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1.
Introduction The Yunnan region is located on the east margin of the collision zone between the Indian and Eurasian plates; it belongs to the south section of the N-S Seismic Belt of China and is the junc-ture of the Yangtze metaplatform, Songpan-Garz?fold system, Sanjiang fold system and South China fold system. This region has complex tectonic movements, crisscross faults and frequently occurring strong earthquakes, and hence it is one of the regions with the strongest earthquake ac-tivi… 相似文献
2.
根据云南地区的基阶瑞利波相速度频散资料，用面波层析成像方法反演得到该区域中上地壳S波速度结构. 给出了研究区域内在4个深度上的S波速度水平分布图像和沿100.5°E、24°N、25°N、26°N及27°N的S波速度-深度剖面图. 结果表明：在小江断裂与红河断裂围成的川滇菱形块体内，26～30km深度处的速度明显低于周边地区，其南段从地表到15km深度均为明显的低速区域. 云南地区的强震（M＞6.0）震中位置与S波速度分布图像具有明显的相关性，主要分布于高速与低速的过渡区域. 相似文献
3.
收集了南北地震带区域地震台网中292个地震台站2008年1月至2011年3月期间的地震波形数据,由频时分析方法提取了Love波相速度频散曲线,经过反演得到了研究区内的Love波相速度分布.根据Love波纯路径频散,采用线性反演方法对0.25°×0.25°的网格点进行了一维S波速度结构反演,利用线性插值获取了南北地震带地区的三维S波速度结构.结果显示了松潘—甘孜地体和川滇菱形块体地区的下地壳具有明显的S波低速层分布,该异常分布特征支持解释青藏高原隆升及其地壳物质运移的下地壳流模型.在100至120km深度上,川滇菱形块体西北部呈现较强的S波高速异常,这可能是印度岩石圈板块沿喜马拉雅东构造结下插至该区域所致,该区域下地壳的低速软弱物质与上地幔的高速强硬物质形成了鲜明对比,暗示了地壳和上地幔可能具有不同的构造运动和变形方式,这为该区域的壳幔动力学解耦提供了条件. 相似文献
4.
Zhongjie Zhang Yingkang Li Guangjie Wang Jiwen Teng S. Klemperer Jingwei Li Jinyi Fan Yun Chen 《中国科学D辑(英文版)》2002,45(6):550-558
We recognized 6 sets of reflecting P- and S-wave events from Moho and other interfaces within the crust, respectively, with
the wide-angle seismic data acquired from 510 km-long Selincuo-Ya’anduo profile in the northern Tibet, fitted the observed
events with forward modeling, and interpreted crustal structure of P- and S-wave velocities and Poisson’s ratio under the
profile. The results demonstrate that the crustal structure between Yarlungzangbo and Bangong-Nujiang sutures changes abruptly,
and the crust is the thickest at the middle part of the profile with thickness of 80 km or more. The “down-bowing” Moho is
the striking feature for the crustal variation along the west-east direction. The Moho uplifts with steps, and the uplifting
rate westward is greater than that eastward. The heterogeneity of P- and S-wave velocities exists both vertically and horizontally,
and one lower velocity layer (LVL) exists with the depth range of 27–34 km and the thickness range of 5–7 km. For the upper
crust, Poisson’s ratio is the lowest at the middle part of the profile; for the lower crust, the Poisson’s ratio at the east
segment is lower than that at west segment, which means that the crustal rigidity for the upper crust is different from the
lower crust, and the lower crust under the east segment of the profile is more ductile. We infer that the substance in the
lower crust endured eastward flow along with the collision between Eurasian and Indian plates, and the “down-bowing” Moho
is attributable to the multi-phase E-W tectonic processes. 相似文献
5.
In order to give a more reliable shallow crust model for the Chinese mainland, the present study collected many short-period surface wave data which are better sensitive to shallow earth structures. Different from traditional two-step surface wave tomography, we developed a new linearized surface wave dispersion inversion method to directly get a 3D S-wave velocity model in the second step instead of inverting for 1D S-velocity profile cell by cell. We convert all the regionalized dispersions into linear constraints for a 3D S-velocity model. Checkerboard tests show that this method can give reasonable results. The distribution of the middle-and upper-crust shear-wave velocity of the Chinese mainland in our model is strongly heterogeneous and related to different geotectonic terrains. Low-velocity anomalies delineated very well most of the major sedimentary basins of China. And the variation of velocities at different depths gives an indication of basement depth of the basins. The western Tethyan tectonic domain (on the west of the 95°E longitude) is characterized by low velocity, while the eastern Tethyan domain does not show obvious low velocity. Since petroleum resources often distribute in sedimentary basins where low-velocity anomaly appears, the low velocity anomalies in the western Tethyan domain may indicate a better petroleum prospect than in its eastern counterpart. Besides, low velocity anomaly in the western Tethyan domain and around the Xing’an orogenic belt may be partly caused by high crustal temperature. The weak low-velocity belt along ~105°E longitude corresponds to the N-S strong seismic belt of central China. 相似文献
6.
Using the P-and S-wave arrivals from the 150 earthquakes distributed in Tibetan Plateau and its neighboring areas, recorded
by Tibetan seismic network, Sichuan seismic network, WWSSN and the mobile network situated in Tibetan Plateau, we have obtained
the average P-and S-wave velocity models of the crust and upper mantle for this region:
The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, Supp., 573–579, 1992. 相似文献
| (1) | The crust of 70 km average thickness can be divided into two main layers: 16 km thick upper crust with P-wave velocity 5.55 km/s and S-wave velocity 3.25 km/s; and 54 km thick lower crust with P-wave velocity 6.52 km/s and S-wave velocity 3.76 km/s. |
| (2) | The p-wave velocity at the upper most mantle is 7.97 km/s, and the S-wave 4.55 km/s. The low velocity layer in the upper mantle occurs approximately at 140 km deep with a thickness of about 55–62 km. The prominent velocity gradient beneath the LVZ is comparable to the gradient above it. |
7.
Crust and uppermost mantle structure of the Ailaoshan-Red River fault from receiver function analysis 总被引：5，自引：1，他引：5
XU Mingjie WANG Liangshu LIU Jianhua ZHONG Kai LI Hua HU Dezhao XU Zhen 《中国科学D辑(英文版)》2006,49(10):1043-1052
S-wave velocity structure beneath the Ailaoshan-Red River fault was obtained from receiver functions by using teleseismic body wave records of broadband digital seismic stations. The average crustal thickness, Vp/Vs ratio and Poisson’s ratio were also estimated. The results indicate that the interface of crust and mantle beneath the Ailaoshan-Red River fault is not a sharp velocity discontinuity but a characteristic transition zone. The velocity increases relatively fast at the depth of Moho and then increases slowly in the uppermost mantle. The average crustal thickness across the fault is 36―37 km on the southwest side and 40―42 km on the northeast side, indicating that the fault cuts the crust. The relatively high Poisson’s ratio (0.26―0.28) of the crust implies a high content of mafic materials in the lower crust. Moreover, the lower crust with low velocity could be an ideal position for decoupling between the crust and upper mantle. 相似文献
8.
A total of 11 earthquakes with 15 Rayleigh wave paths, recorded at 11 broadband digital PASSCAL seismometers installed in
the Tibet Plateau by the Sino-U.S. joint research group, were used to determine the phase velocity and attenuation coefficient
of surface waves in periods of 10–130 s. The average shear wave velocity and quality factor {ie271-1} structures in the crust
and upper mantle were obtained in this region. The result shows the average {ie271-2} is low and there exists a high attenuation
({ie271-3}=93–141) layer in the crust. The depth range of the low {ie271-4} value layer (16–42 km) is consistent with the
range of low velocity layer (21–51 km) in the crust. Below 63 km in the lower crust, {ie271-5} decreases with depth from 114
to 34 at depth of 180 km. The low shear wave velocity and low value of {ie271-6} at the same depth range in the crust indicate
that the rocks in the range is probably melted or partially melted. According to the shear wave velocity structure, the average
thickness of the crust is about 71 km and a clear velocity discontiniuty appears at the depth of 51 km. The low-velocity zone
(4. 26 km/s) at depth of 96–180 km may be corresponding to the asthenosphere.
Contribution No. 96A0047, Institute of Geophysics, SSB, China.
This study was supported by the National Natural Science Foundation of China. 相似文献
9.
The phase velocities of Rayleigh waves and the lateral variation of lithospheric structure in Tibetan Plateau 总被引：1，自引：0，他引：1
According to a Sino-U. S. joint project, eleven broadband digital PASSCAL seismometers had been deployed inside the Tibetan
Plateau, of which 7 stations were on the profile from Lhasa to Golmud and other 4 stations situated at Maxin, Yushu, Xigatze
and Linzhi. Dispersions and phase velocities of the Rayleigh surface waves (10s–120s) were obtained on five paths distributed
in the different blocks of Tibetan Plateau. Inversions of the S-wave velocity structures in Songpan-Ganzi block, Qiang-Tang
block, Lhasa block and the faulted rift zone were obtained from the dispersion data. The results show that significant lateral
variation of the S-wave velocity structures among the different blocks exists. The path from Wenquan to Xigatze (abbreviated
as Wndo-Xiga) passes through the rift-zone of Yadong-Anduo. The phase velocities of Rayleigh waves from 10s to 100s on this
path are significantly higher than that on other paths. The calculated mean crustal velocity on this path is 3.8 km/s, much
greater than that on other paths, where mean crustal velocities of 3.4–3.5 km/s are usually observed. Low velocity zones with
different thicknesses and velocities are observed in the middle-lower crust for different paths. Songpan-Ganzi block, located
in the northern part of Tibetan Plateau is characterized by a thinner crust of 65 km thick and a prominent low velocity zone
in the upper mantle. The low velocity zone with a velocity of 4.2 km/s is located at a depth form 115 km to 175 km. While
in other blocks, no low velocity zone in the upper mantle is observed. The value of Sn in Songpan-Ganzi is calculated to be
4.5 km/s, while those in Qiang-Tang and Lhasa blocks are about 4.6 km/s.
The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,14, Supp., 566–573, 1992. 相似文献
10.
Crustal structure of seismic velocity in southern tibet and east-westward escape of the crustal material 总被引：11，自引：0，他引：11
The reflecting events from Moho and other interfaces within the crust are recognized from the wavefield characteristics of
P- and S-wave for the 480km long wide-angle seismic profile between Peigu Tso and Pumoyong Tso. Then, seismic crustal structures
of P- and S-wave velocities and Poisson ratio under the nearly east-west profile in southern Tibet are interpreted by fitting
the observed traveltimes with the calculated ones by forward modelling. Our interpreting results demonstrate that the crustal
thickness varies remarkably in the east-west direction, showing a pattern that the crust could be divided into three parts
bounded by the west of Dingri and the east of Dinggyê, respectively, where the depth of Moho is about 71km for the western
part, about 76km for the middle and about 74km for the eastern. There is one lower velocity layer (LVL) at the bottom of the
upper crust with depth of 20–30 km. One of the distinct features is that the thickness of LVL abruptly thins from 24km on
the west to 6km on the east. The other is that the velocity variation in the crust along east-west direction for both P- and
S-wave displays a feature as quasi-periodic variation. The lower velocity (compared to the average value for the continent
of the globe) in the lower crust and three sets of north-southward active normal faults are probably attributed to the coupling
process of material delamination in the lower crust, crustal thicking and east-westward escape of the crustal material accompanied
with the continental collision between India and Eurasia Plate. 相似文献
11.
A detailed dispersion analysis of Rayleigh waves generated by local earthquakes and occasionally by blasts that occurred in
southern Spain, was undertaken to obtain the shear-wave velocity structure of the region at shallow depth. Our database includes
seismograms generated by 35 seismic events that were recorded by 15 single-component short-period stations from 1990 to 1995.
All these events have focal depths less than 10 km and body-wave magnitudes between 3.0 and 4.0, and they were all recorded
at distances between 40 and 300 km from the epicentre. We analysed a total of 90 source-station Rayleigh-wave paths. The collected
data were processed by standard digital filtering techniques to obtain Rayleigh-wave group-velocity dispersion measurements.
The path-averaged group velocities vary from 1.12 to 2.25 km/s within the 1.0-6.0 s period interval. Then, using a stochastic
inversion approach we obtained 1-D shear-wave velocity–depth models across the study area, which were resolved to a depth
of circa 5 km. The inverted shear-wave velocities range approximately between 1.0 and 3.8 km/s with a standard deviation range
of 0.05–0.16 km/s, and show significant variations from region to region. These results were combined to produce 3-D images
via volumetric modelling and data visualization. We present images that show different shear velocity patterns for the Betic
Cordillera. Looking at the velocity distribution at various depths and at vertical sections, we discuss of the study area
in terms of subsurface structure and S-wave velocity distribution (low velocity channels, basement depth, etc.) at very shallow
depths (0–5 km). Our results characterize the region sufficiently and lead to a correlation of shear-wave velocity with the
different geological units features. 相似文献
12.
2008年5月12日在中国四川省境内龙门山断裂带发生了8级巨大地震．在其主震前后随着震源区附近应力状态的改变,地壳介质的物性是否也存在相应的异常变化过程？该问题成为汶川地震研究的热点科学问题之一．本研究搜集和整理了中国地震局四川数字地震台网2001年1月1日-2010年5月31日产出的震相观测报告,和中国地震局地球物理研究所流动数字地震台网2008年5月12日——9月30日产出的震相观测报告,采用多台和达法和多地震联合测定法,根据入选的直达波Pg和Sg的震相数据,重点研究了龙门山断裂及其附近地区的P波和S波视速度的时间变化特征,并与波速比的时间变化特征进行了对比分析．为保证计算结果的可靠性和稳定性,对所收集到的数据进行了较为严格的筛选和限定．研究发现,龙门山断裂及其附近地区,在汶川地震前P波和S波视速度存在4年左右的明显降低过程,到震前约半年出现快速恢复．在震前P波和S波的视速度明显降低的过程中,波速比的低值异常过程仅为2年多,且幅度小持续时间较短．在波速比和视速度异常发展的进程中,进入发震中短期异常快速恢复是两者的共同特征． 相似文献
13.
14.
根据流动数字地震台网提供的三分量地震波形记录资料,应用转换函数及快速模拟退火算法对腾冲－临沧地区30个地震台站下的地壳横波速度结构进行了反演.反演结果说明,研究区壳幔边界清晰、莫霍界面附近速度跳跃明显,由此得出该区地壳厚度在40 km左右、并具有从南向北增厚趋势.一个普遍的现象是,在腾冲-宝山地块下地壳存在明显的低速带,低速带的厚度在10～20 km间.研究结果进一步表明各台站下方上地幔速度结构复杂.这些结果为探讨青藏高原东南缘下地壳的侧向黏性流动、碰撞板块边界处壳幔物质交换等均提供了重要的地球物理证据,为探讨印-藏汇聚过程中青藏高原东构造结岩石圈变形、高原隆升及其深部动力学有一定理论意义. 相似文献
15.
ＪｕｄｇｅｍｅｎｔａｎｄｉｎｔｅｒｐｒｅｔａｔｉｏｎｏｆＳｗａｖｅｄａｔａｏｎｔｈｅＢｅｉｊｉｎｇＦｅｎｇｚｈｅｎＤＳＳｐｒｏｆｉｌｅＳＯＮＧＹＡＮＳＯＮＧ（宋松岩）ＸＵＥＳＯＮＧＺＨＯＵ（周雪松）ＸＩＡＮＫＡＮＧＺＨＡＮＧ（张先康）ＳＨ... 相似文献
16.
Surface wave dispersion is studied to obtain the 1-D average velocity structure of the crust in the Korean Peninsula by inverting
group- and phase-velocities jointly. Group velocities of short-period Rayleigh and Love waves are obtained from cross-correlations
of seismic noise. Multiple-filter analysis is used to extract the group velocities at periods between 0.5 and 20 s. Phase
velocities of Rayleigh waves in 10- and 50-s periods are obtained by applying the two-station method to teleseismic data.
Dispersion curves of all group and phase velocities are jointly inverted for the 1-D average model of the Korean Peninsula.
The resultant model from surface wave analysis can be used as an initial model for numerical modeling of observations of North
Korean events for a velocity model appropriated to the Korean Peninsula. The iterative process is focused especially on the
surface sedimentary layer in the numerical modeling. The final model, modified by numerical modeling from the initial model,
indicates that the crust shear wave velocity increases with depth from 2.16 km/s for a 2-km-thick surface sedimentary layer
to 3.79 km/s at a Moho depth of 33 km, and the upper mantle has a velocity of 4.70 km/s. 相似文献
17.
S-wave velocity and Poisson's ratio structure of crust in Yunnan and its implication 总被引：13，自引：2，他引：11
HU Jiafu SU Youjin ZHU Xiongguan & CHEN Yun Geophysical Department of Yunnan University Kunming China Seismological Bureau of Yunnan Province Kunming China Institute of Geology Geophysics Chinese Academy of Sciences Beijing China 《中国科学D辑(英文版)》2005,48(2):210-218
Receiver function of body wave under the 23 stations in Yunnan was extracted from 3-component broadband digital recording of teleseismic event. Thus, the S-wave velocity structure and distribution characteristics of Poisson's ratio in crust of Yunnan are obtained by inversion. The results show that the crustal thickness is gradually thinned from north to south. The crustal thickness in Zhongdian of northwest reaches as many as 62.0 km and the one in Jinghong of further south end is only 30.2 km. What should be especially noted is that there exists a Moho upheaval running in NS in the Chuxiong region and a Moho concave is generally parallel to it in Dongchuan. In addition, there exists an obvious transversal inhomogeneity for the S-wave velocity structure in upper mantle and crust in the Yunnan region. The low velocity layer exists not only in 10.0-15.0 km in upper crust in some regions, but also in 30.0-40.0 km in lower crust. Generally, the Poisson's ratio is on the high side, however it has a better co 相似文献
18.
The lithospheric structure of the Sinai Peninsula is shown by means of nine shear velocity profiles for depths ranging from
zero to 50 km, determined from the Rayleigh wave analysis. The traces of 30 earthquakes, which occurred from 1992 to 1999
in and around the study area, have been used to obtain Rayleigh wave dispersion. These earthquakes were registered by a broadband
station located in Egypt (KEG station). The dispersion curves were obtained for periods between 3 and 40 s, by digital filtering
with a combination of MFT and TVF filtering techniques. After that, all seismic events were grouped in source zones to obtain
a dispersion curve for each source-station path. These dispersion curves were inverted according to generalized inversion
theory, to obtain shear wave velocity models for each source-station path, which is the main goal of this study. The shear
velocity structure obtained for the Sinai Peninsula is shown through the shear velocity distributions with depth. These results
agree well with the geology and other geophysical results, previously obtained from seismic and gravity data. The obtained
velocity models suggest the existence of lateral and vertical heterogeneity. The shear velocity increases generally with depth
for all paths analyzed in the study area. Nevertheless, in some paths a small low velocity channel in the upper or lower crust
occurs. Along these profiles, it is found that the crustal structure of the Sinai Peninsula consists of three principal layers:
upper crust with a sedimentary layer and lower crust. The upper crust has a sedimentary cover of 2 km thick with an average
S-velocity of 2.53 km/s. This upper crust has a variable thickness ranging from 12 to 18 km, with S-wave velocity ranging
from 3.24 to 3.69 km/s. The Moho discontinuity is located at a depth of 30 km, which is reflected by a sharp increase in the
S-velocity values that jump from 3.70–4.12 to 4.33–4.61 km/s. 相似文献
19.
利用新疆和田地震台阵3 km孔径范围内架设的9个子台(包括1套宽频带和9套短周期地震仪)记录的3年远震波形数据,对比研究和分析了短周期地震仪接收函数的稳定性和可靠性.通过比较和分析短周期和长周期地震仪获取的接收函数波形,结果发现:(1)短周期地震仪记录与宽频带地震仪记录得到的接收函数有很好的一致性,且具有较高的稳定性,无论α取值为1.5还是2.5,短周期地震仪接收函数与宽频带地震仪接收函数都具有较强的线性相关性(相关系数0.9),但Ps震相均存在小幅的振幅差(约20%);(2)采用接收函数震相到时信息的方法(如H-κ叠加搜索),短周期地震仪可以代替宽频带地震仪;(3)由于短周期地震仪缺乏0.155 Hz以下的低频信号和在1 Hz以下频段非线性的振幅响应,仅仅采用短周期地震仪接收函数波形反演台站下方S波速度结构,获得下地壳到上地幔顶部的速度偏差较大(约0.3 km/s),可能会造成错误解释(如下地壳低速层),因此需要和其它对波速值敏感的数据(如面波频散)进行联合分析. 相似文献
20.
利用云南和中国地震台网30个台站记录的远震资料,采用接收函数扫描法和线性反演方法对云南及其邻区的壳幔速度结构进行了研究,获得了研究区内地壳厚度、Vp/Vs以及壳幔速度的分布特征.利用接收函数扫描（H-k）法和线性反演方法获取的台站下方地壳厚度结果表明,研究区地壳厚度变化剧烈.速度结构研究结果表明,红河断裂以西的腾冲-保山地块和思茅地块,以及南华板块北部地区的台站（如攀枝花、丽江、东川、永胜等）下方地壳均存在下地壳低速层,且具有高的地壳平均Vp/Vs值.这些不仅暗示研究区的下地壳低速异常可能为高温甚至高温导致的部分熔融所致,同时,也意味着该区下地壳的物质易于发生塑性流动,为地壳的变形和增厚创造了条件.红河断裂带作为云南地区的一个主要边界断裂,其西侧地区地壳厚度变化较东侧剧烈,另一方面,红河断裂西侧的平均地壳Vp/Vs值较其东侧要高.综合前人关于研究区岩石圈速度结构、地热流值、重力场和上地幔各向异性等地球物理场的研究结果.我们推断,现今的思茅块体和保山-腾冲块体在大地构造上应归属于冈瓦纳板块. 相似文献