华北地区地壳P波三维速度结构

1968年邢台地震以后的30余年中, 中国地震局系统先后在大华北地区布置30余条、近20000km的人工地震宽角反射/折射深地震测深(DSS) 剖面, 用以研究地壳及上地幔顶部的速度结构, 取得了大量研究成果.但以往的研究明显的不足是未能形成华北区域性的地壳三维速度结构模型, 从大区域的角度为研究华北地区地壳深部构造特征提供地震学方面的依据.因此, 在现已发表的DSS剖面资料的基础上, 选择了14条测线的资料, 利用地理信息系统(ARC/INFO) 的“矢量化”功能, 以及克里格数据网格化技术构建华北区域性的地壳三维速度结构模型, 从而对华北研究区内地壳三维速度结构的特点得到如下认识: (1) 华北地区地壳表层P波速度变化幅度大, 平面结构较复杂, 大体上划分为相间排列、走向趋势以北西向为主的3个速度区.海河平原和渤海湾的低速带是研究区范围内速度最低的低速区.资料的情况说明, 研究区内沉积盖层的地质构造与上地壳构造之间虽有一定继承性, 但也存在较大差别. (2) 总体上看, 在华北研究区内地壳的P波速度随深度增大而增大, 但局部地区出现速度倒转的现象, 东区的海河平原低速异常逐渐消失, 而西区的山西地堑则以相对低速异常特征为主.区内地壳以太行山脉为界, 划分为东、西两区; 东部和西部, 结晶基底以上地层的构造方向不完全一致; 东部的黄淮海地块, 区域构造以北东向为主, 而西部包括山西地块和鄂尔多斯地块东缘, 其构造方向则以北西向为主. (3) 根据莫霍面的形态特征, 研究区地壳可大致划分为6个区块; 在山西地块范围内, 莫霍面呈近南北向的凹陷带, 地壳厚度大; 内蒙古地块南缘和燕山地块南部, 莫霍面表现出褶皱带的构造特征, 其延展趋势为近东西方向; 鄂尔多斯地块东缘, 莫霍面构造相对复杂, 呈近北西向凸、凹相伴的褶皱; 黄淮海地块(华北裂谷带中、北部) 为莫霍面隆坳区, 隆、坳相间排列, 构造较复杂, 但从整体上看, 这是全区莫霍面最浅的隆起区段; 鲁西台背斜主要为莫霍面断陷区, 其断陷带沿枣庄—曲阜一线向北西方向延伸.      

苏鲁—大别超高压变质带地壳速度结构及其俯冲、折返机制

三维P波速度解析研究结果表明，苏鲁-大别超高压变质带岩石圈地壳速度结构均具有上地壳明显高速且上凸、中地壳增厚、下地壳埋藏较深且莫霍面下凹等基本特征。与大别地区相比较，苏鲁超高压变质带存在着上地壳波速更高，且地表高速区面积与上地壳高速体体积大于大别；而莫霍面下凹程度不如大别地区，地壳山根已逐步趋向消失等独特的区域特征。显示了苏鲁地区曾发生过更激烈的俯冲与折返构造运动，与大别地区相比，有更多高速、高密度的超高压变质岩折返到上地壳与地表；然而在造山运动过程中比大别更早进入了造山运动后期等特征。对比研究结果表明，苏鲁-大别地段的造山、演化过程中，在构造运动基本相似的背景下，存在着区域性特征。苏鲁地区的造山运动以及超高压变质作用，有起始略晚、发生时期较短但相对激烈、结束早、比大别更早进入了造山运动的后期等特征。笔者分析了苏鲁区域性特征形成的主要构造原因是，郯庐断裂带的大规模左旋走滑运动以及通过中国华北区域的大范围NXV—SE向扩张应力场的影响。其中，中生代以来大华北地区的大区域扩张应力场的影响可能是该区俯冲到地幔内的超高压变质岩能够大量折返回地表或上地壳的重要构造原因。     

The lithosphere structure of Northeast China

The lithosphere of northeastern China is composed of the Erguna, Xingan, Songnen, Jiamusi blocks and Mesozoic Wandashan accretionary complex from west to east. Nd isotope model ages indicate that the Xingan and Songnen blocks have the same Nd model ages ranging from 500 to 1 000 Ma. These are obviously younger than those of the Jiamusi block (1 500–2 000 Ma) and the Erguna block (1 500–1 700 Ma), reflecting the different evolutions of individual blocks in the early times. Geochemical tracing analysis shows that the Nd model ages of Paleozoic supercrustal rocks in the four blocks are dominantly Mesoproterozoic, while those of Mesozoic granites are mainly Neoproterozoic. It is shown that the crust ages of the region are characterized by being younger in the lower part and older in the upper part. The Os isotope analysis also indicates that the lithosphere mantle of the region is characteristic of a younger age. The P-wave velocities of the region show more complicated structures in lithosphere and asthenosphere. First of all, notably different from traditional concept of the seismic lithosphere, the low velocity zone of the lithosphere beneath the region has no persistent and continuous top interface which is highly varied in depth and intersected with the high velocity layers, forming sharp velocity discontinuities beneath major tectonic belts, even up to the Moho beneath some tectonic units. But the bottom interface of the low velocity zone is relatively persistent, occurring at a depth of 230–240 km. Another feature is that the lithosphere is characterized by an “overpass type” velocity structure vertically, in which the contoured velocity is distributed in the NE trending within the crust, in a nearly NS trending in the lithosphere mantle from a depth of 45 to 90 km, in a nearly EW trending in the upper part of the asthenosphere from 90 to 170 km and in a ring-like distribution with a diameter of about 300 km in the lower part of the asthenosphere from 170 to 240 km. The P-wave velocity is progressively increasing from 240 to 400 km.     

3–D Tomographic Images and Deep Ore-Control in Northern Margin of the North China Plate

Abstract: 3–D velocity images of the crust beneath the northern margin of the North China Plate have been constructed using P-wave travel time residuals of the latest earthquakes, with the data supplied by Chinese seismic networks.
The seismic image results indicate that there is a lateral heterogeneity in the crust beneath the northern part of the North China block. The velocity images of the upper crust show features closely related to the tectonic features on the surface. It can be seen from these velocity images of the vertical sections, and from the horizontal slice images at depths of 11 and 16 km that there exist East-West and North-East structures. The images indicate that the juncture zone of basin–and–range terrain is between the blue-colored high–velocity block corresponding to the Yanshan mountain range that developed during the Yanshan period in northwest Beijing and the green low-velocity area corresponding to the North China basin in southeast Beijing (Fig. 5). The juncture zone between high-velocity and low–velocity, and EW and NE fault zones have significant ore-control effects. From the chart of epicenters in the northern region of North China, we find that the epicenters of earthquakes are almost entirely distributed within the NE strip. Almost all major earthquakes took place in the transition strip between the high and low-velocity zones in the crust. The distribution of epicenters also reflects the strikes of known NE–faults. From the image sections along the latitude, we find that in the area between 114.0 E –118.0 E , there is a blue high-velocity block standing upright from the Moho to the upper crust (Fig. 6), from which can be deduced that some materials such as magma moved upward from the upper mantle during the history of its geological development.     

Crustal structure in Tengchong Volcano-Geothermal Area, western Yunnan, China

Based upon the deep seismic sounding profiles carried out in the Tengchong Volcano-Geothermal Area (TVGA), western Yunnan Province of China, a 2-D crustal P velocity structure is obtained by use of finite-difference inversion and forward travel-time fitting method. The crustal model shows that a low-velocity anomaly zone exists in the upper crust, which is related to geothermal activity. Two faults, the Longling–Ruili Fault and Tengchong Fault, on the profile extend from surface to the lower crust and the Tengchong Fault likely penetrates the Moho. Moreover, based on teleseismic receiver functions on a temporary seismic network, S-wave velocity structures beneath the geothermal field show low S-wave velocity in the upper crust. From results of geophysical survey, the crust of TVGA is characterized by low P-wave and S-wave velocities, low resistivity, high heat-flow value and low Q. The upper mantle P-wave velocity is also low. This suggests presence of magma in the crust derived from the upper mantle. The low-velocity anomaly in upper crust may be related to the magma differentiation. The Tengchong volcanic area is located on the northeast edge of the Indian–Eurasian plate collision zone, away from the eastern boundary of the Indian plate by about 450 km. Based on the results of this paper and related studies, the Tengchong volcanoes can be classified as plate boundary volcanoes.     

The Crustal Structure and Seismic Activity in North China

A layered crustal block model of North China has been constructed based on large amount of data from seismic sounding carried out in recent two decades. Some deep fault zones, such as the Zhangjiakou.Penglai and Tancheng-Lujiang fault zones, divide the upper crust of North China into three upper crustal terranes and nine bolcks. There are distinct differences in velocity and depth distributions, which reflects Cenozoic block faulting in North China in the process of formation of the deep structure. The upper crust shows the features of transition in isostatic adjustment. The existence of a low-velocity layer in the middle crust is characteristic of the crustal structure in North China. There seems to be an increase of rheology of the rocks in the lower crust and a persistence of stable regional stress field. The patterns of the Moho on two sides of the Yanshan-Taihang Mountains are different. The relief of the Moho around Beijing, Shijiazhuang and Guangrao where the deep faults join together shows a quadrantal distribution in some degree. The dynamic sources for seismic activity are the NE-SW horizontal compression and the diapirism of the upper mantle. The middle and upper crust, especially the layered block structure has the most significant effects on seismicity, and the occurrence of earthquakes is more closely related to them than to the Moho.     

鄂尔多斯盆地西缘煤田构造演化及其控制因素

鄂尔多斯盆地西缘位于华北陆块和秦祁昆山造山带两个一级大地构造单元之间的过渡带内,特定的大地构造背景使其具有复杂的构造演化历程及特殊的煤田构造格局。鄂尔多斯盆地西缘由贺兰山逆冲推覆构造系统和六盘山东麓逆冲推覆构造系统组成,具有"南北分段、东西分带"的特点。为了进一步探讨鄂尔多斯盆地西缘煤田构造格局的形成演化及区域构造控制因素,本文基于野外地质调查和煤田勘查资料,恢复了本区自晚古生代以来的沉降抬升史和古构造应力场特征。印支期:研究区北部最大主压应力方向为北西-南东向,南部最大主压应力方向为北东-南西向;燕山期:北部最大主压应力方向为北西西-南东东向,南部最大主压应力方向为北东东-南西西向;喜马拉雅山期:北部受北西西-南东东向拉张应力,南部最大主压应力方向为北东-南西向。采用有限元数值模拟,探讨了鄂尔多斯盆地西缘煤田构造格局的形成与区域构造的演化的关系,强调北段贺兰山逆冲推覆构造系统的形成与阿拉善地块的向东挤出逃逸密切相关。     

银川盆地构造发展——深地震反射剖面揭示浅部地质与深部构造的联系

横跨银川盆地北西西向的深地震反射剖面,清晰揭示了银川盆地边界断裂以及整个地壳的结构构造特征,这对研究具活动大陆裂谷性质的银川盆地浅-深构造关系具有重大的意义。贺兰山东麓山前断裂、黄河断裂作为银川盆地的西、东边界断裂,前者为一条缓倾斜、延伸至上、下地壳边界的犁式断裂,而后者则为一条切穿地壳并延伸进入上地幔的深大断裂。根据深地震反射剖面揭示的地壳结构特征,银川盆地浅部结构并非前人认为的"堑中堑"结构,而是表现为由一系列东倾犁式正断层控制的新生代断陷。略微下凹的Moho面几何形态以及厚2~3.2 km的层状强反射带为下地壳最显著的反射特征。Moho面深度与强反射带厚度变化趋势与银川盆地沉积厚度变化趋势几乎一致。本文认为,强反射带的成因可能是由源自地幔的基性岩浆以岩席状的形式底侵进入地壳底部造成的,而这部分形成强反射带的物质可能补偿了因银川盆地断陷而造成的地壳减薄,最终导致银川盆地之下Moho面并未像之前所认为的那样隆起。     

南北构造带天水、武都强震区地壳和上地幔顶部结构

利用两条相互垂直的高分辨地震折射/宽角反射剖面和相应的非纵观测的多个扇形剖面取得的人工地震资料, 研究天水和武都8级大震区的地壳和上地幔顶部结构和构造.二维剖面结果显示, 地壳沿垂向可分为上地壳和下地壳两大层.上地壳中部存在低速层, 层内介质速度比背景值低0.3~0.5km/s.莫霍面深度大约为46~48km.NE向的天水-武都剖面下地壳速度在横向上变化剧烈, NW向的成县-武山剖面, 在礼县以西, Moho面和C界面有被上涌物质改造过的迹象.三维速度成像显示, 在105°E附近, 从7至11km的深度范围内, 存在一条近NS向的断裂带, 在该带的两侧速度结构有明显的差异, 西侧为低速异常, 而东侧为高速异常, 这一近NS向的断裂带与二维剖面的下地壳深断裂在位置上很接近.该地区的几个8级大震均发生在105°E附近, 并且呈一近NS条带.      

Early Mesozoic basin development in North China: Indications of cratonic deformation

We integrated a systematic sedimentary data into a regional Early Mesozoic stratigraphic framework which demonstrated a detailed picture of spatiotemporal variations in basin deposition and formation in the North China Craton. The Early Mesozoic basin sedimentary evolution is utilized to interpret polyphase tectonism and to unravel the craton deformation. The Late Triassic, nearly WNW-trending, giant intracratonic Ordos basin was widely distributed across most of North China Craton, with a southern wedge-top depozone along the northern East Qilian–Qinling orogenic belt and a northwestern rift depozone along the Helanshan. The continuous subsidence and deposition within the basin were dominantly related to the thrust load of the East Qilian–Qinling belt and inferred mantle flow effects associated with paleotethys plate subduction, and the rift in the northwestern Ordos was driven by nearly north-vergent compression of the eastern North Qilian–North Qinling active margins with the stable North China Craton. This intracratonic Ordos basin formation initiated the deformation of the North China Craton. Formation of the Jurassic NNE-trending walled intracratonic Ordos basin and the broken flexural basins indicates the North China Craton underwent the second, even more abroad nearly NNE trending crustal deformation, with lithosphere thickening in the eastern part of the North China Craton, and dynamic subsidence in the west, which may have been driven by nearly northwestward subduction of the Izanagi plate and the eastward extrusion and underthrusting of the western North China Craton crustal basement.     

Crustal structure of the northeastern margin of the Tibetan plateau from the Songpan-Ganzi terrane to the Ordos basin

The 1000-km-long Darlag–Lanzhou–Jingbian seismic refraction profile is located in the NE margin of the Tibetan plateau. This profile crosses the northern Songpan-Ganzi terrane, the Qinling-Qilian fold system, the Haiyuan arcuate tectonic region, and the stable Ordos basin. The P-wave and S-wave velocity structure and Poisson's ratios reveal many significant characteristics in the profile. The crustal thickness increases from northeast to southwest. The average crustal thickness observed increases from 42 km in the Ordos basin to 63 km in the Songpan-Ganzi terrane. The crust becomes obviously thicker south of the Haiyuan fault and beneath the West-Qinlin Shan. The crustal velocities have significant variations along the profile. The average P-wave velocities for the crystalline crust vary between 6.3 and 6.4 km/s. Beneath the Songpan-Ganzi terrane, West-Qinling Shan, and Haiyuan arcuate tectonic region P-wave velocities of 6.3 km/s are 0.15 km/s lower than the worldwide average of 6.45 km/s. North of the Kunlun fault, with exclusion of the Haiyuan arcuate tectonic region, the average P-wave velocity is 6.4 km/s and only 0.5 km/s lower than the worldwide average. A combination of the P-wave velocity and Poisson's ratio suggests that the crust is dominantly felsic in composition with an intermediate composition at the base. A mafic lower crust is absent in the NE margin of the Tibetan plateau from the Songpan-Ganzi terrane to the Ordos basin. There are low velocity zones in the West-Qinling Shan and the Haiyuan arcuate tectonic region. The low velocity zones have low S-wave velocities and high Poisson's ratios, so it is possible these zones are due to partial melting. The crust is divided into two layers, the upper and the lower crust, with crustal thickening mainly in the lower crust as the NE Tibetan plateau is approached. The results in the study show that the thickness of the lower crust increases from 22 to 38 km as the crustal thickness increases from 42 km in the Ordos basin to 63 km in the Songpan-Ganzi terrane south of the Kunlun fault. Both the Conrad discontinuity and Moho in the West-Qinling Shan and in the Haiyuan arcuate tectonic region are laminated interfaces, implying intense tectonic activity. The arcuate faults and large earthquakes in the Haiyuan arcuate tectonic region are the result of interaction between the Tibetan plateau and the Sino–Korean and Gobi Ala Shan platforms.     

中国东部岩石圈热状态与流变学强度特征

根据均衡原理制约的地热计算得到中国东部岩石圈的温度分布状态,以40、70、100km和莫霍面深度等温线图以及600°C、1100°C等温面深度的形式表示.同时计算了以1350°C等温面深度表示的中国东部的热岩石圈厚度.结果显示:在扬子克拉通西部四川盆地之下存在160～200km厚的岩石圈根,但在整个华北克拉通之下缺失岩...     

利用接收函数研究鄂尔多斯东缘地壳上地幔结构

       由1876个远震三分量P波地震图组成的数据集,取自布置于鄂尔多斯-太行山一线的宽频带流动台站。通过阵列反 卷积方法,得到地下界面响应的接收函数,并通过共转换点偏移叠加得到地下结构的图像。图像显示,从鄂尔多斯至渤海 湾盆地地壳厚度总体上逐渐变薄,Moho面总体呈小角度向西倾斜。鄂尔多斯块体中部地壳最厚,达到52 km,向东到鄂尔多 斯边缘,地壳厚度减小至43 km。太行山至渤海湾盆地地壳厚度从45 km减小至37 km。山西地堑下方Moho面上隆,和两边的 Moho面相比,抬升8~10 km,且其Moho面的上隆和新生代地堑的凹陷呈镜像关系。     

鄂尔多斯地块基底研究新的思考与认识

鄂尔多斯地块基底岩芯岩石组合、花岗片麻岩的锆石U-Pb年龄、Hf同位素和全岩Nd同位素组成以及航磁异常和地壳速度结构特征表明,该地块中部沿大同-华池基底断裂带存在一航磁异常梯度带,沿该带南缘发育一条2.2~2.0Ga古元古代弧岩浆活动带,并经历了1.96~1.85Ga的变质作用改造,与东缘中部带古元古代中晚期构造演化过程一样,可能代表该地块内部古元古代中晚期形成的一条构造活动带。该活动带以北为东西向展布的正航磁异常带,基底由混合岩化的变泥质和杂砂质片麻岩、片岩及大理岩和石英岩等变质表壳岩和一些花岗片麻岩类构成,记录了新太古代末~2.50Ga和古元古代中期2.2~2.0Ga两期岩浆活动及古元古代末期1.95~1.85Ga变质作用等地质事件,为一主要由新太古代陆壳物质构成的陆块。活动带南部为北东向不规则正、负相间航磁异常带,基底除少量副变质岩外,多为花岗片麻岩类,记录了古元古代中期2.2~2.0Ga岩浆热事件以及1.95~1.85Ga的变质作用改造,除新太古代物质外,还存在古、中太古代陆壳物质,是由一定规模中太古代和部分古太古代陆壳物质以及新太古代新生陆壳添加构成的古老地块。因此,鄂尔多斯地块中部沿大同-华池断裂带成为分割该地块一条重要分界带,其北部地块与其北缘孔兹岩带构成同一构造带,可能代表新太古代陆壳基底之上于古元古代晚期发育的一条大陆边缘活动带。南部则为古、中太古代陆壳与新太古新生陆壳增生而成的古老地块,代表鄂尔多斯地块古老基底陆壳的主体。     

Structure of the Earth’s crust in the northern part of the Barents–Kara region along the 4-AR DSS profile

The 1370 km long 4-AR reference profile crosses the North Barents Basin, the northern end of the Novaya Zemlya Rise, and the North Kara Basin. Integrated geophysical studies including common deep point (CDP) survey and deep seismic sounding (DSS) were carried out along the profiles. The DSS was performed using autonomous bottom seismic stations (ABSS) spaced 10–20 km apart and a powerful air gun producing seismic signals with a step size of 250 m. As a result, detailed P- and S-wave velocity structures of the crust and upper mantle were studied. The basic method was ray-tracing modeling. The Earth’s crust along the entire profile is typically continental with compressional wave velocities of 5.8–7.2 km/s in the consolidated part. Crustal thickness increases from 30 km near the islands of Franz Josef Land to 35 km beneath the North Barents Basin, 50 km beneath the Novaya Zemlya Rise, and 40 km beneath the North Kara Basin. The North Barents Basin 15 km deep is characterized by unusually low velocities in the consolidated crust: The upper crust layer with velocities of 5.8–6.4 km/s has a thickness of about 15 km beneath the basin (usually, this layer wedges beneath deep sedimentary basins). Another special property of the crust in the North Barents Basin is the destroyed structure of the Moho.     

Seismic structure of the Helan–Liupan–Ordos western margin tectonic belt in North-Central China and its geodynamic implications

We study high-resolution three-dimensional P-wave velocity (Vp) tomography and anisotropic structure of the crust and uppermost mantle under the Helan–Liupan–Ordos western margin tectonic belt in North-Central China using 13,506 high-quality P-wave arrival times from 2666 local earthquakes recorded by 87 seismic stations during 1980–2008. Our results show that prominent low-velocity (low-V) anomalies exist widely in the lower crust beneath the study region and the low-V zones extend to the uppermost mantle in some local areas, suggesting that the lower crust contains higher-temperature materials and fluids. The major fault zones, especially the large boundary faults of major tectonic units, are located at the edge portion of the low-V anomalies or transition zones between the low-V and high-V anomalies in the upper crust, whereas low-V anomalies are revealed in the lower crust under most of the faults. Most of large historical earthquakes are located in the boundary zones where P-wave velocity changes drastically in a short distance. Beneath the source zones of most of the large historical earthquakes, prominent low-V anomalies are visible in the lower crust. Significant P-wave azimuthal anisotropy is revealed in the study region, and the pattern of anisotropy in the upper crust is consistent with the surface geologic features. In the lower crust and uppermost mantle, the predominant fast velocity direction (FVD) is NNE–SSW under the Yinchuan Graben and NWW–SEE or NW–SE beneath the Corridor transitional zone, Qilian Orogenic Belt and Western Qinling Orogenic Belt, and the FVD is NE–SW under the eastern Qilian Orogenic Belt. The anisotropy in the lower crust may be caused by the lattice-preferred orientation of minerals, which may reflect the lower-crustal ductile flow with varied directions. The present results shed new light on the seismotectonics and geodynamic processes of the Qinghai–Tibetan Plateau and its northeastern margin.     

Lithospheric structure of the Trans-European Suture Zone along the TTZ–CEL03 seismic transect (from NW to SE Poland)

The large-scale CELEBRATION 2000 seismic experiment investigated the velocity structure of the crust and upper mantle between western portion of the East European Craton (EEC) and the eastern Alps. This area comprises: the Trans-European Suture Zone, the Carpathian Mountains, the Pannonian Basin and the Bohemian Massif. This experiment included 147 chemical shots recorded by 1230 seismic stations during two deployments. Good quality data along 16 main and a few additional profiles were recorded. One of them, profile CEL03, was located in southeastern Poland and was laid out as a prolongation of the TTZ profile performed in 1993. This paper focuses on the joint interpretation of seismic data along the NW–SE trending TTZ–CEL03 transect, located in the central portion of the Trans-European Suture Zone. First arrivals and later phases of waves reflected/refracted in the crust and upper mantle were interpreted using two-dimensional tomographic inversion and ray-tracing techniques. This modelling established a 2-D (quasi 3-D) P-wave velocity lithospheric model. Four crustal units were identified along the transect. From northwest to southeast, thickness of the crust varies from 35 km in the Pomeranian Unit (NW) to 40 km in the Kuiavian Unit, to 50 km in the Radom–Łysogóry Unit and again to 43 km in the Narol Unit (SE). The first two units are thought to be proximal terranes detached from the EEC farther to the southeast and re-accreted to the edge of the EEC during the Early Palaeozoic. The origin of the remaining two units is a matter of dispute: they are either portions of the EEC or other proximal terranes. In the area of the Polish Basin (first two units), the P-wave velocity is very low (V_p < 6.1 km/s) down to depths of 15–20 km indicating that a very thick sedimentary and possibly volcanic rock sequence, whose lower portion may be metamorphosed, is present. The velocity beneath the Moho was found to be rather high, being 8.25 km/s in the northwestern portion of the transect, 8.4 km/s in the central sector, and 8.1 km/s in the southeastern sector.     

珠江口外海域滨海断裂带沿构造走向的变化特征

珠江口外海域滨海断裂带是南海北部陆缘重要的控震和发震构造,其研究关系到区域防震抗震、地壳稳定性评价及对南海构造演化的认识.为探明滨海断裂带沿构造走向上的变化特征,对2015年珠江口海陆联测数据进行了处理,使用射线追踪、走时模拟等方法,获得了珠江口西侧的地壳纵波速度结构模型和滨海断裂带在珠江口地区的发育位置和构造形态等信息.结果显示,珠江口西侧滨海断裂带总体倾向SE,向下可能延伸至莫霍面;沉积层在断裂带陆侧较薄,在滨海断裂带处突然增厚;断裂带内地壳速度为5.3~6.7 km/s,相对两侧地壳表现出低速特征;莫霍面的埋深由断裂带陆侧的28.5 km抬升至其海侧的24.5 km;海陆两侧的地壳结构具有明显的非均一性.对比前人在珠江口东侧的研究成果,珠江口外滨海断裂带总体形态特征相似,但也表现出明显的差异,自东向西,断裂带内部的结构形态从简单变得复杂,逐渐发育明显的阶梯状断层;北界断裂从断距很大的陡崖式正断层逐渐转变为断距较小的低角度正断层,且北界断裂的位置向北错动了一段距离,断裂带内的低速异常则逐渐变弱.本研究不但可以加深对滨海断裂带浅、深部结构的认识,而且还能为研究南海北部陆缘的发震构造提供参考.      

苏鲁造山带地壳上地幔结构层析成像研究

扬子与华北板块在三叠纪的俯冲碰撞形成了著名的苏鲁超高压造山带,其板块碰撞接触关系一直是热点问题.利用国家台网中心64个省台记录的1 079个近震事件的10 922个P波到时和251个远震事件的11 931个P波到时数据,采用远近震联合反演的层析成像方法对苏鲁地区进行了地壳上地幔速度结构反演.结果显示,研究区内两个低速异常区分别对应山东半岛西部的华北板块地幔上隆区和壳幔相互作用强烈的长江中下游成矿带地区.在地幔300 km深度之下出现的高速异常体可能代表了早中生代扬子与华北板块碰撞之前俯冲拆沉的古特提斯洋板块.传统观点的扬子板块岩石圈向北俯冲不明显,华北板块表现为向东南俯冲的高速特征.华北板块俯冲以苏鲁造山带中部的北纬35°为界,分为南北两种俯冲样式.北部俯冲不明显,华北板块停滞在郯庐断裂带以西;南部则表现华北板块向东南陡倾俯冲到苏鲁造山带之下.      

Crustal density structure from 3D gravity modeling beneath Himalaya and Lhasa blocks,Tibet

The Himalaya and Lhasa blocks act as the main belt of convergence and collision between the Indian and Eurasian plates. Their crustal structures can be used to understand the dynamic process of continent–continent collision. Herein, we present a 3D crustal density model beneath these two tectonic blocks constrained by a review of all available active seismic and passive seismological results on the velocity structure of crust and lower lithosphere. From our final crustal density model, we infer that the present subduction-angle of the Indian plate is small, but presents some variations along the west–east extension of the orogenic belt: The dip angle of the Moho interface is about 8–9° in the eastern and western part of the orogenic belt, and about 16° in the central part. Integrating crustal P-wave velocity distribution from wide-angle seismic profiling, geothermal data and our crustal density model, we infer a crustal composition model, which is composed of an upper crust with granite–granodiorite and granite gneiss beneath the Lhasa block; biotite gneiss and phyllite beneath the Himalaya, a middle crust with granulite facies and possible pelitic gneisses, and a lower crust with gabbro–norite–troctolite and mafic granulite beneath the Lhasa block. Our density structure (<3.2 g/cm³) and composition (no fitting to eclogite) in the lower crust do not be favor to the speculation of ecologitized lower crust beneath Himalaya and the southern of Lhasa block.