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1.
Geometric form of Haiyuan fault zone in the crustal interior and dynamics implications 总被引：1，自引：0，他引：1
The deep seismic reflection data on profile HY2 are reprocessed by the method of simultaneous inversion of velocity distribution
and interface position. By the travel-time inversion with the data of the diving wave Pg and fault plane reflection wave,
we determine the geometric form and velocity of Haiyuan fault zone interior and surrounding rock down to 10 km depth. The
measured data show that the amplitudes have strong attenuation in the range of stake number 37–39 km, suggesting the fault
zone has considerable width in the crustal interior. The results of this paper indicate that to the north of the fault zone
the crystalline basement interface upheaves gradually from southwest to northeast and becomes shallow gradually towards northeast,
and that to the south of the fault zone, within the basin between Xihua and Nanhua mountains, the folded basement becomes
shallow gradually towards southwest. The obliquity of the fault zone is about 70° above the 3 km depth, about 60° in the range
of the 3–10 km depths. From the results of this paper and other various citations, we believe that Haiyuan fault zone is in
steep state from the Earth’s surface to the depth of 10 km.
Foundation item: Joint Seismological Science Foundation of China (201001) and State Key Basic Research Development and Programming Project
(95-13-02-02).
Contribution No. RCEG200308, Exploration Geophysical Center, China Earthquake Administration. 相似文献
2.
DEFORMATION CHARACTERISTICS AND KINEMATIC PARAMETERS INVERSION OF HAIYUAN FAULT ZONE BASED ON TIME SERIES INSAR 
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下载免费PDF全文 Located at the bend of the northeastern margin of Qinghai-Tibet Plateau, the Haiyuan fault zone is a boundary fault of the stable Alashan block, the stable Ordos block and the active Tibet block, and is the most significant fault zone for the tectonic deformation and strong earthquake activity. In 1920, a M8.5 earthquake occurred in the eastern segment of the fault, causing a surface rupture zone of about 240km. After that, the segment has been in a state of calmness in seismic activity, and no destructive earthquakes of magnitude 6 or above have occurred. Determining the current activity of the Haiyuan fault zone is very important and necessary for the analysis and assessment of its future seismic hazard.
To study activity of the Haiyuan fault zone, the degree of fault coupling and the future seismic hazard, domestic and foreign scholars have carried out a lot of research using geology methods and GPS geodetic techniques, but these methods have certain limitations. The geology method is a traditional classical method of fault activity research, but dislocation measurement can only be performed on a local good fault outcrop. There are a limited number of field measurement points and the observation results are not equally limited depending on the sampling location and sampling method. The distribution of GPS stations is sparse, especially in the near-fault area, there is almost no GPS data. Therefore, the spatial resolution of the deformation field features obtained by GPS is low, and there are certain limitations in the kinematic parameter inversion using this method.
In this study, we obtain the average InSAR line-of-sight deformation field from the Maomaoshan section to the mid-1920s earthquake rupture segment of the Haiyuan earthquake in the period from 2003 to 2010 based on the PSInSAR technique. The results show that there are obvious differences between the slip rates of the two walls of the fault in the north and the south, which are consistent with the motion characteristics of left-lateral strike-slip in the Haiyuan fault zone. Through the analysis of the high-density cross-fault deformation rate profile of the Laohushan segment, it is determined that the creep length is about 19km. Based on the two-dimensional arctangent model, the fault depth and deep slip rate of different locations in the Haiyuan fault zone are obtained. The results show that the slip rate and the locking depth of the LHS segment change significantly from west to east, and the slip rate decreases from west to east, decreasing from 7.6mm/a in the west to 4.5mm/a in the easternmost. The western part of the LHS segment and the middle part are in a locked state. The western part has a locking depth of 4.2~4.4km, and the middle part has a deeper locking depth of 6.9km, while the eastern part is less than 1km, that is, the shallow surface is creeping, and the creep rate is 4.5~4.8mm/a. On the whole, the 1920 earthquake's rupture segment of the Haiyuan fault zone is in a locked state, and both the slip rate and the locking depth are gradually increased from west to east. The slip rate is increased from 3.2mm/a in the western segment to 5.4mm/a in the eastern segment, and the locking depth is increased from 4.8km in the western segment to 7.5km in the eastern segment. The results of this study refine the understanding of the slip rate and the locking depth of the different segments of the Haiyuan fault zone, and provide reference information for the investigation of the strain accumulation state and regional seismic hazard assessment of different sections of the fault zone. 相似文献
3.
为了获得三维地震透射成像技术在活断层探测中的有效性和应用价值的评价,在银川盆地中北部布设了一个三维地震透射台阵,利用该台阵获得的基底初至折射波和莫霍界面反射波资料,采用有限差分反演、时间项反演和连续速度模型反演方法,对台阵区域基底及上地壳结构进行了分析.结果表明：研究区基底呈东西浅、中部深的界面形态,且西陡东缓,最深处大致位于芦花台至西大滩一带,埋深达7 km.芦花台断层、银川—平罗断层、黄河断层在研究区内均表现为北北东走向的速度差异条带,且断层两侧基底及沉积界面埋深存在显著变化.芦花台断层东倾,倾角较陡,延伸至研究区基底之下;银川—平罗断层倾向西,是一条超基底的隐伏断层;黄河断层西倾,延伸深度超过研究区基底.本探测结果证明,初至折射波与莫霍面反射波探测相结合的三维地震透射台阵技术能够给出研究区上地壳三维细结构图像,不仅可以揭示主要断裂的展布位置、浅部空间形态和特征,而且可以揭示断裂向基底之下的延伸状况. 相似文献
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彭州断裂是龙门山山前一条重要的隐伏断裂.为了调查彭州断裂的位置、性质及其活动性,5·12汶川MS8.0地震发生后,作者采用可控震源和高精度的地震反射勘探方法,对彭州隐伏断裂进行了高分辨率地震反射成像.本文利用获得的浅层地震剖面资料并结合石油地震反射剖面,给出了彭州断裂的空间展布特征以及断裂两侧的新生代地层厚度.结果表明,彭州断裂为一条走向NE、倾向NW、倾角约为58°～62°的逆断层,该断层向上错断了第四纪沉积层,具有明显的第四纪活动,向下大约在深度8～10 km左右收敛到向西缓倾的滑脱面之上.研究结果为评价断裂的活动性和灾后重建提供了地震学证据. 相似文献
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对穿过宁夏海原大震区西安州(N36.5°,E105.5°)北至同心县韦州(N37.28°,E106.48°)的大地电磁测深剖面，采用远参考道大地电磁方法进行测量和资料处理，得到高精度的数据如视电阻率、阻抗相位、二维偏离度、最佳主轴方位角等. 依据这些数据，对测区的电性结构进行了定性分析和二维定量反演解释. 结果表明，沿剖面可以分成5个电性区块，与西、南华山隆起(Ⅰ)、兴仁堡—海原盆地(Ⅱ)、中卫—清水河盆地(Ⅲ)、中宁—红寺堡盆地(Ⅳ)和鄂尔多斯西缘带(Ⅴ)对应，各区块的边界由大断裂构成. 地表到深度10km左右，西、南华山隆起和鄂尔多斯西缘带呈高阻特性，兴仁堡—海原、中卫—清水河、中宁—红寺堡三个盆地的电阻率较低且呈盆地凹陷形状，盆地基底显示为西南深东北浅的簸箕状起伏形态，基底最深约为8km. 西、南华山隆起、中卫—清水河盆地和鄂尔多斯西缘带的下地壳为“正常”电阻率结构. 兴仁堡—海原和中宁—红寺堡盆地的下地壳上部为“异常”低电阻率带. 1920年的海原大震区存在明显的电性结构差异，震区西南侧和上部区域为相对高阻，东北侧和下部区域为相对低阻. 相似文献
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对获得的玉树震区的人工地震测深资料,利用正演拟合地震测深方法进行处理与计算,获得了玉树震区的地壳速度结构和构造的基本特征。结果表明,不同区域的地壳速度结构在纵向和横向上均具有明显的非均匀性。 地壳呈层状结构,研究区结晶基底界面起伏较大,玉树附近下方较厚达8km左右,在400.0km桩号向北至温泉方向基底结构逐渐减薄为2.5km。基底界面的凹陷、隆起与不同的地质构造单元具有较好的对应关系;地壳厚度由囊谦、玉树附近的72km向南、北逐渐减薄为62km。在200.0～400.0km桩号之间二维速度等值线及壳内界面起伏变化较大,在玉树附近下方莫霍面有一弧形凹陷。 相似文献
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考虑到面波频散对介质S波速度、接收函数对界面深度的各自敏感性优势,综合利用面波和接收函数资料实现联合反演,求取滇西地区壳幔速度结构. 本文利用适配滤波频时分析技术处理覆盖滇西地区的长周期面波资料,获得105～1050s周期范围内的面波群速度频散,进而利用分格反演方法提取研究区内1°×1°网格纯路径频散;基于滇西地区宽频带三分量远震记录,经反褶积后得到台站下方的远震P波接收函数. 联立面波纯路径频散信息和接收函数资料建立系统方程,利用阻尼最小二乘法实现联合反演,从而获得滇西地区壳幔S波速度结构. 结果表明,滇西地区以红河断裂为界,东西两侧壳幔结构存在明显差异,断裂西侧约20km深度处存在一厚度为10km左右的低速层,而东侧并不明显;滇缅泰块体上的畹町、沧源一带属于上地幔低速区,而另一个地幔低速区则位于滇中块体上的康滇古隆起上,两处地幔低速区与大地高热流分布、强震活动具有较好的对应关系. 相似文献
10.
玛沁-兰州-靖边地震测深剖面地壳速度结构的初步研究 总被引：75，自引：27，他引：75
为研究青藏高原块体和鄂尔多斯地块间的相互作用和构造变形的深部驱动机制,布设了1000km长的玛沁-兰州-靖边综合地球物理探测剖面.本文只介绍由人工地震观测资料所得到的初步结果.地壳分层性明显,以C界面为界,总体上可分为上、下地壳两大部分,每个部分又包含一些次一级的界面;横向变化的总趋势是从东北至西南地壳逐渐变厚,地壳厚度的变化主要由下地壳厚度的变化所引起;地壳平均速度,总的变化趋势是自东北向西南逐渐降低,其中在泽库以西和海原地区的速度值明显偏低;在泽库以西存在多个壳内低速层,在海原附近存在一个低速层;壳内反射界面,沿测线由东北至西南逐步增多;从地震反射波形来看,在海原地区Pc波非常强,且延续时间长;另外,在海原地区和泽库以西地区Pm波的复杂性系数很大,远远大于其他地段的值.以上结果表明,泽库以西地区和海原地区地壳-上地幔存在着明显结构异常,反映了巴颜喀拉地块和柴达木地块、祁连地块和鄂尔多斯地块间的相互作用 相似文献
11.
通过在上海地区开展深、浅地震反射、地震宽角反射/折射、高分辨地震折射和大地电磁测深等联合剖面探测, 获得了该地区近地表至Moho面的精细速度结构、电性结构和深浅构造关系.结果表明, 该地区地壳可划分为上、中、下三个组成部分.其中,上地壳厚为12～14 km,波速为57～59 km/s;中地壳厚度约为10 km,波速为59～62 km/s;下地壳厚为10～11 km, 波速为62～63 km/s,Moho面深度约为32 km.剖面浅部地质构造复杂,共解释出12条特征明显的断裂.其中,除3条断裂错断结晶基底（G界面）并向下延伸至上地壳底界面外,其他断裂均在深度3～5 km以上终止或收敛于G界面之上.此外,仅在剖面西侧基底下部约13～15 km埋深处发现一厚度在2 km左右的壳内高导层.所以,在综合各方面资料后分析认为,在剖面经过地区不存在发生大地震的深部构造条件,近地表所存在的活动断层是未来产生对该区有影响地震的震源区. 相似文献
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利用穿越区域南段为秦岭褶皱带山区,中段为渭河断陷盆地,北段为鄂尔多斯地台南缘的宽角反射/折射地震测深剖面所获得的资料对该区地壳结构进行研究.结果表明:该区地壳呈明显的分层、分区结构;上下地壳的分界是由壳内反射波较为连续可靠的P2以及P3所确定的.鄂尔多斯地台是本区M界面最深的地区,地壳厚度大,达42 km左右,结构相对简单,结晶基底浅. 秦岭褶皱带的地壳厚度约37~38 km,结晶基底浅,甚至出露.渭河断陷盆地莫霍界面相对两侧明显且不对称的上隆,地壳结构复杂;而莫霍界面相对鄂尔多斯地块突变隆起和上地幔高速物质侵入于下地壳,是该区发生中强地震的深部构造背景. 相似文献
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为了研究北京平原区的地壳结构特征、断裂的空间展布、断裂活动性以及深浅构造关系,在北京平原区的南部完成了1条长90 km的深地震反射剖面.探测结果表明,该区地壳以双程反射时间(TWT)6～7 s的强反射带Tc为界分为上地壳和下地壳,上地壳厚约18～19 km,下地壳厚约16～17 km,Moho界面深度约为34～35 km.该区结晶基底起伏变化较大,上、下地壳分界面和Moho界面都是一个具有一定厚度的过渡带.上地壳反射层位丰富,断裂构造发育,构造形态清晰.在夏垫断裂西北,剖面揭示了4～5组能量较强的反射震相,表现为典型的隆起区特征;在夏垫断裂东南,上部为一套向东南倾伏的密集强反射层,下部为一套形态各异、结构复杂的强反射层,这些反射具有典型的沉积盆地特征,盆地最深处约为11 km.剖面揭示的地壳深断裂倾角较陡,向上切穿了上、下地壳分界面,延伸到上地壳沉积盆地的底部,向下切穿了壳幔过渡带,与上部断裂和沉积盆地构成了独特的组合关系. 相似文献
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对11炮宽角地震反射/折射的Pg波走时数据进行了反演,结果表明:阿尼玛卿缝合带东段基底速度结构整体呈低速带分布,两侧的速度分布相对均匀;缝合带内基底界面剧烈下凹,最深达5.5 km,不存在稳定的基底界面;松潘-甘孜微块体基底界面整体埋深达3.5 km,相对平坦,其中部略微下凹;从缝合带过渡到西秦岭褶皱带,基底界面急剧抬升至1.8 km,之后迅速下降至4.7 km,然后趋于平坦;缝合带的地壳变形存在挤压和走滑两种形式,在缝合带及邻近地区,上部地壳物质曾有过向北方向逃逸的迹象. 相似文献
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海原一六盘山构造带是青藏高原东北缘地区的一条重要边界,在海原断裂带和六盘山断裂带接触区形成了特殊的马东山挤压阶区,本文对跨过该挤压阶区一条密集测点大地电磁剖面数据进行了处理和二维反演,获得的深部电性结构图像揭示在马东山挤压阶区深部电性结构表现为在高阻背景下镶嵌多个向西南倾斜的低阻条带电阻率结构样式,并在深度约25 km汇聚到中下地壳低阻层内,共同组成"正花状"结构;海原一六盘山构造带西南侧到陇中盆地区间呈现高、低阻相互"楔合"的深部结构特征,而其东北侧的鄂尔多斯西缘带自地表到中下地壳为较完整的高阻块体.另外结合跨过海原断裂带中段和西秦岭造山带的大地电磁探测结果,对海原一六盘山构造带分段性及其两侧的陇中盆地和鄂尔多斯地块的接触关系进行了研究分析.大地电磁探测成果佐证了在海原断裂带中段为具有走滑特点的断裂,而其尾端与六盘山断裂带斜交区域的马东山地区发生了强烈的逆冲推覆与褶皱变形;活动构造研究发现沿海原断裂带所产生的左旋走滑位移被其尾端的马东山、六盘山以东西向的地壳缩短调节吸收,GPS观测表明青藏高原东北缘地区现今构造变形分布在海原一六盘山构造带以西上百公里的范围内,陇中盆地一海原一六盘山构造带和鄂尔多斯地块一线的深部电性结构图像也很好地解释了该区变形状态:海原一六盘山构造带带及西南盘的陇中盆地的中下地壳非常破碎,在青藏高原向北东方向的推挤下容易发生变形,而北东盘鄂尔多斯地块地壳结构完整,很难发生构造变形.对海原一六盘山构造带马东山阶区和龙门山构造带的深部电性结构及变形特征等进行了比较分析,发现该区有与2008年汶川地震相似的深部构造背景,应重视该区强震孕育环境的探测研究. 相似文献
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基于甘肃省夏河县—陕西省靖边县剖面的8次人工地震初至波数据, 利用有限差分走时方法反演得到了沿该剖面长约650 km的上部地壳速度结构和结晶基底的深度分布． 反演结果显示: 海原构造区西侧的西秦岭—祁连山褶皱区上部地壳的横向非均匀性明显, 基底深度从1 km到5 km不等, 反映了褶皱区改造变形强烈的构造特征; 其东侧的鄂尔多斯盆地基底深度约为5—6 km, 其速度均匀、 稳定, 上地壳呈弱速度梯度特征; 海原构造区及海原弧形断裂带附近上部地壳的破坏变形最严重, 区内横向高低速相间分布． 综上可知, 海原构造区东西两侧上地壳结构的显著差异揭示了其结构复杂性的成因及其与地震活动性的关系． 相似文献
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Introduction Artificial seismic sounding is a geophysical exploration technique developed in prospectingfor oil and gas and other mineral resources and consists of reflection wave and refraction waveexploration methods. With rapid development of computer techniques and sounding instruments,the reflection wave method became a high-resolution imagery technique for underground struc-tures and is widespreadly used in detection of underground caves and in engineering exploration.In previous se… 相似文献
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By using moving average method to separate Bouguer gravity anomaly field in Sichuan-Yunnan region, we got the low-frequency Bouguer gravity anomaly field which reflects the undulating of Moho interface. The initial model is obtained after seismic model transformation and elevation correction. Then, we used Parker method to invert the low-frequency Bouguer gravity anomaly field to obtain the depth of Moho interface and crustal thickness in the area. The results show that the Qinghai-Tibet block in the northwest of the study area deepens and thickens from the edge to the interior, with the depth of Moho interface and the crust thickness of about 52~62km and 54~66km, respectively. The depth of Moho interface in Sichuan Basin is about 38~42km. In Sichuan-Yunnan block, the depth of Moho interface is about 42~62km from southeast to northwest. Beneath the West Yunnan block, west of the Red River fault zone, the Moho depth is about 34~52km from south to north. The Longmen Mountains and Red River fault zone are the gradient zone of the Moho depth change. Along the Red River fault zone, the depth difference of Moho interface is increasing gradually from north to south. No obvious uplift is found on the Moho interface of Panzhihua rift valley. The depth of Moho interface distribution in Sichuan and Yunnan is obviously restricted by the collision between the Indian plate and the Eurasian plate and the lateral subduction of the Indo-China peninsula. The mean square error of the depth of Moho interface is less than 1.7km between the result of divisional density interface inversion and artificial seismic exploration. At the same time, we compared the integral with divisional inversion result. It shows that:in areas where there is obvious difference between the crust velocity and density structure in different tectonic blocks, the use of high resolution seismic exploration data as the constraints to the divisional density interface inversion can effectively improve the reliability of inversion results. 相似文献
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利用三河—平谷8.0级大震区实施的深地震反射剖面与宽角反射剖面探测方法获得的结果进行了综合研究和解释. 结果表明：两种探测方法给出的地壳基本分层是一致的,在三河—平谷大震区上地壳的埋深为21～23km,莫霍界面的深度为36～37km;该地区基底结构起伏变化较大,浅部断裂发育,在确定的数条断裂构造带中夏垫断裂是一条特征明显、深浅共存的断裂构造带;震源区周围差异明显的速度异常结构和特殊而复杂的地质构造环境意味着这些部位是发生大地震的有利部位;该地区莫霍界面起伏变化和较厚的反射叠层以及局部复杂的楔形反射带的存在等现象表明,该地区地壳结构发生过强烈的挤压、变形,同时也反映出岩浆活动对下地壳结构进行了物质的和结构的强烈改造,从而构成了该地区复杂的地壳深部结构,可将其视为三河—平谷8.0级大地震孕育和发生的深部要素. 相似文献