchuan earthquakes). The number of strong aftershocks, the parameters of Gutenberg-Richter’s relation, and the modified form of Omori’s law are confirmed based on the aftershock sequence data from the Mw9.0 Tohoku earthquake. Moreover, for a large earthquake, the seismogenic structure could be a fault, a fault system, or an intersection of several faults. The seismogenic structure of the earthquake suggests that the event occurred on a thrust fault near the Japan trench within the overriding plate that subsequently triggered three or more active faults producing large aftershocks. 展开更多
关键词 2011mw9.0 Tohoku earthquake AFTERSHOCK seismogenic structure
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日本海沟俯冲带M_W9.0地震震源区应力场演化分析 被引量:10
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作者 杨佳佳 张永庆 谢富仁 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2018年第4期1307-1324,共18页
于2011年3月11日发生在日本东北部的MW9.0级逆冲型板间地震是日本有地震记录以来震级最大的一次地震.本研究基于NIED F-net矩张量解目录中的震源机制解,选取两个长轴相互垂直的矩形区域进行应力场2D反演,获取了日本海沟俯冲带地区应力... 于2011年3月11日发生在日本东北部的MW9.0级逆冲型板间地震是日本有地震记录以来震级最大的一次地震.本研究基于NIED F-net矩张量解目录中的震源机制解,选取两个长轴相互垂直的矩形区域进行应力场2D反演,获取了日本海沟俯冲带地区应力场的空间及时间分布图像.结果表明:主震前,俯冲带地区应力状态在空间上大体趋于一致,即应力轴(P轴、σ1轴及SHmax轴)系统性地倾向板块汇聚方向,P轴、σ1轴倾角整体偏缓(<30°),且远离震源区及日本海沟东侧区域内的应力轴倾角普遍大于主震震源区内应力轴倾角;主震前,受2003年5月26日在宫城县北部发生的MW7.0地震影响,位于MW9.0地震震源区西北侧的应力场出现明显扰动,σ1轴倾向顺时针偏转150°~180°,并于之后大体恢复至震前状态,同期其他地区没有明显变化,这种情况可能和主震断层局部(深部)的前兆性滑动有关;主震后,距离震源区较远处应力场变化不大,主震震源区内应力场发生显著改变,P轴及σ1轴均以大角度(>60°)倾伏于板块汇聚方向,SHmax轴顺时针偏转60°~90°且在日本海沟附近普遍平行于海沟轴.这项研究以时空图像的方式展示了大地震前应力场变化的特点,反映了大地震孕震过程中构造与地震的相互作用,对于理解大地震孕震过程有重要意义. 展开更多
关键词 东日本mw9.0地震 日本海沟 俯冲带 震源机制解 应力反演
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基于粘弹性球体地球模型的震后位移与重力变化计算软件 被引量:5
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作者 付广裕 刘泰 《大地测量与地球动力学》 CSCD 北大核心 2017年第7期661-667,共7页
在考虑地球曲率、成层结构、可压缩性与自重的前提下,Tanaka等[1-2]提出一套较为完备的粘弹性球体位错理论,可计算全球任意位置由地震产生的同震与震后形变(含位移、重力变化、大地水准面变化)。Gao等[3]给出了与上述理论相匹配、界面... 在考虑地球曲率、成层结构、可压缩性与自重的前提下,Tanaka等[1-2]提出一套较为完备的粘弹性球体位错理论,可计算全球任意位置由地震产生的同震与震后形变(含位移、重力变化、大地水准面变化)。Gao等[3]给出了与上述理论相匹配、界面友好的计算软件,能计算30个震后时间点对应的震后形变。本研究针对Gao等的软件进行改进,可计算震后任意时间点对应的震后形变。新软件由3个部分组成:1)与32个震后时间点相对应的32套离散格林函数数值框架;2)格林函数插值计算程序,可针对上述32套格林函数数值框架进行插值运算,输出任意震后时间点对应的格林函数数值结果;3)积分计算程序,调用上述格林函数数值结果,计算任意类型地震在地表任意位置产生的同震与震后形变。一般情况下,使用者只需按要求准备辅助文件,提供发震断层模型和观测站位置信息,以及震中周围地区地幔粘滞性因子,先后运行格林函数插值计算程序和积分计算程序,即可计算出目标地震在地表任意位置产生的同震与震后形变。本文基于粘弹球体位错理论与弹性球体位错理论,分别计算2011年日本MW9.0地震引起的远场同震位移,2套结果的高度一致性证明了新程序的正确性。最后,介绍需要注意的若干事项,便于使用者掌握该软件。 展开更多
关键词 粘弹性球体位错理论 震后形变 位错格林函数 地幔粘滞性 2011年日本mw9.0地震
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震后GPS坐标时序中对数弛豫时间的估计
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作者 李萌 严丽 +1 位作者 肖根如 陈志高 《武汉大学学报(信息科学版)》 EI CAS CSCD 北大核心 2022年第11期1832-1839,共8页
全球定位系统(global positioning system,GPS)坐标时序去除同震形变和震前稳态速度场后,采用加权非线性最小二乘估计震后对数弛豫时间,可更准确地提取震后对数弛豫项,从而可以分析震后弛豫项对测站位移的独立物理贡献,并为震后余滑和... 全球定位系统(global positioning system,GPS)坐标时序去除同震形变和震前稳态速度场后,采用加权非线性最小二乘估计震后对数弛豫时间,可更准确地提取震后对数弛豫项,从而可以分析震后弛豫项对测站位移的独立物理贡献,并为震后余滑和黏滞性松弛效应等现象的分析提供参考。以日本2009—2019年GPS坐标时序为例,估计2011年Mw 9.0地震震后对数弛豫时间,发现不同站点的对数弛豫时间与其震中距关系显著,且服从高斯分布。据此,构建高斯函数加常数模型,可由震中距概略估计震后对数弛豫时间。高斯分布曲线的峰值、峰值位置、半宽度信息、最低位置分别为3.5 a、0 km、262 km、0.5 a,由此得出震后对数弛豫项影响时间大于0.5 a的站点主要集中在震中距约524 km范围内。震后弛豫效应区域分布的差异性显著,对数弛豫时间越长的区域,弛豫项水平位移表征越大,其中存在两个平均弛豫时间2.5 a的中心区域,与震后余滑的中心区域及时间相吻合。 展开更多
关键词 GPS坐标时序 对数弛豫时间 2011年日本mw 9.0地震 震中距 高斯分布
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