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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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Coseismic gravity and displacement changes of Japan Tohoku earthquake(Mw 9.0) 被引量:2
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作者 Xinlin Zhang Shuhei Okubo +1 位作者 Yoshiyuki Tanaka Hui Li 《Geodesy and Geodynamics》 2016年第2期95-100,共6页
The greatest earthquake in the modern history of Japan and probably the fourth greatest in the last 100 years in the world occurred on March 11, 2011 off the Pacific coast of Tohoku.Large tsunami and ground motions ca... The greatest earthquake in the modern history of Japan and probably the fourth greatest in the last 100 years in the world occurred on March 11, 2011 off the Pacific coast of Tohoku.Large tsunami and ground motions caused severe damage in wide areas, particularly many towns along the Pacific coast. So far, gravity change caused by such a great earthquake has been reported for the 1964 Alaska and the 2010 Maule events. However, the spatial-temporal resolution of the gravity data for these cases is insufficient to depict a co-seismic gravity field variation in a spatial scale of a plate subduction zone. Here, we report an unequivocal co-seismic gravity change over the Japanese Island, obtained from a hybrid gravity observation(combined absolute and relative gravity measurements). The time interval of the observation before and after the earthquake is within 1 year at almost all the observed sites, including 13 absolute and 16 relative measurement sites, which deduced tectonic and environmental contributions to the gravity change. The observed gravity agrees well with the result calculated by a dislocation theory based on a self-gravitating and layered spherical earth model. In this computation, a co-seismic slip distribution is determined by an inversion of Global Positioning System(GPS) data. Of particular interest is that the observed gravity change in some area is negative where a remarkable subsidence is observed by GPS, which can not be explained by simple vertical movement of the crust. This indicated that the mass redistribution in the underground affects the gravity change. This result supports the result that Gravity Recovery and Climate Experiment(GRACE) satellites detected a crustal dilatation due to the 2004 Sumatra earthquake by the terrestrial observation with a higher spatial and temporal resolution. 展开更多
关键词 tohoku earthquake(Mw 9.0) Co-seismic gravity change Co-seismic displacement change Coseismic geoid change Dislocation theory Global Positioning System Absolute gravity measurement Relative gravity measurement
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Co-seismic displacements of 2011 Japan Mw9.0 earthquake recorded by far-field GPS stations 被引量:7
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作者 Yang Shaomin Nie Zhaosheng Jia Zhige Chen Huijie Peng Maolei 《Geodesy and Geodynamics》 2011年第3期12-15,共4页
Co-seismic displacements of the 2011 Mw9.0 Japan earthquake recorded by GPS stations in China and surrounding areas showed a movement toward the epicenter. The horizontal displacements were up to 1 - 3 cm in northeast... Co-seismic displacements of the 2011 Mw9.0 Japan earthquake recorded by GPS stations in China and surrounding areas showed a movement toward the epicenter. The horizontal displacements were up to 1 - 3 cm in northeastern China, 3 -8 mm in the North China, and 2 cm in the Korean peninsula. The vertical movements in China were small uplifts. 展开更多
关键词 co-seismic deformation Mw9.0 tohoku earthquake Tanlu fault belts GPS
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Co-seismic deformation of 2011 Mw9.0 Japan earthquake observed by InSAR technique 被引量:2
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作者 Shen Qiang Tan Kai 《Geodesy and Geodynamics》 2011年第3期24-30,共7页
Co-seismic line-of-sight displacements of the 2011 Mw9.0 Japan earthquake derived from InSAR data of Envisat ASAR, ALOS PALSAR and TerraSAR-X show a maximum value of about - 245cm to -221cm near the epicenter. This re... Co-seismic line-of-sight displacements of the 2011 Mw9.0 Japan earthquake derived from InSAR data of Envisat ASAR, ALOS PALSAR and TerraSAR-X show a maximum value of about - 245cm to -221cm near the epicenter. This result is in good agreement with the result of GPS measurement. The ob- served displacement pattern suggests an earthquake-rupture zone over 500km long, with a ground-motion pat- tern in the vicinity of the northern segment more complex than that of the southern segment, possibly due to immediate aftershocks that occurred between satellite passes. 展开更多
关键词 Mw9.0 tohoku earthquake INSAR surface displacement
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从同震和震后形变分析日本东北M_W 9.0级大地震对近场地震活动性的影响 被引量:11
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作者 孙玉军 董树文 +3 位作者 范桃园 张斯奇 张怀 石耀霖 《地球物理学进展》 CSCD 北大核心 2013年第3期1131-1139,共9页
2011年日本东北大地震后,不断有报道认为日本南海海槽可能会发生强震,日本东北大地震对南海海槽断层活动有何影响?本文采用粘弹性半无限空间模型,利用反演得到的日本东北大地震的断层模型,计算了岛内部分断层的同震和震后形变以及库仑... 2011年日本东北大地震后,不断有报道认为日本南海海槽可能会发生强震,日本东北大地震对南海海槽断层活动有何影响?本文采用粘弹性半无限空间模型,利用反演得到的日本东北大地震的断层模型,计算了岛内部分断层的同震和震后形变以及库仑应力变化.结果表明:2011年日本东北大地震,使得平行于日本海沟的岛内逆冲断层应力释放明显,5km深度,库仑应力降低值都在50kPa以上,按照该地区每年应力积累1~10kPa计算,相当于释放了5~50年的应力积累;平行于南海海槽的岛内逆冲断层,同震库仑应力增加了1kPa左右,相当于0.1~1年的正常构造运动应力积累;对于岛内的走滑断层,若其滑动方向与同震或震后形变方向一致,则库仑应力增加,反之则降低,如1948年福井地震发震断层库仑应力增加10kPa左右,相当于1~10年的正常构造运动应力积累,地震危险性明显增加.同时,分析了不同软流圈粘滞性对震后形变和库仑应力的影响,发现对于不同的软流圈粘滞性系数,震后的形变和库仑应力相比同震都会有所增加.因此,对于平行南海海槽的岛内逆冲断层和岛内部分滑动方向与同震形变一致的走滑断层,震后地震危险性相比同震会进一步增强. 展开更多
关键词 日本东北大地震 震后形变 库仑应力 地震活动性
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利用粘弹性球体位错理论研究2011年日本M_W9.0地震引起的震后位移时空变化 被引量:3
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作者 刘泰 付广裕 苏小宁 《地震》 CSCD 北大核心 2017年第3期1-11,共11页
基于2011年3月~2015年9月的GPS观测数据,研究了2011年日本M_W9.0地震引起的震后位移时空变化,分析震后4.5a内震后断层余滑和粘滞性松弛对震后位移场的贡献。基于子断层叠加的思想,对Tanaka的粘弹性球体位错理论配套计算程序(环型解部分... 基于2011年3月~2015年9月的GPS观测数据,研究了2011年日本M_W9.0地震引起的震后位移时空变化,分析震后4.5a内震后断层余滑和粘滞性松弛对震后位移场的贡献。基于子断层叠加的思想,对Tanaka的粘弹性球体位错理论配套计算程序(环型解部分)加以改进,克服其近场计算精度不足(甚至错误)的缺陷,提高了近场震后位移的计算精度。利用弹性球体位错理论配套计算程序和改进后的粘弹性球体位错理论配套计算程序,分别计算2011年日本M_W9.0地震产生的同震位移,两组结果的差异仅占信号的1%左右,验证了对粘弹性球体位错理论配套计算程序改造的正确性。最后,结合震后3~4.5aGPS观测数据,利用Tanaka的粘弹性球体位错理论确定了2011年日本M_W9.0地震震中周边区域地幔粘滞性系数,其最佳拟合值为6×10^(18)Pa·s。 展开更多
关键词 球体位错理论 GPS 位移 地幔粘滞性系数 2011年日本Mw 9.0地震
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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:6
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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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利用GPS和InSAR数据反演2011年日本东北M_W9.0地震断层的同震滑动分布 被引量:4
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作者 王永哲 《地震学报》 CSCD 北大核心 2015年第5期796-805,885,共10页
本文首先对Envisat/ASAR数据进行干涉处理,获取2011年日本东北MW9.0地震的地表InSAR同震形变场;然后通过对InSAR同震形变数据重采样方法的深入分析,选择条纹率法结合干涉图的空间相干性对InSAR同震形变数据进行重采样;最后基于弹性半空... 本文首先对Envisat/ASAR数据进行干涉处理,获取2011年日本东北MW9.0地震的地表InSAR同震形变场;然后通过对InSAR同震形变数据重采样方法的深入分析,选择条纹率法结合干涉图的空间相干性对InSAR同震形变数据进行重采样;最后基于弹性半空间位错模型,联合InSAR与GPS形变数据,采用最小二乘法反演发震断层的滑动分布.研究结果表明:考虑相干性的条纹率重采样方法,更适用于形变场中存在除断层外的有限边界、且形变场范围较大的InSAR数据重采样处理;断层滑动主要发生在地表以下50km范围内,最大滑动量为49.9m,矩张量为4.89×1022 N·m,所对应的矩震级为MW9.1,与地震学反演的结果比较吻合. 展开更多
关键词 日本东北MW9.0地震 合成孔径雷达干涉测量 数据重采样 同震滑动分布
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2011年日本东北Mw 9.0级地震的岩石圈三维建模分析
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作者 闫兵 贾东 +1 位作者 李一泉 王毛毛 《高校地质学报》 CAS CSCD 北大核心 2012年第4期676-685,共10页
2011年3月11日日本东北地区太平洋海域发生Mw 9.0级地震。日本海沟板块俯冲速率高,地震活动性强,因此研究程度高,到目前为止已获得了覆盖日本海沟弧前区域的地震波剖面数据。本文利用8条岩石圈结构剖面建立了日本海沟的三维岩石圈结构... 2011年3月11日日本东北地区太平洋海域发生Mw 9.0级地震。日本海沟板块俯冲速率高,地震活动性强,因此研究程度高,到目前为止已获得了覆盖日本海沟弧前区域的地震波剖面数据。本文利用8条岩石圈结构剖面建立了日本海沟的三维岩石圈结构模型。日本海沟岛弧地壳由上到下包含5层:古近系—新近系—第四系海相沉积岩、白垩系海相沉积岩、岛弧上地壳俯冲杂岩、岛弧下地壳和地幔楔;日本海沟北部还存在中地壳;洋壳是一个双层构造,上层为熔岩和席状岩墙群,下层为堆晶辉长岩;陆壳和洋壳之间存在一个低速的板间层。本文在三维模型基础上讨论了俯冲板块的弯曲点和弯曲轴等几何学特征,分析了日本海沟俯冲带的历史地震和日本东北Mw 9.0级地震主震和余震的震源分布,日本东北地区的地震活动与太平洋板块向日本岛弧下方的俯冲活动关系密切。 展开更多
关键词 日本东北Mw9 0级地震 日本海沟 三维建模 俯冲型大地震 弯曲点 弯曲轴
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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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Comparative analysis of the characteristics of global seismic wave propagation excited by the M_w 9.0 Tohoku earthquake using numerical simulation 被引量:4
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作者 YAN ZhenZhen ZHANG Huai +1 位作者 FAN XiangTao DU XiaoPing 《Science China Earth Sciences》 SCIE EI CAS 2014年第7期1626-1636,共11页
Giant earthquakes generate rich signals that can be used to explore the characteristics of the hierarchical structure of the Earth’s interior associated with the eigenfrequencies of the Earth.We employ the spectral e... Giant earthquakes generate rich signals that can be used to explore the characteristics of the hierarchical structure of the Earth’s interior associated with the eigenfrequencies of the Earth.We employ the spectral element method,incorporated with large-scale parallel computing technology,to investigate the characteristics of global seismic wave propagation excited by the2011 Mw9.0 Tohoku earthquake.The transversely isotropic PREM model is employed as a prototype of our numerical global Earth model.Topographic data and the effect of the oceans are taken into consideration.Wave propagation processes are simulated by solving three-dimensional elastic wave governing equations with the seismic moment tensor obtained from the Global Centroid Moment Tensor Catalog.Three-dimensional visualization of our computing results displays the nature of the global seismic wave propagation.Comparative analysis of our calculations with observations obtained from the Incorporated Research Institutions for Seismology demonstrates the reliability and feasibility of our numerical results.We compare synthetic seismograms with incorporated and unincorporated ocean models.First results show that the oceans have obvious effects on the characteristics of seismic wave propagation.The peak displacement and peak velocity of P waves become relatively small under the effect of the ocean.However,the effect of the ocean on S-waves is complex.The displacement and velocity of S waves decrease rapidly over time using an unincorporated ocean model.Therefore,the effects of the ocean should be incorporated when undertaking quantitative earthquake hazard assessments on coastal areas.In addition,we undertake comparative analysis on the characteristics of the Earth’s oscillation excited by the 2004 Sumatra-Andaman,2008 Wenchuan,and 2011Tohoku earthquakes that incorporate the effect of the Earth’s gravitational potential.A comparison of the amplitude spectra of the numerical records indicates that energy released by the three big earthquakes is different.Our comparative analysis realizes that the computing results can accurately reproduce some eigenfrequencies of the Earth,such as toroidal modes 0T2 to 0T13and spheroidal modes 0S7 to 0S31.These results demonstrate that numerical simulations can be successfully used to investigate the Earth’s oscillations.We propose that numerical simulations can be used as one of the major tools to further reveal how the Earth’s lateral heterogeneities affect the Earth’s oscillations. 展开更多
关键词 Mw9.0 tohoku earthquake Sea of Japan numerical simulation global seismic wave propagation Earth's oscillations
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Static slip model of the M_w 9.0 Tohoku (Japan) earthquake:Results from joint inversion of terrestrial GPS data and seafloor GPS/acoustic data 被引量:8
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作者 DIAO FaQi XIONG Xiong ZHENG Yong 《Chinese Science Bulletin》 SCIE CAS 2012年第16期1990-1997,共8页
Based on co-seismic displacements recorded by terrestrial GPS stations and seafloor GPS/acoustic stations, the static slip model of the 2011 Mw 9.0 Tohoku earthquake was determined by inverting the data using a layere... Based on co-seismic displacements recorded by terrestrial GPS stations and seafloor GPS/acoustic stations, the static slip model of the 2011 Mw 9.0 Tohoku earthquake was determined by inverting the data using a layered earth model. According to a priori information, the rupture surface was modeled with a geometry that is close to the actual rupture, in which the fault dip angle increases with depth and the fault strike varies with the trend of the trench. As shown by the results inferred from the joint inversion, the "geodetic" moment is 3.68 × 10 22 Nm, corresponding to Mw 9.01, and the maximum slip is positioned at a depth of 13.5 km with a slip magnitude of 45.8 m. Rupture asperities with slip exceeding 10 m are mainly distributed from 39.6 to 36.97°N, over a length of almost 240 km along the trench. The slip was mostly concentrated at depths shallower than 40 km, up-dip of the hypocenter. "Checkerboard" tests reveal that a joint inversion of multiple datasets can resolve the slip distribution better than an inversion with terrestrial GPS data only-especially when aiming to resolve slip at shallow depths. Thus, the joint inversion results obtained by this work may provide a more reliable slip model than the results of other studies that are only derived from terrestrial GPS data or seismic waveform data. 展开更多
关键词 GPS数据 联合反演 滑移模型 地震位移 地面 海底 静态 东北
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震后GPS坐标时序中对数弛豫时间的估计 被引量:1
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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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