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Fracture characteristics of the 1997 Jiashi,Xinjiang, China, earthquake swarm inferred from source spectra 被引量:8
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作者 周仕勇 许忠淮 《Acta Seismologica Sinica(English Edition)》 CSCD 2000年第2期125-135,共11页
Broadband P and S waves source spectra of 12 M_s≥5.0 earthquakes of the 1997 Jiashi, Xinjiang, China. earthquake swarm recorded at 13 GDSN stations have been analyzed. Rupture size and static stress drop of these ear... Broadband P and S waves source spectra of 12 M_s≥5.0 earthquakes of the 1997 Jiashi, Xinjiang, China. earthquake swarm recorded at 13 GDSN stations have been analyzed. Rupture size and static stress drop of these earthquakes have been estimated through measuring the corner frequency of the source spectra. Direction of rupture propaga- tion of the earthquake faulting has also been inferred from the azimuthal variation of the comer frequency. The main results are as follows: ① The rupture size of M_s≥6.0 strong earthquakes is in the range of 10~20 km, while that of Ms_=5.0~5.5 earthquakes is 6~10 km. ② The static stress drop of the swarm earthquakes is rather low, being of the order of 0.1 MPa. This implies that the deformation release rate in the source region may be low. ③ Stress drop of the earthquakes appears to be proportional to their seismic moment, and also to be dependent on their focal mechanism. The stress drop of normal faulting earthquakes is usually lower than that of strike-slip type earth quakes. ④ For each M_s≥6.0 earthquake there exists an apparent azimuthal variation of the comer frequencies. Azimuthally variation pattern of comer frequencies of different earthquakes shows that the source rupture pattern of the Jiashi earthquake swarm is complex and no uniform rupture expanding direction exists. 展开更多
关键词 jiashi earthquake swarm corner frequency stress drop rupture direction
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Analysis on the master event method and precise location of 1997 Jiashi strong earthquake swarm in western China 被引量:9
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作者 周仕勇 许忠淮 +2 位作者 韩京 许洪新 努尔尼沙 《Acta Seismologica Sinica(English Edition)》 EI CSCD 1999年第3期285-291,共7页
Master event location method was described in detail in this paper. Some problems in the application of master event method have been analyzed and some improvements of the method have been made. As compared the locat... Master event location method was described in detail in this paper. Some problems in the application of master event method have been analyzed and some improvements of the method have been made. As compared the location results of MS>=3.0 earthquakes of Jiashi swarm obtained by using this method with that by the traditional absolute method, the result obtained by using the master event method shows more reasonable and more consistent with that from the focal mechanism solutions. After relocation, we can see, the epicenters of M>=5.0 earthquakes show an echelon-type alignment along NNW-SSE direction, and all earthquakes concentrate nearly in a volume region about 30 km (N-S) × 15 km (E-W) × 15 km (U-D). Earthquake focal depths are mainly in the range of 15-28 km. 展开更多
关键词 jiashi strong earthquake swarm master event location
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Tomographic determination of the upper crustal structure in the Jiashi strong earthquake swarm region 被引量:1
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作者 杨卓欣 赵金仁 +5 位作者 张先康 张成科 成双喜 段玉玲 张建狮 王帅军 《Acta Seismologica Sinica(English Edition)》 CSCD 2002年第2期162-170,共9页
A three-dimensional temporary seismic transmission array was arranged in a 50x60 km2 region around Jiashi strong earthquake swarm to receive seismic waves generated by 8 fires from different azimuths. With the inversi... A three-dimensional temporary seismic transmission array was arranged in a 50x60 km2 region around Jiashi strong earthquake swarm to receive seismic waves generated by 8 fires from different azimuths. With the inversion method without model blocks and using P and S reflections from Moho at critical distances, the 3-D images of P, S velocity perturbation and ratio vP/vS perturbation of the upper crust under the seismic array were reconstructed. Meanwhile, the seismicity of the Jiashi earthquake swarm was taken into consideration in the analysis of the seismogenesis. The results indicate that the upper crustal structure under the Jiashi strong earthquake swarm region is characterized by significant inhomogeneity both laterally and vertically. From 12 km depth, it is clear that there is an NNW-oriented high P-wave velocity anomalous body corresponding to the epicenter of the swarm with low-velocity anomaly around it, which is the direct cause of the strong earthquakes. High vP/vS is distributed in the same location, which may indicate the decline of shear strength of the source region owing to relative softness of the medium, this can be accounted as an explanation for the seismicity feature of the Jiashi strong earthquake swarm. 展开更多
关键词 jiashi strong earthquake swarm 3-D seismic transmission 3-D images of velocity perturbation the upper crust crustal inhomogeneity
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Research on the Application of Time Structure Variation Analysis to the Jiashi-Bachu Earthquake Swarm Sequence 被引量:2
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作者 Yang Xin Long Haiying +1 位作者 Shangguan Wenming Nie Xiaohong 《Earthquake Research in China》 2008年第3期251-264,共14页
In 1997 - 2003, 27 earthquakes with M≥ 5.0 occurred in the Jiashi-Bachu area of Xinjiang. It was a rare strong earthquake swarm activity. The earthquake swarm has three time segments of activity with different magnit... In 1997 - 2003, 27 earthquakes with M≥ 5.0 occurred in the Jiashi-Bachu area of Xinjiang. It was a rare strong earthquake swarm activity. The earthquake swarm has three time segments of activity with different magnitudes in the years 1997, 1998 and 2003. In different time segments, the seismic activity showed strengthenin-qguiet changes in various degrees before earthquakes with M ≥ 5.0. In order to delimitate effectively the precursory meaning of the clustering (strengthening) quiet change in sequence and to seek the time criterion for impending prediction, the nonlinear characteristics of seismic activity have been used to analyze the time structure characteristics of the earthquake swarm sequence, and further to forecast the development tendency of earthquake sequences in the future. Using the sequence catalogue recorded by the Kashi Station, and taking the earthquakes with Ms≥ 5.0 in the sequence as the starting point and the next earthquake with Ms = 5.0 as the end, statistical analysis has been performed on the time structure relations of the earthquake sequence in different stages. The main results are as follows: (1) Before the major earthquakes with M ≥ 5.0 in the swarm sequence, the time variation coefficient (δ-value) has abnormal demonstrations to different degrees. (2) Within 10 days after δ= 1, occurrence of earthquakes with M ≥ 5.0 in the swarm is very possible. (3) The time variation coefficient has three types of change. (4) The change process before earthquakes with M5.0 is similar to that before earthquakes with M6.0, with little difference in the threshold value. In the earthquake swarm sequence, it is difficult to delimitate accurately the attribute of the current sequences (foreshock or aftershock sequence) and to judge the magnitude of the follow-up earthquake by δ-value. We can only make the judgment that earthquakes with M5.0 are likely to occur in the sequence. (5) The critical clustering characteristics of the sequence are hierarchical. Only corresponding to a certain magnitude can the sequence have the variation state of critical clustering. (6) The coefficient of the time variation has a clear meaning in physics. After the clustering-quiet state of earthquake activity has appeared, it can describe clearly the randomness of the seismogenic system. Furthermore, it can efficiently clarify whether or not the clustering quiescence variation is of some prognostic meaning. In the case that the earthquake frequency attenuation is essentially normal (h 〉 1 ) and there is no remarkable clustering-quiescence state, it is still possible to discover the abnormal change of the sequence from the time variation coefficient. On the contrary, in the later period of swarm activity, after the appearance of many seismic quiescence phenomena, this coefficient did not appear abnormally, even when h 〈 1, suggesting that the δ-value diagnosis is more universal. 展开更多
关键词 Time variation coefficient Earthquake clustering RANDOMNESS Time structure ofearthquake sequence jiashi earthquake swarm
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Fine upper crustal structure of Jiashi strong earthquake swarm region in Xinjiang in-ferred from high resolution seismic refraction profile data
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作者 徐朝繁 张先康 +3 位作者 段永红 杨卓欣 鄷少英 胡修奇 《Acta Seismologica Sinica(English Edition)》 EI CSCD 2006年第1期62-71,共10页
The data obtained from a high resolution seismic refraction profile, which was carded out in Jiashi, Xinjiang, strong earthquake swarm area, were processed with both finite difference inversion and Hagedoorn refractor... The data obtained from a high resolution seismic refraction profile, which was carded out in Jiashi, Xinjiang, strong earthquake swarm area, were processed with both finite difference inversion and Hagedoorn refractor wavefront imaging technique and the fine upper crustal structure was determined. The results show that the upper crustal structure is relatively well-distributed in laterally and obviously by layers vertically.From surface to 11.0 km depth, there are about four layers. The P wave velocity of top two layers range from 1.65 to 4.5 km/s and their bottom boundaries, the buried depths of which are 0.4, 2.96-3.0 km respectively, are almost horizontal; The third layer is comparatively complicated and its P wave velocity presents inhomogeneous in both laterally and vertically. The bottom boundary of third layer is crystalline basement and shows a little uplift, which seemly suggest that the upper crust had been resisted while the hard Tarim block inserting into Tianshan Mountain; The forth layer is relatively even and its P wave velocity is about 6.3 km/s. There are a lateral velocity variation at the depth of about 4.0 km, and suggest that it has something to do with the hidden Meigaiti fault and Meigaiti-Xiasuhong fault but there are no the structure features about these faults stretching to the surface and passing through the crystalline basement. The seismogenic tectonic of Jiashi strong earthquake swarm at least lies in middle or lower crust beneath 11.0 km depth. 展开更多
关键词 jiashi strong earthquake swarm region high resolution refraction finite different inversion Hagedoorn principle refractor wavefront imaging
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Basement interface structural characteristics beneath Jiashi strong earthquake swarm area in Xinjiang, China
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作者 徐朝繁 段永红 +3 位作者 田晓峰 潘纪顺 张建狮 胡修奇 《Acta Seismologica Sinica(English Edition)》 CSCD 2007年第5期507-512,共6页
The seismic data obtained from high resolution seismic refraction profile in Jiashi strong earthquake swarm area in Xinjiang, China were further processed with ray hit analysis method and more complete basement interf... The seismic data obtained from high resolution seismic refraction profile in Jiashi strong earthquake swarm area in Xinjiang, China were further processed with ray hit analysis method and more complete basement interface structural characteristics beneath Jiashi strong earthquake swarm area were determined. The results show that there are two clear basement interfaces at the upper crust in Jiashi strong earthquake swarm area. The first one with buried depth ranging from 2.6 km to 3.3 km presents integral and continuous structure, and it appears an inclined plane interface and smoothly rises up toward Tianshan Mountain. The second basement interface with buried depth from 8.5 km to 11.8 km, is the antiquated crystalline basement of Tarim basin. Near the post number of 37 km, the buried depth of the crystalline basement changed abruptly by 2.5 km, which maybe result from an ultra crystalline basement fault. If taking this fault as a boundary, the crystalline basement could be divided into two parts, i.e. the southwestern segment with buried depth about 11.5 km, and the northeastern segment with buried depth approxi-mately from 8.5 km to 9.0 km. That is to say, in each segment, the buried depth changes not too much. The northeast segment rises up as a whole and upheaves slightly from southwest to northeast, which reflects the upper crustal deformation characteristics under the special tectonic background at the northwestern edge of Tarim basin. 展开更多
关键词 jiashi strong earthquake swarm area high resolution refraction survey ray hit analysis method basement interface structure ultra crystalline basement fault
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A priliminary study on the sequence characteristics and focal mechanism solution of the Jiashi strong earthquake swarm 被引量:2
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作者 XIN YANG GUO YING GAO Seismological Bureau of Xinjiang Uygur Autonomous Region, rümqi 830011, China 《Acta Seismologica Sinica(English Edition)》 CSCD 1998年第6期16-23,共8页
The sequence characteristics and focal mechanism solution of the Jiashi, Xinjiang strong earthquake swarm are analyzed and studied in this paper. The result shows that before the M S=6.6 earthquake, value h o... The sequence characteristics and focal mechanism solution of the Jiashi, Xinjiang strong earthquake swarm are analyzed and studied in this paper. The result shows that before the M S=6.6 earthquake, value h of sequence frequency attenuation coefficient was less than 1, then value h was more than 1. Before occurrence of M S6.0 earthquakes the energy is released either in a continuously strengthened way or a sharply strengthened way, and before M S5.0 earthquakes the sequence frequency shows calm. The study on the focal mechanism solution of the strong earthquake swarm shows that the source faults are mainly in a right lateral, strike slip way and the faults have characteristics of tensor shear. 展开更多
关键词 earthquake swarm sequence characteristics focal mechanism SOLUTION focal displacement feature jiashi
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Study on Stress Triggering During the Activity Process of the Jiashi Strong Earthquake Swarm
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作者 Wang Qiong Wang Haitao 《Earthquake Research in China》 2007年第3期255-268,共14页
The Bachu-Jiashi earthquake of MS6.8 occurred on February 24,2003,about 20km from the southeast of the 1997~1998 Jiashi seismic region in Xinjiang,and its aftershocks are rich and strong.Did the 1997~1998 Jiashi str... The Bachu-Jiashi earthquake of MS6.8 occurred on February 24,2003,about 20km from the southeast of the 1997~1998 Jiashi seismic region in Xinjiang,and its aftershocks are rich and strong.Did the 1997~1998 Jiashi strong earthquake swarm trigger the Bachu-Jiashi MS6.8 earthquake? The Atushi earthquake of MS6.7 occurred in 1996,and the 1997~1998 Jiashi strong earthquake swarm occurred about 70km from the Atushi earthquake 10 months later.Did the Atushi earthquake of M-S6.7 encourage the 1997~1998 Jiashi strong earthquake swarm? There were 9 earthquakes with M-S6.0 from 1996 to 1997 in the Jiashi seismic region,how did they act on each other? To answer the above questions,the article studies the triggering effect of the activity process of the whole Jiashi earthquake swarm from the 1996 Atushi earthquake of M-S6.7,the 1997~1998 Jiashi strong swarm to the 2003 Bachu-Jiashi earthquake of M-S6.8,and analyzes the seismicity characteristics around the Jiashi region.The results show that the 1996 Atushi earthquake of M-S6.7 encouraged the 1997~1998 Jiashi strong swarm to some extent,the accumulative Coulomb stress change from the previous M-6.0 earthquakes of the Jiashi strong swarm had certain triggering effects on the following M-6.0 events,and the Coulomb stress change converted from the Jiashi strong swarm strongly encouraged the 2003 Bachu-Jiashi earthquake with M-S6.8. 展开更多
关键词 jiashi strong earthquake swarm Static Coulomb failure rupture stress change Stress triggering
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伽师地震区地壳细结构及发震断层的初步研究 被引量:33
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作者 李松林 张先康 +3 位作者 W.D.Mooney 赖晓玲 A.J.Michael 段永红 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2002年第1期76-82,T001,T002,共9页
1997年至 1 998年伽师地区共出现 9次震级为 6 .1— 6 .8级的强震 .在一个非常短的时间间隔内和非常小的地区范围内接连出现这么多次震级非常接近的地震 ,确实非常罕见 .为研究伽师强震区的深部构造背景和孕震机制 ,本文对伽师地震区的... 1997年至 1 998年伽师地区共出现 9次震级为 6 .1— 6 .8级的强震 .在一个非常短的时间间隔内和非常小的地区范围内接连出现这么多次震级非常接近的地震 ,确实非常罕见 .为研究伽师强震区的深部构造背景和孕震机制 ,本文对伽师地震区的余震观测资料进行了分析处理 .利用联合反演技术同时得到了地震震源位置和地震区地壳三维速度结构 .余震震中沿一北北东向条带分布 ,与强震分布的两个条带中的北东向条带位置基本重合 .三维反演得到的速度结构结果表明 ,在地下 1 2km以下存在一条北北东向和一条北北西向的低速条带 .上述两低速条带与强震分布的两个条带位置很接近 .初步推测 ,低速条带对应了地壳深部的两条断裂 .在我们观测期间 ,北北东向断裂有微震活动 ,北北西向断裂相对平静 . 展开更多
关键词 伽师地震群 速度结构 断层成像 联合反演 地质构造 地壳
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伽师强震群震源破裂特征的初步分析 被引量:45
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作者 单新建 何玉梅 +3 位作者 朱燕 马宝柱 张桂芳 杨成荣 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2002年第3期416-425,共10页
为深入研究 1 997年新疆伽师地区连续发生的强震群的震源破裂特征 ,利用全球数字地震台网 (GDSN)宽频带数字资料及区域台网资料 ,较详细地研究了伽师强震群的震源机制及震源破裂特征 .结果表明 :伽师强震群的震源机制解主要有走滑和正... 为深入研究 1 997年新疆伽师地区连续发生的强震群的震源破裂特征 ,利用全球数字地震台网 (GDSN)宽频带数字资料及区域台网资料 ,较详细地研究了伽师强震群的震源机制及震源破裂特征 .结果表明 :伽师强震群的震源机制解主要有走滑和正倾两种破裂类型 ,其共同特点是主压应力轴方向沿北北东向 ,主张应力轴沿北西向 ,与区域构造应力场方向存在差异 ,具有明显局部特征 ;从震源破裂特征来看 ,伽师强震的滑动尺度、上升时间和持续时间均较小 ,震源破裂面积不大 ,是由一点向四周快速扩散的脆性破裂 ,无明显伸展方向 ;伽师强震群的破裂断层面为北东向 ,与震源深度梯度变化带、地壳接触变形梯度变化带、等烈度线以及地震扩展方向吻合 ;伽师强震群是在近南北向挤压环境下 ,在震源区附近剪切和张扭应力作用下发生的多次沿北东向的脆性快速破裂 。 展开更多
关键词 伽师强震群 震源机制 震源破裂特征 张性破裂 左旋走滑
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新疆伽师强震群的震源破裂特征 被引量:18
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作者 单新建 何玉梅 +2 位作者 朱燕 马宝柱 杨成荣 《地震地质》 EI CSCD 北大核心 2002年第1期59-68,共10页
利用国内外短周期P波初动符号及全球数字地震台网 (GDSN)的宽频带数字记录资料 ,研究了 1997年 1月 2 3日至 1997年 11月 4日伽师强震群的震源机制解和伽师强震群中的 5个强震、后续地震及其周边地震的震源破裂过程。从震源机制解来看 ... 利用国内外短周期P波初动符号及全球数字地震台网 (GDSN)的宽频带数字记录资料 ,研究了 1997年 1月 2 3日至 1997年 11月 4日伽师强震群的震源机制解和伽师强震群中的 5个强震、后续地震及其周边地震的震源破裂过程。从震源机制解来看 ,伽师强震群主要有走滑和正倾两种破裂类型 ,主压应力轴方向主要为NNE向和近垂直 ,而主张应力轴为NW向并近水平 ,与区域构造应力场方向存在差异 ,具有明显的局部特征。从破裂过程看 ,伽师强震群的破裂过程相对简单 ,破裂面积不大 ,上升时间较短 ,是由一点向四周快速扩散的脆性破裂 ,无明显的伸展方向 ,与阿图什地震完全不同。研究结果表明 ,伽师强震群与震源附近的地壳结构在垂向和横向上的非均匀变化有着密切关系 ,而阿图什地震与塔里木盆地的现今构造运动关系密切。伽师强震群是在震源区附近地壳上部垂向和水平向力共同作用下发生的多次沿NNE向的快速脆性破裂 。 展开更多
关键词 伽师强震群 震源机制 破烈过程 构造运动 新疆
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伽师强震群区上地壳三维速度层析成像——人工爆破和天然地震的联合反演 被引量:13
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作者 潘素珍 张先康 +4 位作者 杨卓欣 张成科 赵金仁 王帅军 段玉玲 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2007年第5期1456-1463,共8页
伽师震区位于天山褶皱、帕米尔构造弧与塔里木块体三个构造单元的交接地带,近年来该区发生了一系列的强震活动.为进一步获得该震区详细的地壳速度结构,本文利用人工爆破和天然地震资料联合反演的方法,对1997年新疆伽师震区布设的三维人... 伽师震区位于天山褶皱、帕米尔构造弧与塔里木块体三个构造单元的交接地带,近年来该区发生了一系列的强震活动.为进一步获得该震区详细的地壳速度结构,本文利用人工爆破和天然地震资料联合反演的方法,对1997年新疆伽师震区布设的三维人工地震透射台阵和流动地震台网的资料进行处理,重建了台阵下方上地壳三维速度扰动图像,并结合地震活动分布,对伽师强震群的地震成因作出进一步分析.结果表明研究区上地壳速度结构在纵向和横向上具有明显的非均匀性,随着深度的逐渐加深,震区下方以萨如锡为中心的低速异常体逐步被高速异常体所替代.自12 km深度开始,在与强震群震中相应的位置上,明显出现沿北北西向的高P波速度异常体,在其周围为相对低速分布,呈现出低速条带环绕高速条带的分布格局,VP/VS在相同的位置上也表现为高值分布.这种结构上的差异可能与伽师强震群发生有密切关系.16 km深度的P波速度层析图表明,伽师强震群发生在地壳相对高速扰动区内或是高速扰动向低速扰动过渡的边缘,壳内高速体的存在为强震的孕育和发生提供了重要基础. 展开更多
关键词 伽师强震群 联合反演 速度异常体 速度扰动
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帕米尔东北侧地壳物性结构及其发震环境探讨 被引量:16
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作者 刘志 张先康 +3 位作者 周雪松 赵金仁 张成科 潘纪顺 《地震学报》 CSCD 北大核心 2003年第3期242-249,共8页
通过对帕米尔东北侧伽师及其周边地区两条深地震测深剖面S波资料的处理计算 ,结合P波研究结果 ,得到了S波二维地壳速度结构和波速比 (vP/vS)分布 .研究表明 :①塔里木块体平均地壳波速比明显高于西昆仑和天山褶皱带 ,显示了“坚硬”、... 通过对帕米尔东北侧伽师及其周边地区两条深地震测深剖面S波资料的处理计算 ,结合P波研究结果 ,得到了S波二维地壳速度结构和波速比 (vP/vS)分布 .研究表明 :①塔里木块体平均地壳波速比明显高于西昆仑和天山褶皱带 ,显示了“坚硬”、稳定地壳物性特征 .下地壳正常偏低的波速比 (泊松比 )值 ,说明塔里木块体的“下插”是该地区地壳运动的主要特征 ;②天山褶皱带上地壳岩层相对较“软” ,易于在应力作用下断裂破碎和应力能量释放 ,是其小震密集分布的重要构造因素 ;③伽师附近正处在下地壳C界面和壳幔边界的上隆顶部或拐点上 ,是强震群发生的深部构造背景 .上地壳中下部的块体边界附近波速比值的交错变化和接触面复杂形态的存在 ,形成了伽师强震群出现的特殊构造环境 .震源处波速比相对较高 ,剪切模量较小 ,可能是伽师强震群应力降偏低的主要原因 . 展开更多
关键词 S波二维地壳速度结构 波速比 地震测深剖面 发震环境 地壳运动 应力作用 伽师强震群
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伽师强震群区震源细结构的深地震反射探测研究 被引量:18
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作者 杨卓欣 张先康 +4 位作者 嘉世旭 刘保金 酆少英 赵成斌 潘纪顺 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2006年第6期1701-1708,共8页
穿过伽师强震群的深地震反射剖面提供了研究区从地表直至莫霍界面的地壳细结构图像.探测结果表明:研究区上、下地壳分界面埋深约20-30km,莫霍界面埋深约52~58km.上地壳内部存在着两种截然不同的反射图像.上地壳上部为沉积盖层,... 穿过伽师强震群的深地震反射剖面提供了研究区从地表直至莫霍界面的地壳细结构图像.探测结果表明:研究区上、下地壳分界面埋深约20-30km,莫霍界面埋深约52~58km.上地壳内部存在着两种截然不同的反射图像.上地壳上部为沉积盖层,厚度约8-9km,盖层内部反射成层分布,显示了稳定而连续的沉积特点;上地壳下部则为“反射透明”背景下存在的叠层状反射带.下地壳内部呈现明显的反射性质,具体体现在上、下地壳分界面和莫霍间断面都表现为具有一定持续时间的多循环反射叠层结构特征.时间剖面上所有反射事件由北东向南西下倾的整体图像直观地反映了塔里木盆地地壳变形而向西昆仑下插入的事实.剖面47km桩号附近,上地壳下部至壳幔过渡带以上地壳范围内存在一条高倾角的深断裂,具有走滑性质,本研究认为该深断裂与1997年伽师强震群的发生密切相关,推断它为伽师强震群的发震构造.而时间剖面上壳幔过渡带反射的连续性则说明该断裂没有向下穿过莫霍面.存在于上地壳上部的两条高倾角的浅部断层可能对应于地质推测的麦盖提一下苏洪断裂带,它们与位于其下方的地壳深断裂构成了伽师强震群可能的深、浅构造关系。 展开更多
关键词 伽师强震群 深地震反射 震源细结构
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1997年新疆伽师强震群发展过程中发震断层间相互作用的影响 被引量:21
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作者 周仕勇 姜明明 Russell Robinson 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2006年第4期1102-1109,共8页
1997年发生在新疆伽师的强震群迄今仍在持续活动,从1997年1月21日震群发生至1997年10月18日,共发生5级以上地震15次.震群发生前,该地区几乎没有地震活动.根据伽师震群地震的精确定位结果及震源机制解,我们设定该震群的发震构造是一组NNW... 1997年发生在新疆伽师的强震群迄今仍在持续活动,从1997年1月21日震群发生至1997年10月18日,共发生5级以上地震15次.震群发生前,该地区几乎没有地震活动.根据伽师震群地震的精确定位结果及震源机制解,我们设定该震群的发震构造是一组NNW(北北西)向的雁形右旋走滑断层和一组NE(北东)向雁形正倾滑断层.并以此作为模拟该区域理论地震活动的力学模型,开展震群区域理论地震活动的模拟研究.模拟结果证实了断层间的相互作用或应力传递能产生震群活动的猜测,并对伽师震群中为何部分地震的震源机制是正断层进行了合理解释.进一步推测伽师位于地壳厚度的陡变带也可能是引起该地区地震活动丛集发生的原因. 展开更多
关键词 伽师震群 断层相互作用 地震活动性模拟
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伽师强震群区上地壳三维速度层析成像 被引量:27
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作者 杨卓欣 赵金仁 +5 位作者 张先康 张成科 成双喜 段玉玲 张建狮 王帅军 《地震学报》 CSCD 北大核心 2002年第2期153-161,共9页
以伽师强震群为中心布设了一个 5 0km× 6 0km范围的三维人工地震透射临时台阵 ,接收来自不同方位的 8次爆破激发产生的地震波 ;利用所记录到的莫霍界面临界反射P波、S波走时 ,采用模型不分块反演技术 ,重建台阵下方上地壳三维P ,S... 以伽师强震群为中心布设了一个 5 0km× 6 0km范围的三维人工地震透射临时台阵 ,接收来自不同方位的 8次爆破激发产生的地震波 ;利用所记录到的莫霍界面临界反射P波、S波走时 ,采用模型不分块反演技术 ,重建台阵下方上地壳三维P ,S波速度扰动图象 ,以及vP/vS 扰动分布图象 ;并结合伽师震群的地震活动分布 ,对该震群的成因进行了分析 .结果表明 ,研究区上地壳存在明显的不均匀性 .自 12km深度开始 ,在与震群震中相应的位置上 ,明显出现沿北北西向的高P波速度块体 ,在它的周围为相对低速分布 ,这种结构上的差异是伽师强震群发生的最直接原因 ;vP/vS 在相同的位置上为高值分布 ,则表明由于介质相对软弱可能造成震源体抗剪强度下降 . 展开更多
关键词 伽师强震群 三维人工地震透射 上地壳三维速度扰动图象 地壳不均匀性 地震波 P波 S波
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新疆伽师强震群区上部地壳细结构的高分辨折射地震探测研究 被引量:20
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作者 徐朝繁 张先康 +3 位作者 段永红 杨卓欣 酆少英 胡修奇 《地震学报》 CSCD 北大核心 2006年第1期60-69,共10页
2004年4月在伽师强震群区完成了一条高分辨折射地震探测剖面.我们采用有限差分反演和哈格多恩原理折射波前成像方法进行了处理,得到了该地区上部地壳细结构图象.结果显示上部地壳结构总体上横向比较均匀,纵向分层明显.该地区地壳顶... 2004年4月在伽师强震群区完成了一条高分辨折射地震探测剖面.我们采用有限差分反演和哈格多恩原理折射波前成像方法进行了处理,得到了该地区上部地壳细结构图象.结果显示上部地壳结构总体上横向比较均匀,纵向分层明显.该地区地壳顶部11km以上可分为4层:顶部约400m以上为浅表盖层,P波速度约1.65~1.8km/s,该层为较松散的风化层;第二层为纵向强梯度层,P波速度在1.8~4.5km/s之间,纵向梯度约1.2km·s^-1/km,其厚度在2.96~3.0km之间,其底界面几乎水平;第三层的厚度有较大变化,其埋深从东北向西南逐渐变深,西南端层厚约6.5km,东北端减薄为5.5km.该层的上部和下部又表现为不同的速度结构特征,其上部速度较均匀,平均P波速度约4.8km/s,下部相对于第二层来说为一弱梯度层,梯度约0.35km·s^-1/km,P波速度在5.1~6.25km/s之间.该层的底界为结晶基底,其结晶基底西南深东北浅,形成一个向天山方向上翘的斜坡,似乎显示出坚硬的塔里木块体在插入天山下时受阻的上部地壳结构特征;第四层比较均匀,速度约为6.3km/s.在4km深度左右有一横向速度异常变化,推断可能与隐伏的麦盖提断裂及下苏洪一麦盖提断裂有关,但未见这些断裂延伸至地表及穿过基底的结构特征.伽师强震群的发震构造至少应位于11km深度以下的中下地壳之中. 展开更多
关键词 伽师强震群区 高分辨折射 有限差分反演 哈格多恩原理 折射波前成像
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新疆伽师强震群区的InSAR观测研究 被引量:32
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作者 乔学军 郭利民 《大地测量与地球动力学》 CSCD 北大核心 2007年第1期7-13,共7页
利用欧空局提供的ERS1/2 SAR数据,结合美国NASA的高精度SRTM数字高程模型DEM,获得了1996~1999年间伽师强震群部分地区的差分干涉图像。结果表明,该地区同期的地震活动及地壳形变主要受东西向和北东东向断层的影响,柯坪断裂带南北... 利用欧空局提供的ERS1/2 SAR数据,结合美国NASA的高精度SRTM数字高程模型DEM,获得了1996~1999年间伽师强震群部分地区的差分干涉图像。结果表明,该地区同期的地震活动及地壳形变主要受东西向和北东东向断层的影响,柯坪断裂带南北两侧块体的差异运动量约为5mm/a(LOS方向),其中1998年8月2日Ms6.0地震和27日Ms6.6地震可能与隐伏断层无关。 展开更多
关键词 伽师强震群 INSAR 隐伏断层 天山 差分干涉图像
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利用尾波包络线反演方法研究伽师强震群区地壳的非均匀结构 被引量:6
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作者 王勤彩 陈章立 +2 位作者 Y.Asano 郑斯华 A.Hasegawa 《地球物理学报》 SCIE EI CAS CSCD 北大核心 2009年第1期90-98,共9页
以单次散射模型、球形辐射源、一维线性速度模型为基础计算理论包络线,通过尾波归一化方法把理论与观测包络线结合起来形成非线性方程组,用迭代最小二乘方法反演伽师强震群区的散射系数空间分布.结果表明,伽师强震群区下方中上地壳中存... 以单次散射模型、球形辐射源、一维线性速度模型为基础计算理论包络线,通过尾波归一化方法把理论与观测包络线结合起来形成非线性方程组,用迭代最小二乘方法反演伽师强震群区的散射系数空间分布.结果表明,伽师强震群区下方中上地壳中存在明显的非均匀结构.在10~25km各深度图像上,研究区中部都存在一低散射系数区,这个低散射系数区在10km、15km深度被高散射系数区包围,在20km深度仅其东侧存在高散射系数区.1997年的7次Ms≥6.0级地震发生在研究区中部的低散射系数区内或低散射系数区向高散射系数区过渡带的低散射系数一侧. 展开更多
关键词 伽师强震群区 散射系数 尾波包络线 地壳的非均匀结构
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伽师地区强震群前后地壳运动变形的数值模拟 被引量:9
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作者 赵齐乐 秦小军 +4 位作者 乔学军 王琪 曾心传 吴云 陈文胜 《地壳形变与地震》 CSCD 2000年第4期29-35,共7页
运用 DDA( Discontinuous Deformation Analysis)方法 ,用 GPS测量资料模拟了伽师强震群前后的地壳运动及变形的演化过程。模拟结果表明 :1994~ 1998年整个研究区域以南北向压应变增大为主 ,帕米尔东北侧和南天山的应变率较大。伽师及... 运用 DDA( Discontinuous Deformation Analysis)方法 ,用 GPS测量资料模拟了伽师强震群前后的地壳运动及变形的演化过程。模拟结果表明 :1994~ 1998年整个研究区域以南北向压应变增大为主 ,帕米尔东北侧和南天山的应变率较大。伽师及邻近区域有明显的南北向挤压为主的应力集中。若强制应力集中块体沿最大剪应力方向 ( NEE向 )破裂 ,在伽师地区会出现显著的应力降。相对喀什的速率场表明 :帕米尔与南天山有较大的南北向相对挤压运动 ,由于帕米尔向北运动的带动使塔里木块体有微弱的右旋运动。破裂后托特拱孜断裂和柯坪断裂出现相对左旋运动 ,能量有沿着断裂向北东东方向传递的趋势。 展开更多
关键词 强震群 GPS观测 数值模拟 地壳变形 地震前兆
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