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1.
通过对云南数字地震台站的宽频带远震接收函数反演，获得了云南地区数字地震台站下方0-0km深度范围的S波速度结构.结果表明，云南地区地壳厚度变化剧烈，中甸、丽江等西北部地区，地壳厚度达62km左右，景洪、思茅和沧源等南部地区，地壳厚度仅为32-34km.厚地壳从西北部向东南方向伸展，厚度和范围逐渐减小，至通海一带地壳厚度减为42km，其形态和范围与小江断裂和元江断裂围成的川滇菱形块体相一致.地壳厚度较小的东、南部地区Moho面速度界面明显；在地壳厚度较大或变化剧烈的地区，Moho面大多表现为S波速度的高梯度带.云南地区S波速度结构具有很强的横向不均匀性.km深度以上，北部地区S波速度明显低于南部地区，在-20km深度范围内，北部地区的S波速度比南部地区高.地壳内部S波速度界面的连续性较差，低速层的深度和范围不一，近一半的台站下方不存在明显的低速层.受南部地区上地幔的影响，40-50km深度范围内，S波速度南部高、北部低，高速区随深度增加逐渐向北推移，低速异常区形态与川滇菱形块体的形态趋向一致.70-80km深度的上地幔速度分布与云南地区大震分布具有一定的相关性. 相似文献
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以川滇甘陕地区263个有详细场地资料的强震台站获得的2 388条强震记录为基础资料,对每一条水平向强震记录采用差分进化算法确定了动力放大系数β_(max)。在考虑震级、震中距和场地类别基础上,分别统计不同震级、震中距和场地类别的动力放大系数β_(max),并研究了它们对动力放大系数β_(max)的影响。统计结果表明,川滇甘陕地区放大系数谱平台值随着震级的增大而增大,变化规律显著;随震中距没有明显变化;根据统计结果,本文建议川滇甘陕这一地区的Ⅰ类场地动力放大系数β_(max)取2.5,Ⅱ类场地取2.7,本文的研究结果对进一步合理确定动力放大系数β_(max)有重要参考价值。 相似文献
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利用广东及其邻域福建、江西、湖南、广西、海南、台湾共82个宽频带数字地震台的远震资料, 计算获得了所有台站下方的体波接收函数,并通过接收函数 搜索叠加方法反演了这些台站下方的地壳厚度和平均泊松比。研究结果表明,广东及周周边地区的地壳厚度介于26.8～33.6km之间,平均为29.5km。由西北到东南逐渐变薄,为大陆地壳向大洋地壳的缓慢过渡。珠江三角洲、粤西、粤桂琼交界、广西南宁、广东南澳地区地壳厚度较薄,为25.0－28.0km;海南的翁田、广东的湛江、上川岛地壳厚度最薄,在26km左右;福建明溪、湖南永州周边地区地壳厚度较厚、地壳厚度在31.0～34.0km间。研究区域内地壳泊松比为0．20～0．29,海南岛的东南部,粤东和闽西的沿海地区,以及江西南部具有明显的高泊松比,这可能与这些地区具有广泛的温泉分布和高热流值的特性有关。地壳厚度和泊松比的分布具有明显的分块特征,并与断层和历史地震的分布相关。 相似文献
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广东及其邻域的地壳厚度和泊松比分布 总被引：1，自引：0，他引：1
利用广东及其邻域福建、江西、湖南、广西、海南、台湾共82个宽频带数字地震台的远震资料,计算获得了所有台站下方的体波接收函数,并通过接收函数H-κ搜索叠加方法反演了这些台站下方的地壳厚度和平均泊松比.研究结果表明,广东及其周边地区的地壳厚度为26.8 ～ 33.6km,平均为29.5 km.由西北到东南逐渐变薄,表现出大陆地壳向大洋地壳的缓慢过渡过程.珠江三角洲、粤西、粤桂琼交界、广西南宁、广东南澳等地区地壳厚度较薄,为25.0～28.0km;海南的翁田、广东的湛江、上川岛等地壳厚度最薄,在26km左右;福建明溪、湖南永州周边地区地壳厚度较厚,为31.0～34.0km.研究区域内地壳泊松比为0.20～0.29,海南岛的东南部、粤东和闽西的沿海地区以及江西南部具有明显的高泊松比,这可能与这些地区具有广泛的温泉分布和高热流值的特性有关.地壳厚度和泊松比分布的分块特征明显,并与断层和历史地震的分布有关. 相似文献
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云南地区地壳厚度与泊松比变化及其意义 总被引：1，自引：0，他引：1
利用云南省“十五”期间建成的46 个宽频带地震台2007 年7 月～ 2008 年7 月间记录的6 级以上远震波形资料,提取各台站下方的P 波接收函数,并据此计算和分析了云南地区的地壳厚度变化情况和泊松比的分布特征。得到的较前更高空间分辨率的结果表明,云南地区的地壳厚度总体呈现“北深南浅”的特征,最北部的中甸台地壳厚度是53. 5km,而最南端的勐腊台仅为31. 7km。红河断裂的边界作用较为明显,断裂以东的地壳厚度较大,以西的则较小;断裂西侧的地壳厚度变化较为舒缓,东侧则变化剧烈,且自东南向西北厚度逐渐加深。在川滇菱形块体及周围存在2 个上地幔隆起,一个隆起的中心轴在楚雄-元谋一带,另一个隆起的中心轴在东川附近。从泊松比的分布情况来看,研究区内泊松比的分布是不均匀的,自南向北存在较大差异,北部的中甸台处达到最大0. 289,而南部的景谷台处仅为0. 146,与地壳厚度“北深南浅”的趋势基本相一致。泊松比在滇东块体内较低,在滇中块体内较高;北纬24°以北地区泊松比显然比以南地区要高。总的分布状态为:川滇菱形块体周围的泊松比属于中-高值(0. 26≤σ≤0. 29)。 相似文献
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山东地区位于华北东部,包含沂沭断裂带、鲁西隆起等重要构造单元,地质构造演化非常复杂,但目前尚缺乏对山东地区整体的地壳结构、壳内形变、壳幔耦合等方面的研究.本文基于该地区52个地震台站两年的波形记录,采用接收函数Ps转换波分裂和H-κ叠加的方法得到了研究区地壳各向异性、平均地壳厚度以及泊松比特征,为该地区的构造演化提供了重要的地震学约束.结果 表明,研究区地壳结构存在较强的横向不均匀性.鲁西隆起南部地壳各向异性方向可能与断裂和地壳内部的构造拆离有关.泰山地区地壳厚度与泊松比呈现负相关,地壳各向异性不明显,表明泰山处在快速隆升阶段.胶东地区东部较小的地壳厚度和泊松比与地幔上涌和苏鲁造山带发育的超高压变质岩有关.沂沭断裂带南北段的地壳结构具有显著差异,南段地壳厚度与泊松比存在明显的横向变化,表明南段可能存在剧烈的地幔上涌.较厚的沉积层使得济阳凹陷内台站下方的泊松比偏小,而较薄的铁镁质下地壳层则可能是胶北隆起部分台站下方泊松比偏小的主要原因. 相似文献
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运用H-k扫描和人工读取震相到时两种方法对比研究云南地区地壳结构 总被引：1，自引：0，他引：1
利用云南及其邻区59个宽频地震台站记录到的30°~100°远震资料,采用P波接收函数方法对云南地区的地壳厚度和地壳平均泊松比分布进行分析。研究结果显示:用H-k扫描和人工读取震相到时两种方法得到的云南地区地壳厚度和泊松比分布情况较为吻合。研究区域内Moho面埋深南浅北深,横向变化达30~40 km。在川滇菱形块体东南缘,地壳厚度等值线呈东南向舌状突出。泊松比呈块体分布特征,断裂两侧差异显著。高泊松比的分布主要集中在滇缅泰块体内和研究区域北部以及小江断裂附近,这与该区处于印度板块与欧亚板块碰撞俯冲前缘的特殊地理位置有关。 相似文献
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本文利用径向和切向接收函数确定地壳各向异性的方法,处理了布设在青藏高原东北缘甘东南地区、横跨西秦岭北缘等断裂的24个密集宽频带流动台站远震资料,得到了研究区地壳各向异性特征.结果显示,平均快波方向呈现NW-SE、NWW-SEE及NNW-SSE,平均分裂时间0.56 s.甘东南中部及北部地区快波方向与GPS速度方向、前人利用XKS波分裂获取的快波方向及该地区断层展布方向基本一致,说明该地区壳幔运动可能是耦合的.同时研究区南部少数台站快波方向呈现NNW-SSE,与断裂方向及GPS速度方向有一定夹角,表明台站下方壳幔运动可能是解耦的.全区快波方向自北向南由近E-W逐渐转变为NW-SE,最后变为NNW-SSE.据此推测地壳在该区的变形挤压有顺时针方向旋转的趋势,这与该区块体挤压应力方向一致. 相似文献
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青藏高原东南缘地下深部结构的研究对了解青藏高原的变形机制和动力学过程具有重要意义.本文利用四川、云南固定台站记录到的远震波形资料,首先采用接收函数H-k叠加方法获得青藏高原东南缘台站下方的地壳厚度和波速比.进而利用接收函数一次转换波和多次波幅度信息确定了青藏高原东南缘Moho面上的S波速度和密度跃变.研究结果表明:研究区由南到北地壳厚度逐渐增加,从永德、沧源、孟连地区的33 km左右增至巴塘地区的69.7 km左右,厚度变化了近乎37 km.四川盆地和松潘甘孜块体南部的姑咱地区具有高泊松比、速度密度跃变较小特征,表明这两个地区含有较多铁镁物质.腾冲地区、龙门山西侧的汶川地区、四川盆地西南缘的沐川地区以及则木河断裂的石门坎至东川地区同属于高泊松比、速度密度跃变较大,显示这些地区壳内存在部分熔融. 相似文献
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Structure and Significance of S-wave Velocity and Poisson’s Ratio in the Crust beneath the Eastern Side of the Qinghai-Tibet Plateau 总被引：2，自引：0，他引：2
The receiver functions of body waves of distant earthquakes obtained for the regions beneath 41 digital stations (Lhasa and
GANZ in Tibet, Mandalay and Rangoon in Myanmar, SHIO in India, CHTO in Thailand, and station network in Sichuan and Yunnan)
were used to invert for S-wave structure in the crust and upper mantle in Sichuan, Yunnan, and their surrounding areas. Meanwhile
the distribution characteristics of the Poisson’s ration and the crustal thickness in Sichuan and Yunnan areas were also obtained.
Results indicate that the depth of Moho beneath the eastern side of Qinghai-Tibetan plateau varies strikingly. It is obvious
that the greatest changes in crustal thickness occur in a north-south direction. The crustal thickness decreases from north
to south, being as thick as 70 km in eastern Tibet, the northern portion of our area of interest, and less than 30 km in Chaing
Mai and Rangoon, the southern portion of our area. There are, however, exceptions regarding the trend. The thickness exhibits
an east-west variation trend in the area from Ma’erkong-Kongding in Sichuan to Lijiang in Yunnan. In general the Jinpingshan-Longmenshan
fault and Anninghe fault can be taken as the boundaries of this exception area. The thickness in Kongding in the west is 68 km,
while it is only 39 km in Yongchuan in the east. Moreover the Poisson’s ratio values in the blocks of central Sichuan and
Sichuan-Yunnan Diamond are high, and a low velocity layer in the crust of this area can be obviously detected. The distribution
characteristics of the high Poisson’s ratio and the low velocity of the crust in this block correspond to the tectonic structure,
being in contrast with the surrounding areas. Combining with the distribution features of the modern tectonic stress field,
it is deduced that the Sichuan-Yunnan area is probably the channel through which the materials of the lithosphere flow eastward. 相似文献
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本文利用川西地震台阵记录到的远震P波走时数据和非线性层析成像算法,获得龙门山地区400 km深度范围内的三维P波速度结构.为了适应川西地区复杂的地质结构,本文的层析成像方法采用了快速行进三维走时计算算法和Tarantola非线性反演算法.我们的结果揭示了川滇地块、松潘-甘孜地块和四川盆地三个不同地块构造差异及该区深部动力学特征.本文的研究表明：1）研究区地壳上地幔P波速度结构具有较为明显的分区特征,松潘-甘孜地块和川滇地块岩石圈速度较低,四川盆地岩石圈速度较高,四川盆地的岩石圈厚度从南250 km向北逐渐减薄至100 km.松潘-甘孜地块上地幔存在地幔上涌的特征.2）川滇地块和四川盆地仅是垂直接触关系,而在龙门山地区四川盆地前缘存在减薄的现象,并伴随松潘-甘孜地块上地幔低速物质有侵入四川盆地岩石圈下方的特征,这显示了四川盆地与松潘-甘孜地块和川滇地块的动力学关系的差异.3）以映秀为界,龙门山断裂带被从松潘-甘孜侵入的低速异常分为南北两段：龙门山南段和龙门山北段,汶川大地震及其余震序列均分布在龙门山断裂带的北段.在青藏高原向东挤压和地幔上涌的双重作用下造成松潘-甘孜地块隆升,由于汶川处于龙门山北段的最南端,应力容易在此集中.这些因素可能是汶川MS8.0地震的基本动力学背景.本文的结果不支持四川盆地的俯冲及层间流动的动力学模型. 相似文献
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地壳厚度和泊松比是反映地壳结构和内部物质组成的重要参数,能够为区域构造和动力学研究提供重要依据.本文基于福建地区分布相对均匀的88个测震台2014—2017年的远震波形数据提取P波接收函数,采用H-κ叠加获得台站下方的地壳厚度和泊松比,并与该地区已有的研究结果进行对比、分析及整合,最终获得了研究区117个观测台站下方的地壳厚度和泊松比,揭示了中国福建地区地壳结构和泊松比变化特征.结果显示:(1)研究区内地壳厚度整体较薄,在27.4~34.3 km之间,平均值为31.4 km.地壳厚度从西北往东南减薄,具有明显条带和块状特征,与地壳主要深大断裂的分布有一定相关性.本文以更为密集的台站结果进一步验证了研究区具有由陆壳向洋壳逐渐减薄的过渡特征,并揭示了地壳新的局部起伏.这也意味着福建地区从内陆到沿海并非线性减薄,存在小尺度横向非均匀性.(2)研究区内泊松比平均值为0.25,范围为0.20~0.30,北部整体偏高,南部整体较低,泊松比分布特征与该区地壳物质组成和矿物含量密切相关.沿海地区泊松比明显高于内陆地区,推测与沿海地区较高的热流值和幔源物质底侵过程有关.(3)地壳厚度与泊松比成负相关,推测在地壳伸展背景下,古太平洋板块俯冲华南大陆,幔源物质进入地壳,在造成莫霍面抬升的同时提高了泊松比. 相似文献
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Sliding-window cross-correlation method is firstly adopted to identify sPn phase, and to constrain focal depth from regional
seismograms, by measuring the time separation between sPn and Pn phases. We present the focal depths of the 17 moderate-sized
aftershocks (M
S⩾5.0) of the Wenchuan M
S8.0 earthquake, using the data recorded by the regional seismic broadband networks of Shaanxi, Qinghai, Gansu, Yunnan and
Sichuan. Our results show focal depths of aftershocks range from 8 to 20 km, and tend to cluster at two average depths, separate
at 32.5°N, i.e., 11 km to the south and 17 km to the north, indicating that these aftershocks are origin of upper-to-middle
crust. Combined with other results, we suggest that the Longmenshan fault is not a through-going crustal fault and the Pingwu-Qingchuan
fault may be not the northward extension of the Longmenshan thrust fault.
Supported by the National Natural Science Foundation of China (Grant Nos. 40604009 and 40574040) and Special Project for the
Fundamental R & D of Institute of Geophysics, China Earthquake Administration (Grant No.DQJB08B20) 相似文献
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造山带地区的复合力系作用往往使Moho界面发生变形,局部表现为倾斜状态.为了得到这些区域精确地壳速度比结构,本文基于H-κ方法发展了H-κ-θ方法.该方法不仅考虑了倾斜Moho层的响应,同时利用径向和切向接收函数信息,增加了对扫描的约束.利用该方法对青藏高原东南缘地壳厚度和速度比结构进行研究,结果表明：研究区内地壳明显存在不均匀性,松潘—甘孜地体平均地壳厚度约为60 km,四川盆地西缘约为47 km,扬子地台约为43 km,三江块体和扬子地台东南缘已接近正常地壳厚度;松潘—甘孜地体与扬子地台相邻部位地壳平均地震波速度比（Vp/Vs）普遍偏高,且四川盆地西侧发现一绕盆地边缘的弧形高Vp/Vs异常区（>1.88）,我们推测该异常可能由青藏高原向东逃逸的地壳流体受到高强度的四川盆地阻挡,在其西侧堆积所致. 相似文献
18.
GAO Jian YANG Yi-hai HUANG Shi-yuan YANG Cong ZHANG Yuan-sheng LIU Cun-xi LI Shao-rui HUA Qian 《地震地质》1979,42(1):147-162
The receiver function which carries the information of crustal materials is often used to study the shear-wave velocity of the crust as well as the crustal anisotropy. However, because of the low signal-to-noise ratio in Pms(P-to-S converted phase from the Moho), the crustal anisotropy obtained by shear-wave splitting technique for a single receiver function usually has large errors in general. Recent advance in the analysis method based on Pms arrival time varying with the back-azimuth change can effectively overcome the above defects. Thus in this paper, we utilize the azimuth variations of the Pms to study the crustal anisotropy in Chongqing region for the first time. According to the earthquake catalogue provided by USGS, seismic waveform of earthquakes with magnitude larger than 5.5 and epicenter distance range of 30°~90° between January 2015 and December 2016 are collected from 14 broadband seismic stations of Chongqing seismic network. We carry out the bootstrap resampling to test the reliability of the radial maximum energy method for the observation data. In addition, we also applied the receiver function H-Kappa analysis in this paper to study the crustal thickness and Poisson's ratio.
Our results show the crustal thickness ranges from 40~50km, and there is a thin and thick crust in the southern and northern Chongqing, respectively. The crustal average Poisson's ratio ranges from 0.23~0.31, the Poisson's ratio reaches the maximum value in the central part of Chongqing, while the Poisson's ratio in the northern and southern parts of Chongqing is obviously low. We obtain the crustal anisotropy from 9 stations in total. The delay time of crustal anisotropy distributes between 0.08s and 0.48s, with the average value of 0.22s. Among them, the CHS, QIJ and WAZ stations in central Chongqing have relatively large crustal delay time(>0.3s), followed by ROC station in the western Chongqing(0.25s), while the delay time in CHK station in northern Chongqing and WAS station in southern Chongqing are 0.08s, showing relatively weak crustal anisotropy. The fast polarization directions(FPDs)also change obviously from south to north. In southern Chongqing, FPDs are dominant in NNE-SSW and NEE-SWW, while the FPDs in WAZ station change to NWW-SEE, and the FPDs appear to be NW-SE in CHK in the northern Chongqing. In general, the FPDs are sub-parallel to the strikes of faults in most areas of Chongqing areas.
Combined with other results from GPS observations, tectonic stress field and XKS splitting measurements, the main conclusions can be suggested as following:The cracks preferred orientation in the upper crust is not the main source of crustal anisotropy in Chongqing area. The crust and lithospheric upper mantle in the eastern Sichuan fold belt(ESFB)and Sichuan-Guizhou fault fold belt(SGFFB)are decoupled, and the deformation characteristics in the north and south parts of ESFB and SGFFB is different. The complex tectonic deformation may exist beneath the mountain-basin boundary, causing the fast directions of crustal anisotropy different from that in other areas of ESFB and SGFFB. The faults with different strikes may weaken the strength of average crustal anisotropy in some areas. The crustal deformation in southern Dabashan nappe belt(DNB)may be mainly controlled by the fault structure. 相似文献
19.
Twenty broadband seismographs were deployed along Hongyuan, Sichuan to Wuwei, Gansu. 81 teleseismic events were recorded in one year. We computed receiver functions from teleseismic waveform data and obtained S wave velocity structure beneath each station along the profile by using receiver function inversion method. The results revealed that the crustal structure is very complex and crustal average S wave velocity is to be on the low side. Low velocity structure generally exists in the depth range of 10～40 km in the crust between Aba arc fault and northern edge fault of Qinling earth＇s axis and it is a tectonic feature of complex geological process such as ancient A＇nyemaqen Tethys ocean from closing and side colliding to subducted plate exhumed or thrust rock slice lifted. The Moho is about 50 km depth along the profile and is slightly deeper in the south than in the north. 相似文献
20.
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