共查询到20条相似文献，搜索用时 15 毫秒
1.
Susan A. Raikes 《Earth and Planetary Science Letters》1976,29(2):367-372
A study of teleseismic P-residuals for 13 stations in southern California reveals that these vary systematically with the azimuth of the event; the residuals generally tend to be negative in the NW and SE quadrants. This effect is greatest in the north of the region: a maximum peak-to-peak variation of 1.3 sec with residuals as low as ?0.9 sec was observed at Isabella. The delays become less negative further south in the region, and at the southernmost station, Glamis, delays of up to +0.75 sec were observed to the west. The latter may be associated with velocity decreases in the active geothermal areas of the Imperial Valley. A simple model, consisting of a region some 175 km wide and 100 km thick at a depth of approximately 100 km in which a velocity increase of up to 0.45 km/sec occurs, is proposed to account for the observed variations. This region trends NW-SE approximately parallel to the North America-Pacific plate boundary. The proposed velocity changes are consistent with a pinching out of the low-velocity (partial melting) zone under the area, such as has been proposed to explain the low heat flow in the Sierra Nevada, and may be related to the presence of an ancient (～ 30 m.y.) subduction zone under southern California. 相似文献
2.
The Barents Sea is underlain by a thick (up to 5 km) sedimentary basin. Seismic refraction has outlined four main velocity discontinuities which have been correlated with geological units on the basis of the geological history of the region. The basin is underlain by a crystalline basement, the nature of which cannot be determined on the basis of seismic velocity alone. Metamorphosed Paleozoic units (velocities around 5–4 km/sec) lie over this basement. Their thickness is not well established but appears to reach 1 or 2 km in some cases. A very distinct and thick (up to 2.5 km) layer (4.1 km/sec) is found almost everywhere and is thought to correspond to a major discontinuity at the end ot the Paleozoic. This discontinuity is followed by a variable velocity layer (2.4–4 km/sec, up to 1.2 km thick) which includes Mesozoic and Cenozoic sediments and is limited to the south of the Barents Sea. The absence of thick Tertiary deposits support the idea that the Barents shelf was emergent at that time. Recent low-velocity sediments are found close to the shelf edge.Gravity anomaly trends reflect a series of depressions of the 5.4-km/sec layer isobath map and suggest that the deeper part of the basin is made of a succession of faulted blocks or intense folds. 相似文献
3.
在我国西北地区的柴达木盆地东部和甘肃地区,在距离炮点40互100公里处,能够接收到不少能量较强的地壳深界面反射波。另外还发现一种与一般反射波性质不同的波,其视速度特大,视速度随距离的变化不大,而且有较明显的终点;其吋距曲线与一般深界面反射波的时距曲线相交。根据它的特征可以判断地壳中存在具有速度梯度的高速夹层.求得的夹层参数为: 甘肃地区柴达木盆地东部覆盖层厚度 18.8公里 30.5公里覆盖层平均速度 5.5公里/秒 5.3公里/秒夹层厚度 6.0公里 3.2公里夹层速度 7.5-8.5公里/秒 7.5-8.0公里/秒夹层的上下界面均为强反射面,可以产生多次反射波。分別利用相邻两个反射波可以求得各层参数,并能避免射线折射的影响。甘肃地区和柴达木盆地东部的地壳厚度分別为51和52公里。地壳中有高速夹层的存在,可以更好地说明P~*速度分散的原因,而且也能够解释Lg波的传播机制。 相似文献
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5.
ELIZABETH T. BUNCE 《Geophysical Prospecting》1969,17(1):28-35
Seismic refraction measurements were made in two areas of the Baltic Sea in June 1967. The refraction data were obtained in the course of the transmission measurements program of Operation MILOC BALTIC 67. Three profile pairs were obtained, two in the area south of Öland Island, Sweden, the third to the east, north of the peninsula of Hel, Poland. The water depths vary from 60 to 90 meters between the areas. The receiving positions for the two profiles south of Oland Island are only 46 km apart but the structures differ markedly. The northern section, only 500 m thick, shows a rather thin sedimentary cover above 350 m of 3.7 km/sec material that in turn overlies 5.6 - 5.9 km/sec velocity material. The southern section, almost 2 km thick, has an equivalent amount of low velocity material, and a layer about 1 km thick having velocity 4.8 km/sec that overlies 6.0 km/sec velocity material. The eastern profile shows high velocity material, 5.6 km/sec, at 2.5 km depth. Correlation of the layers determined by seismic refraction with nearby geology suggests that the structural change south of Öland Island may represent the boundary of the Sarmatian Shield in this region. 相似文献
6.
By using the teleseismic receiver function method, this paper analyzes the crustal thickness and v_P/v_S ratios beneath the 4 National seismic stations (KMI, TNC, CD2 and PZH) in the Sichuan-Yunnan area. This study gives the variance of Moho depths and velocity ratios of the 4 stations in different directions. The results show that the Moho depth beneath the Kunming station is around 50km, and the velocity ratio varies between 1.62 and 1.69. The thickness of crust and the velocity ratio do not change much with the direction. The crust beneath Tengchong station shows clear directivity, being 40.7km thick in the northeast and 49.7km thick in the southeast. The difference of the v_P/v_S values is remarkable between the two directions, reaching 0.2. The Chengdu station also has shallow Moho, about 40km, but is 8km deeper in the northeast and southwest and the velocity ratio has a change of 0.13 between the two directions. The crust beneath the Panzhihua station is stable. In all directions, the Moho depth is around 60km and the v_P/v_S ratio doesn't change significantly. 相似文献
7.
Prantik Mandal R. K. Chadha N. Kumar I. P. Raju C. Satyamurty 《Pure and Applied Geophysics》2007,164(10):1963-1983
During the last six years, National Geophysical Research Institute, Hyderabad has established a semi-permanent seismological
network of 5–8 broadband seismographs and 10–20 accelerographs in the Kachchh seismic zone, Gujarat with a prime objective
to monitor the continued aftershock activity of the 2001 Mw 7.7 Bhuj mainshock. The reliable and accurate broadband data for the 8 October Mw 7.6 2005 Kashmir earthquake and its aftershocks from this network as well as Hyderabad Geoscope station enabled us to estimate
the group velocity dispersion characteristics and one-dimensional regional shear velocity structure of the Peninsular India.
Firstly, we measure Rayleigh-and Love-wave group velocity dispersion curves in the period range of 8 to 35 sec and invert
these curves to estimate the crustal and upper mantle structure below the western part of Peninsular India. Our best model
suggests a two-layered crust: The upper crust is 13.8 km thick with a shear velocity (Vs) of 3.2 km/s; the corresponding values
for the lower crust are 24.9 km and 3.7 km/sec. The shear velocity for the upper mantle is found to be 4.65 km/sec. Based
on this structure, we perform a moment tensor (MT) inversion of the bandpass (0.05–0.02 Hz) filtered seismograms of the Kashmir
earthquake. The best fit is obtained for a source located at a depth of 30 km, with a seismic moment, Mo, of 1.6 × 1027 dyne-cm, and a focal mechanism with strike 19.5°, dip 42°, and rake 167°. The long-period magnitude (MA ~ Mw) of this earthquake is estimated to be 7.31. An analysis of well-developed sPn and sSn regional crustal phases from the bandpassed
(0.02–0.25 Hz) seismograms of this earthquake at four stations in Kachchh suggests a focal depth of 30.8 km. 相似文献
8.
利用2005年1月1日~2008年1月1日紫坪铺台网及YZP台连续波形资料,通过噪声互相关技术研究了紫坪铺水库区域在蓄水、泄水过程中库区介质的变化特征,同时对可能的渗透过程进行了讨论。使用移动窗口互谱方法计算库区台站对之间的相对波速变化。结果表明,在紫坪铺水库的3次大规模蓄水及2次泄水过程中,地下介质相对波速变化与水位变化之间存在较为明显的相关性,并在时间上有一定延迟,可能与水的渗透有关。分析认为蓄水对浅层介质产生的作用最快,影响最大,波速的变化是蓄水产生的压力及渗透共同作用的结果。在第1次蓄水时,压力起主要作用,后2次蓄水时,渗透起主要作用,且渗透作用已影响至8km左右的断层。 相似文献
9.
Tuneto Kurita 《Physics of the Earth and Planetary Interiors》1974,8(2):177-201
The upper-mantle structure down to about 220 km in the central United States has been inferred from long-period P- and S-wave spectra of deep earthquakes recorded at three WWSSN stations, by using the re-formulated transfer ratio method. This method has been experimentally shown to be a very powerful means for elucidating the fine configuration of the low-velocity zone. The strong advantage of this method is its ability to determine separately the extent of the velocity decrease and the depth to the bottom of this zone, which is more uncertain by the other methods.From the Interior Plain to the Gulf of Mexico the low-velocity zone shifts to a shallower depth while increasing its thickness and decreasing its velocities. This zone is made up of an approx. 50 km thick layer ranging in depth from about 150 to 200 km under the Interior Plain, an approx. 75 km thick layer from about 120 to 195 km under the Gulf Coastal Plain, and an approx. 80 km thick layer from about 95 to 175 km under the continental shelf of the Gulf of Mexico, all nearly along 89°N longitude. The decrease in S-wave velocity at the top of this zone is about 0.30, 0.45, and 0.70 km/sec under each of the above areas, although the last value may be somewhat an overestimate. Both boundaries of this zone are sharp, the transition occurring over at most ca. 10 km. In this region the existence of the high-velocity lid zone is possible. 相似文献
10.
Prantik Mandal R. K. Chadha N. Kumar I. P. Raju C. Satyamurty 《Pure and Applied Geophysics》2007,164(11):2235-2254
During the last six years, the National Geophysical Research Institute, Hyderabad has established a semi-permanent seismological
network of 5 broadband seismographs and 10 accelerographs in the Kachchh seismic zone, Gujarat, with the prime objective to
monitor the continued aftershock activity of the 2001 Mw7.7 Bhuj mainshock. The reliable and accurate broadband data for the Mw 7.6 (8 Oct., 2005) Kashmir earthquake and its aftershocks from this network, as well as from the Hyderabad Geoscope station,
enabled us to estimate the group velocity dispersion characteristics and the one-dimensional regional shear-velocity structure
of peninsular India. Firstly, we measure Rayleigh- and Love-wave group velocity dispersion curves in the range of 8 to 35
sec and invert these curves to estimate the crustal and upper mantle structure below the western part of peninsular India.
Our best model suggests a two-layered crust: The upper crust is 13.8-km thick with a shear velocity (Vs) of 3.2 km/s; the
corresponding values for the lower crust are 24.9 km and 3.7 km/sec. The shear velocity for the upper mantle is found to be
4.65 km/sec. Based on this structure, we perform a moment tensor (MT) inversion of the bandpass (0.05–0.02 Hz) filtered seismograms
of the Kashmir earthquake. The best fit is obtained for a source located at a depth of 30 km, with a seismic moment, Mo, of
1.6 × 1027 dyne-cm, and a focal mechanism with strike 19.5°, dip 42°, and rake 167°. The long-period magnitude (MA ~ Mw) of this earthquake is estimated to be 7.31. An analysis of well-developed sPn and sSn regional crustal phases from the bandpassed
(0.02–0.25 Hz) seismograms of this earthquake at four stations in Kachchh suggests a focal depth of 30.8 km. 相似文献
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本文对用爆炸地震资料研究地壳与上地幔结构及速度分布的τ法反演进行了探讨,并且在Bessonova提出的平均值方法的基础上,就减少解的不确定性及简化反演过程提出了新的作法:1.τ（p）的上下界各自独立地参与反演而后再将所得到的结果合并起来;2.在τ法反演中,抽去地壳模型中的低速层。根据以上两种计算方案,改进方法,取得较好的效果。 本文还用Bessonova的平均值方法计算了我国东部地区地壳-上地幔爆炸地震探测剖面的实例。该地区地壳厚度约为31 km,在18 km深处存在着低速层,厚度约6 km,速度为6 km/s。 相似文献
13.
利用2010年布设在西藏南迦巴瓦构造结的郎嘎、崩嘎、直白和拉格四个宽频地震台所观测到的近5个月的地震记录,采用时间域迭代反褶积技术处理得到接收函数,通过筛选多条相近震中距和反方位角的高质量接收函数求取其叠加平均.对大地电磁数据做Rhoplus分析处理得到视电阻率和相位曲线.利用单台接收函数和相同位置的大地电磁视电阻率和相位联合反演地下一维壳幔结构.联合反演采用遗传算法,并通过权衡图分析大地电磁和地震数据的兼容性.理论值和实测值的对比显示两种数据能同时得到较好拟合.联合反演结果表明:(1)中上地壳为9 km至14 km厚的高阻高速层覆盖于低阻低速层之上的结构,中地壳低阻低速层可能与深部流体和局部熔融共同作用有关.(2)下地壳存在最厚达20 km的高导的壳幔过渡层,波速在4 km/s左右;上地幔约130 km至150 km以下存在软流圈.(3)上地壳的高阻高速层解释为多雄拉组混合岩化角闪岩相变质岩,而直白台所显示的低阻低速层与高压麻粒岩的少量部分熔融有关,可能源于壳幔过渡带镁铁质岩石的相变或更深处幔源岩浆底侵作用的产物. 相似文献
14.
TheP-arrival times of local and regional earthquakes that are outside of a small network of seismometers can be used to interpret crustal parameters beneath the network by employing the time-term technique. Even when the estimate of the refractor velocity is poorly determined, useful estimates of the station time-terms can be made. The method is applied to a 20 km diameter network of eight seismic stations which was operated near Castaic, California, during the winter of 1972–73. The stations were located in sedimentary basins. Beneath the network, the sedimentary rocks of the basins are known to range from 1 to more than 4 km in thickness. Relative time-terms are estimated fromP-waves assumed to be propagated by a refractor in the mid-crust, and again fromP-waves propagated by a refractor in the upper basement. For the range of velocities reported by others, the two sets of time-terms are very similar. They suggest that both refractors dip to the southwest, and the geology also indicates that the basement dips in this direction. In addition, theP-wave velocity estimated for the refractor of mid-crustal depths, roughly 6.7 km/sec, agrees with values reported by others. Thus, even in this region of complicated geologic structure, the method appears to give realistic results. 相似文献
15.
QU Jun-hao WANG Chang-zai LIU Fang-bin ZHOU Shao-hui ZHENG Jian-chang LI Xin-feng ZHANG Qin 《地震地质》2019,41(1):99-118
Since the earthquake of ML3.8 occurring on October 1, 2013 in Ruishan, Weihai City, Shandong Province, the sequence has lasted for about 4 years(Aug. 31, 2017). Seismicity is enhanced or weakened and fluctuated continuously. More than 13250 aftershocks have been recorded in Shandong Seismic Network. During this period, the significant earthquake events were magnitude 4.2(ML4.7)on January 7, 4.0(ML4.5)on April 4, M3.6(ML 4.1)on September 16 in 2014 and M4.6(ML5.0)on May 22, 2015. The earthquake of ML5.0 was the largest one in the Rushan sequence so far. In order to strengthen the monitoring of aftershocks, 18 temporary stations were set up near the epicenter at the end of April, 2014(official recording began on May 7)by Shandong Earthquake Agency, which constitutes an intensified network in Rushan that surrounds the four quadrants of the small earthquake concentration area together with 12 fixed stations nearby, and provides an effective data foundation for the refinement of Rushan earthquake sequence.
The velocity structure offers important information related to earthquake location and the focal medium, providing an important basis for understanding the background and mechanism of the earthquake. In this paper, double-difference tomography method is used to relocate the seismic events recorded by more than six stations of Rushan array from May 7, 2014 to December 31, 2016, and the inversion on the P-wave velocity structure of the focal area is conducted. The Hyposat positioning method is used to relocate the absolute position. Only the stations with the first wave arrival time less than 0.1 second are involved in the location. A total of 14165 seismic records are obtained, which is much larger than that recorded by Shandong Seismic Network during the same period with 7708 earthquakes and 2048 localizable ones. A total of 1410 earthquakes with ML ≥ 1.0 were selected to participate in the inversion. Precise relocation of 1376 earthquakes is obtained by using double-difference tomography, in which, there are 14318 absolute traveltime P waves and 63162 relative travel time P waves. The epicenters are located in distribution along NWW-SEE toward SEE and tend to WS, forming a seismic belt with the length about 3km and width about 1km. The focal depths are mainly concentrated between 4km and 9km, occurring mainly at the edge of the high velocity body, and gradually dispersing with time. It has obvious temporal and spatial cluster characteristics. Compared with the precise relocation of Shandong network, the accuracy of the positioning of Rushan array is higher. The main reason is that the epicenter of Rushan earthquake swarm is near the seaside, and the fixed stations of Shandong Seismic Network are located on the one side of the epicenter. The nearest three stations(RSH, HAY, WED)from the epicenter are Rushan station with epicentral distance about 13km, the Haiyang station with epicentral distance about 33km, and Wendeng station with epicentral distance about 42km. The epicentral distance of the rest stations are more than 75km. In addition, the magnitude of most earthquakes in Rushan sequence is small. The accuracy of phase identification is relatively limited due to the slightly larger epicentral distance of the station HAY and station WED in Shandong Seismic Network. Furthermore, the one-dimensional velocity model used in network location is simple with only the depth and velocity of Moho surface and Conrad surface. The epicentral distances of the 18 temporary stations in Rushan are less than 10km, and the initial phase is clear. The island station set up on the southeast side and the Haiyangsuo station on the southwest side form a comprehensive package for the epicenter. Compared with the double-difference algorithm method, the double-difference tomography method used in this paper is more accurate for the velocity structure, thus can obtain the optimal relocation result and velocity structure.
the velocity structure shows that there are three distinct regions with different velocities in the vicinity of the focal area. The earthquakes mainly occur in the intersection of the three regions and on the side of the high velocity body. With the increase of depth, P wave velocity increases gradually and there are two distinct velocity changes. The aftershock activities basically occur near the dividing line to the high velocity side. The south side is low velocity abnormal body and the north side is high velocity abnormal body. High velocity body becomes shallower from south to north, which coincides with the tectonic conditions of Rushan. Considering the spatial relationships between the epicenter distribution and the high-low velocity body and different lithology of geological structure, and other factors, it is inferred that the location of the epicenter should be the boundary of two different rock bodies, and there may be a hidden fault in the transition zone between high velocity abnormal body and low velocity abnormal body. The interface position of the high-low velocity body, the concentrating area of the aftershocks, is often the stress concentration zone, the medium is relatively weak, and the intensity is low. There is almost no earthquake in the high velocity abnormal body, and the energy accumulated in the high velocity body is released at the peripheral positions. It can be seen that the existence of the high-low velocity body has a certain control effect on the distribution of the aftershocks. 相似文献
16.
在沙城以东的延庆盆地及其邻近区域内布设了由GDS－1000宽频带数字地震仪组成的流动地震台阵，利用台阵记录的宽频带远震P波波形数据和非线性接收函数反演方法获得了延怀盆地内0-80km深度范围的地壳、上地幔S波速度结构．利用计算机三维彩色剖分显示技术研究了台阵下地壳、上地幔速度结构的横向非均匀变化。结果表明，研究区域内的地壳厚度为40km左右，壳幔界面有4km左右的上下起伏．地表沉积盖层在延庆盆地中心附近厚度约1km，而在向盆地外围延伸的方向上相对变薄．研究区域内上地壳S波速度结构较复杂，而下地壳与上地幔则相对比较均匀．其上地壳最突出的特点是在10km深度附近有明显的S波低速层．在延庆盆地下方，它延伸到6-20km的深度范围．在延庆盆地南侧，该低速层有从西往东逐渐减弱的趋势．研究区域内的地震基本上都发生在延庆盆地下方上地壳低速体外围．据此推断，延庆盆地及其临近区域内的地震活动与该区域地壳内的热状态有密切关系． 相似文献
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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
18.
珠江口地区位于南海北部大陆的边缘,具有洋陆过渡型地壳特征,且NE向滨海断裂带从其中穿过,强震风险不可忽视。文中基于2015年珠江口海陆联合三维人工地震探测数据,人工进行初至P波震相拾取,并使用VELEST程序分别反演了陆域和海域的最小一维P波速度模型(走时残差均方根最小)和台站校正结果。台站校正结果的空间分布与区域地形、地质构造和沉积厚度相关较好,正值多分布在珠江三角洲沉积盆地和珠江口盆地内,而负值多分布在花岗岩等基岩出露地区以及滨海断裂带北侧和北部断阶带内的部分隆起地区。新模型对人工地震走时的拟合精度较高,陆域走时残差均方根为0.07s,海域为0.21s。与华南模型相比,新模型对区域地震定位的效果更好,重定位后,陆域的P波地震走时残差降低了22.6%、S波降低了21.2%;海域的P波地震走时残差降低了25.7%、S波降低了15.6%。新模型可为区域地震定位、地震参数和三维成像研究提供参考。 相似文献
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20.
利用接收函数方法研究四川地区地壳结构 总被引：3，自引：0，他引：3
采用接收函数反演和共转换点(CCP)偏移叠加成像方法, 利用四川数字地震台网宽频带的52个区域固定地震台站和布设的两条52个宽频带流动地震观测台站的远震地震波形数据资料, 对四川地区地壳结构进行研究。 结果表明, 四川地区的Moho面深度在青藏高原和四川盆地差异明显, 在川西高原地区地壳厚度为52~68 km, 在川滇地块地壳厚度为50~60 km, 在中地壳内存在不连续的低速层分布; 而在四川盆地地壳厚度为38~45 km, 地壳内没有低速层存在。 Moho面深度从川西高原的60多公里至四川盆地的约40 km, 在二者的交界处龙门山断裂带下面, 存在厚度约30 km左右宽的下降过渡带, 说明其下的Moho面可能受断层影响, 结构比较复杂; 在高原地区的上地壳界面和下地壳上界面比四川盆地的相应界面深; 高原地区在中地壳的上部有不连续的低速层分布, 在松潘—甘孜地块的上地壳下部存在向南东运动的脆性推覆体, 在羌塘—理塘地块的上地壳下部存在向南东和南运动的脆性物质流动。 相似文献