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1.
本文通过对出露于青藏高原东南缘云南六合地区的新生代深源岩石包体(斜长角闪岩、角闪石岩和石榴石透辉岩)的显微组构和地震波各向异性的研究来约束新生代青藏高原东南缘的地壳各向异性.通过角闪石地质压力计计算得知斜长角闪岩、角闪石岩和石榴石透辉岩包体来源于地壳28~36km,为中-下地壳岩石包体.EBSD测量结果显示包体中角闪石的CPO (晶格优选定向)为Type-IV型和(100)[001]滑移,单斜辉石的CPO为SL型和(100)[001]滑移,暗示中-下地壳为高温强变形的特征.通过CPO数据计算获得斜长角闪岩、角闪石岩和石榴石透辉岩包体全岩VP各向异性为1.9%~13.3%,最大分裂的剪切波各向异性(AVS)为1.17%~8.01%.结合前人的研究结果,该地区的地壳岩石能够解释利用Pms震相测量获得的分裂延迟时间,表明云南西北地区的壳内各向异性源于中-下地壳矿物的定向排列.云南西北地区的Pms快波方向近NW-SE向分布并与SKS的快波方向相近,暗示岩石圈变形是耦合的,受控于青藏高原向东南挤出的构造背景.  相似文献   

2.
Partial melting and reactive melt transport may change the composition, microstructures, and physical properties of mantle rocks. Here we explore the relations between deformation and reactive melt transport through detailed microstructural analysis and crystallographic orientation measurements in spinel peridotite xenoliths that sample the shallow lithospheric mantle beneath the southeastern rim of the Siberian craton. These xenoliths have coarse-grained, annealed microstructures and show petrographic and chemical evidence for variable degrees of reaction with silicate melts and fluids, notably Fe-enrichment and crystallization of metasomatic clinopyroxene (cpx). Olivine crystal preferred orientations (CPO) range from strong to weak. [010]-fiber patterns, characterized by a point concentration of [010] normal to the foliation and by dispersion of [100] in the foliation plane with a weak maximum parallel to the lineation, predominate relative to the [100]-fiber patterns usually observed in lithospheric mantle xenoliths and peridotite massifs. Variations in olivine CPO patterns or intensity are not correlated with modal and chemical compositions. This, together with the analysis of microstructures, suggests that reactive melt percolation postdated both deformation and static recrystallization. Preferential crystallization of metasomatic cpx along (010) olivine grain boundaries points to an influence of the preexisting deformation fabrics on melt transport, with higher permeability along the foliation. Similarity between orthopyroxene (opx) and cpx CPO suggests that cpx orientations may be inherited from those of opx during melt-rock reaction. As observed in previous studies, reactive melt transport does not weaken olivine CPO and seismic anisotropy in the upper mantle, except in melt accumulation domains. In contrast, recovery and selective grain growth during static recrystallization may lead to development of [010]-fiber olivine CPO and, if foliations are horizontal, result in apparent isotropy for vertically propagating SKS waves, but strong anisotropy for horizontally propagating surface waves.  相似文献   

3.
利用青藏高原东北缘区域数字地震台网43个台站的远震SKS波形资料,采用最小能量法和旋转相关法得到台站下方上地幔介质各向异性的分裂参数:快波偏振方向(φ)和快慢波时间延迟(δt)。研究结果表明:在塔里木盆地东南缘区域,各向异性快波方向与该区域的断裂走向存在明显的夹角,该盆地向柴达木盆地的俯冲方向一致,各向异性归因为古构造运动遗留下的"化石各向异性",且由于壳幔物质的拆沉作用,推测该区域壳幔之间存在解耦作用;在祁连—河西走廊区,SKS快波偏振方向呈NW-SE,与主要断裂带的走向一致;在西秦岭北缘断裂带附近,观测到快慢波时间延迟有着较大的变化,可能是岩石圈变形和软流圈物质流动共同导致;在鄂尔多斯板块内,快波方向呈NW-SE方向,可能暗示青藏高原深部物质分叉绕流运动。青藏高原东北缘不同区域台站下方的各向异性均具有差异性,进一步证实了青藏高原东北缘地区构造变形的复杂性。  相似文献   

4.
岩石圈各向异性主要由上地幔矿物晶格优势排列方向和上地壳内裂缝、裂隙的定向分布造成.在各向异性特征显著区域,利用SKS震相剪切波分裂获得的延迟时间高达1.5s以上.本文根据方位各向异性,利用广义反射透射系数矩阵方法正演S波接收函数,研究各向异性对不同反方位角接收函数转换震相走时的影响.我们发展了基于HTI模型各向异性走时校正的方法,成功的在单层和多层(快轴方向相同或不同)的各向异性介质中对齐不同反方位角接收函数的Moho面和LAB的转换震相走时.我们将该方法应用于在青藏高原东北缘的流动台站,试图在各向异性强度较大区域对实测数据转换震相走时的校正效果进行测试.结果表明:各向异性走时校正能够加强单台接收函数转换震相的可追踪性,能量增强的叠后转换震相在时深转换后更利于对界面深度的识别与判断;在考虑三维成像的情况下,我们的各向异性校正方法对提高成像结果的准确性有重要意义.  相似文献   

5.
利用甘肃和青海两省固定宽频带地震台记录的远震波形资料,挑选高质量SKS震相,联合使用最小切向能量方法和旋转互相关方法获得230对高信噪比分裂参数;同时对接收函数中Pms震相随方位角的变化进行拟合,得到了24个台站的地壳各向异性分裂参数.整个区域SKS分裂快波方向均值为123°,Pms分裂快波方向均值为132°,且大部分区域SKS、Pms快波方向与地表构造走向相一致,说明青藏高原东北缘以岩石圈垂直连贯变形为主,地壳上地幔相互耦合.SKS、Pms分裂时差均值分别为1.0s和0.6s,显示地壳各向异性对于SKS分裂时差有较大贡献.昆仑断裂附近Pms、SKS分裂快波方向与昆仑断裂走向基本一致,说明昆仑断裂可能是岩石圈尺度深大断裂;而阿尔金断裂东缘二者快波方向显著差异意味着阿尔金断裂在东缘可能仅为地壳尺度的断裂.  相似文献   

6.
当人们试图解释青藏高原异常的剪切波分裂成因时,以下的问题让人们感到困惑:(1)为什么异常大的SKS分裂延时(1.91-2.4s)出现在青藏高原北部Sn波缺失区;(2)为什么分裂延时突变(1.47s和1.09s)出现在Sn波缺失区的边缘;(3)为什么快波极化方向(FPD)与地表大规模的构造走向之间存在约20°-30°的偏差. 本文在综合分析流变学实验和岩石物理学实验研究成果、青藏高原地质和地球物理资料的基础上,提出青藏高原北部地震波各向异性受岩石圈地幔主要矿物的晶格优选方位(LPO)和熔体的定向分布(MPO)的双重控制,并模拟计算了MPO对青藏高原北部岩石圈地幔各向异性强度的贡献. 研究结果表明,由MPO强化的青藏高原北部岩石圈地幔各向异性强度可达10髎,相应的各向异性层厚度平均为94km. 该结果为研究区SKS分裂的成因解释以及造山带深部地质过程的研究提供了新的约束条件.  相似文献   

7.
青藏高原东南缘地震各向异性及其深部构造意义   总被引:1,自引:0,他引:1       下载免费PDF全文
青藏东南缘是青藏高原物质东流的通道,为了更全面了解复杂的岩石圈结构和强烈的变形特征,本文介绍了青藏东南缘岩石圈各向异性的形态,综合其他研究者得到的该区域壳幔各向异性结果,增加了部分新的资料,更新了青藏东南缘岩石圈方位各向异性图像,探讨了区域深部构造意义.
基于近场小震、远震和背景噪声资料计算结果,青藏东南缘地震各向异性展现出独特的区域空间分布和垂向层次性分布形态,展现了3个主要特征.(1)青藏东南缘上地壳各向异性与地表变形测量结果相符,快剪切波偏振方向(即快波方向)呈现与地表运动特征一致的发散性,与主压应力方向一致,但受到地质构造的影响.(2)青藏东南缘下地壳方位各向异性展现了更好的方向一致性,但方位各向异性程度相对较弱,在红河断裂带西北端部和小江断裂带下方有两个下地壳低速区,其方位各向异性程度与上地壳相当.(3)青藏东南缘岩石圈方位各向异性,呈现南、北分区特征,南北分界线大致在26°20'N,快波方向在北部近似为NS方向,在南部近似为EW方向.
本文推测:(1)在26°20'N北侧的上地幔有较厚的高速体,高速体南侧边缘呈现出近EW走向的直立墙形构造,其南侧软弱的上地幔物质在EW方向上流动,导致了岩石圈方位各向异性特征在空间发生突然的变化,快波方向由北部的NS变为南部的EW方向;(2)小江断裂带是现今的华南地块的地壳西边界,但岩石圈尺度的方位各向异性展现出的趋势性表明,华南地块的上地幔物质越过了小江断裂带到达其西侧,揭示了华南地块与青藏地块接触碰撞造成的岩石圈物质变形和上地幔软流圈物质运移的深部图像.地震各向异性能揭示区域深部构造与介质变形的信息,不同观测资料的综合分析有助于获得更清晰的各向异性三维图像.  相似文献   

8.
青藏高原东南缘作为高原物质侧向挤出的前沿地带,是研究岩石圈变形机制、高原物质侧向逃逸和深部动力学等科学问题的关键地区之一.本文利用研究区内540个宽频带流动地震台站记录的远震面波资料,基于程函方程面波层析成像方法获得了青藏高原东南缘周期14~80 s瑞利面波相速度和方位各向异性分布图像.结果显示:14~20 s周期内,面波方位各向异性分布与断裂带的走向和最大主压应力的方向密切相关,可能受到了断裂带和区域构造应力场的共同作用.川滇菱形块体的北部次级块体及丽江—小金河断裂带附近随着面波周期的增加,各向异性快波方向从NS向逐步转变为NE-SW方向,并与断裂带大致平行,而其以南的攀枝花附近表现为高相速度和弱各向异性的特征.我们推测,在川滇菱形块体北部存在明显的下地壳流,流动方向与块体向南的挤出方向基本一致,该地壳流受到攀枝花附近的高速、高强度坚硬块体阻挡,其前缘向西南方向流动.川滇菱形块体中部地区由于坚硬块体的存在,下地壳没有明显的通道流.在红河断裂以西地区,30~60 s周期范围的面波各向异性快波方向和红河断裂大致平行,推测可能与渐新世至中新世早期印支地块向南东方向的挤出密切相关.研究区东北部,四川盆地南缘地壳各向异性以NE-SW和NEE-SWW向为主与SKS快波方向明显不同,推测主要与该地区地壳的早期构造变形有关同时也说明SKS各向异性主要来自上地幔介质;在研究区南部104°E以西的中长周期面波各向异性方向与SKS分裂研究获得的近EW快波方向基本一致,但在104°E以东地区面波各向异性较弱且快波方向与SKS的观测结果存在明显差异,我们推测东部SKS各向异性来源深度至少在150 km以下.  相似文献   

9.
—We examine the possibility of seismic anisotropy in the asthenosphere due to present plate motion using SKS splitting results. The fast directions of anisotropy correlate weakly with the directions of the absolute plate motion (APM) for all APM models. Weak correlation indicates the possibility of asthenospheric anisotropy as well as frozen anisotropy in the lithosphere. Detection of strain rate dependence of anisotropy is helpful to further conclusion of the problem. The selection of reference frame is important to describe shear deformation in the asthenosphere beneath continent due to plate motion. The behavior of hot spots to the mesosphere, fixed or drifted by mantle return flow, is a key of the selection of the reference frame. For the NNR-NUVEL1 model, APM correlated anisotropy appears only at plate velocity faster than 1.4 cm/yr. It suggests the new possibility of the formation of asthenospheric anisotropy in addition to frozen anisotropy in the lithosphere. A critical plate velocity for the formation of anisotropy can be caused by the dislocation-diffusion transition as a function of strain rate on a deformation mechanism map of the upper mantle olivine.  相似文献   

10.
The crustal and upper mantle azimuthal anisotropy of the Tibetan Plateau and adjacent areas was studied by Rayleigh wave tomography. We collected sufficient broadband digital seismograms trav-ersing the Tibetan Plateau and adjacent areas from available stations, including especially some data from the temporary stations newly deployed in Yunnan, eastern Tibet, and western Sichuan. They made an adequate path coverage in most regions to achieve a reasonable resolution for the inversion. The model resolution tests show that the anisotropic features of scope greater than 400 km and strength greater than 2% are reliable. The azimuthal anisotropy pattern inside the Tibetan Plateau was similar to the characteristic of tectonic partition. The crustal anisotropy strength is greater than 2% in most re-gions of East Tibet, and the anisotropy shows clockwise rotation surrounding the eastern Himalayan syntaxis. Vertically, the anisotropy direction indicates a coherent pattern within the upper crust, lower crust, and lithosphere mantle of the Tibetan Plateau, which also is consistent with GPS velocity field and SKS fast polarization directions. The result supports that the crust-mantle deformation beneath the Tibetan Plateau is vertically coherent. The anisotropy strength of crust and lithospheric upper mantle in Yunnan outside the Tibetan Plateau is lower than 2%, so SKS splitting from core-mantle boundary to station should largely be attributed to the anisotropy of asthenosphere.  相似文献   

11.
It has been hypothesised that seismic and electrical anisotropy at the base of the lithosphere are caused by strain-induced lattice-preferred orientation (LPO) of olivine [100] axes parallel to present-day plate motion. This would imply that seismic and electrical anisotropy observations can provide geodynamicists with fundamental information for characterising mantle flow. The qualitative agreement between the fast direction of SV-waves and direction of maximum electrical conductance modelled deeper than 150 km below the North Central craton of Australia appear to support a common alignment mechanism, and the observed, anisotropic electrical conductances can be generated by hydrogen diffusivity in a water-poor (<1000 ppm H/Si) olivine mantle. A quantitative test is proposed for the hypothesis that electrical anisotropy is generated by anisotropic hydrogen diffusion rates (D) in olivine. Electrical anisotropy factors are computed using random resistor network models assuming that D[100]≈20×D[010]≈40×D[001]. Electrical and seismic anisotropies calculated from olivine LPO angular distribution functions modelled for a range of shear strains under a simple shear deformation demonstrate that the intensity of olivine [100] alignments (and associated shear strains) that would be required to explain the electrical anisotropy in the mantle below central Australia are significantly greater than predicted by Rayleigh wave anisotropies. The poor agreement between the observed electrical anisotropies and the electrical anisotropies that would be predicted from the Rayleigh wave anisotropies indicates that either (i) electrical anisotropy in the upper mantle below central Australia is not generated by hydrogen diffusivity alone or (ii) the seismic anisotropy is underestimated. The orientation of the olivine [100] axes maxima is inferred to be ∼30° rotated relative to the direction of present-day absolute plate motion (APM) that is determined relative to the hotspot reference frame (HS2-NUVEL1). Both the APM direction that is determined relative to a reference frame defined by requiring no-net rotation of the lithosphere (NNR-NUVEL1) and GPS-derived plate motion vectors fit the geophysical observations of upper mantle anisotropy better. This may support the contention that hotspots are not stationary relative to the deep mantle.  相似文献   

12.
Peridotite xenoliths with a broad range of textures provides evidence for consistent microstructural evolution in a vertical transect of the shallow lithospheric mantle (35–55 km depth) beneath the Persani Mountains, SE Carpathians, Romania, due to ongoing plate convergence in the Carpathian Arc nearby. The recrystallized grain size, crystal preferred orientations strength, and resulting seismic anisotropy vary continuously and display a strong correlation to equilibrium temperatures, suggesting a continuous change in deformation conditions with depth. The shallowmost xenoliths have microstructures typical of high stress deformation, marked by strong recrystallization to fine grain sizes, which results in weak crystal preferred orientations and anisotropy. The deepest xenoliths have coarse-grained porphyroclastic microstructures and strong crystal preferred orientations. Replacive orthopyroxene structures, consuming olivine, and high H2O concentrations in the pyroxenes are observed in some xenoliths indicating limited percolation of fluids or volatile-rich melts. Despite the high stress deformation and high H2O contents in some of the studied xenoliths, analysis of olivine crystallographic orientations indicates that [100] slip systems, rather than “wet” [001] accommodate most of the deformation in all samples. Seismic anisotropy estimated from the measured olivine and pyroxene crystal preferred orientations suggests that the strike-parallel fast SKS polarization directions and ~ 1 s delay times measured in the SE Carpathians are likely the consequence of convergence-driven belt-parallel flow in the lithospheric mantle.  相似文献   

13.
地震层析成像研究清晰给出了地球深部俯冲板片的大尺度形态,但与俯冲过程相关的地幔流动特征仍不明确.在俯冲地幔楔系统中,前人观测到了与海沟平行和垂直的快波偏振方向.本文研究了西北太平洋俯冲板片在地幔过渡带中停滞形成的"大地幔楔"中的各向异性特征.对具有长期稳定观测数据的MDJ台站SKS震相和区域深源地震的直达S波震相进行了...  相似文献   

14.
Located at the northeastern margin of the Tibetan plateau,the Ordos block is a stable tectonic unit in North China.With its active boundary fault zones,the Ordos block played an important role in the eastward extrusion mechanism of the Tibetan plateau.Peking University deployed a linear array of 15 portable broadband seismometers across the western Weihe graben during September 2005 to August 2006 and later a 2-D seismic array(Southwest Ordos Array) of 14 portable broadband seismometers during 2007-2008 at its southwestern boundary.Analyses of shear wave splitting of SKS and SKKS phases at these stations show that the fast directions trend ~110° with an average delay time of 0.9 s in the southwestern margin of the Ordos block.The agreement between the lithosphere deformation indicated by GPS data and Quaternary fault slip-rate observations and the mantle flow represented by shear wave splitting implies that accordant deformation patterns from lithosphere to asthenosphere in relation to the eastward extrusion of the Tibetan plateau could extend at least to 200 km depth.Spatial distribution of splitting polarization directions indicates that the mantle flow driven by the Tibetan plateau is blocked by the Ordos block and locally restricted in a narrow channel along the Qinling-Dabie fault zones between the Ordos block and Sichuan basin.  相似文献   

15.
青藏高原中部地壳和上地幔各向异性分析   总被引:1,自引:1,他引:0       下载免费PDF全文
张智  田小波 《地球物理学报》2011,54(11):2761-2768
对布设于青藏高原中部INDEPTH-III宽频带数字地震台阵的41个台站记录的远震体波资料所提取出的P波接收函数和SKS波形资料做偏振分析,并采用以误差为权的叠加分析方法求得每一个台站的Pms和SKS快波偏振方向和快慢波的时间延迟,获得了从拉萨块体中部,经喀喇昆仑-嘉黎断裂系和班公湖-怒江缝合带,到羌塘块体中部的地壳和...  相似文献   

16.
Strong seismic anisotropy beneath Tibet has recently been reported from the study of SKS shear wave splitting. The fast split waves are generally polarized in an easterly direction, close to the present day direction of motion of the Tibetan crust relative to stable Eurasia, as deduced from Holocene slip rates on the major active faults in and around Tibet. This correlation may be taken to suggest that the whole Tibetan lithosphere is being extruded in front of indenting India and that the anisotropic layer is the deforming asthenosphere, that accommodates the motion of the Tibetan lithosphere relative to the fixed mantle at depth. Uncertainties about this motion are at present too large to bring unambiguous support to that view. Assuming that this view is correct however, a simple forward model is used to compute theoretical delay times as a function of the thickness of the anisotropic layer. The observed delay times would require a 50–100 km thick anisotropic layer beneath south-central Tibet and an over 200 km thick layer beneath north-central Tibet, where particularly hot asthenosphere has been inferred. This study suggests that the asthenospheric anisotropy due to present absolute block motion might be dominant under actively deforming continents.  相似文献   

17.
Over the past 10 years,the number of broadband seismic stations in China has increased significantly.The broadband seismic records contain information about shear-wave splitting which plays an important role in revealing the upper mantle anisotropy in the Chinese mainland.Based on teleseismic SKS and SKKS phases recorded in the seismic stations,we used the analytical method of minimum transverse energy to determine the fast wave polarization direction and delay time of shear-wave splitting.We also collected results of shear-wave splitting in China and the surrounding regions from previously published papers.From the combined dataset we formed a shear-wave splitting dataset containing 1020 parameter pairs.These splitting parameters reveal the complexity of the upper mantle anisotropy image.Our statistical analysis indicates stronger upper mantle anisotropy in the Chinese mainland,with an average shear-wave time delay of 0.95 s;the anisotropy in the western region is slightly larger(1.01 s)than in the eastern region(0.92 s).On a larger scale,the SKS splitting and surface deformation data in the Tibetan Plateau and the Tianshan region jointly support the lithospheric deformation mode,i.e.the crust-lithospheric mantle coherent deformation.In eastern China,the average fast-wave direction is approximately parallel to the direction of the absolute plate motion;thus,the upper mantle anisotropy can be attributed to the asthenospheric flow.The area from the Ordos block to the Sichuan Basin in central China is the transition zone of deformation modes between the east and the west regions,where the anisotropy images are more complicated,exhibiting"fossil"anisotropy and/or two-layer anisotropy.The collision between the Indian Plate and the Eurasian Plate is the main factor of upper mantle anisotropy in the western region of the Chinese mainland,while the upper mantle anisotropy in the eastern region is related to the subduction of the Pacific Plate and the Philippine Sea Plate beneath the Eurasian Plate.  相似文献   

18.
南北构造带北段上地幔各向异性特征   总被引:9,自引:5,他引:4       下载免费PDF全文
对布设在南北构造带北段的中国地震科学探测台阵项目二期674个宽频带流动台站和鄂尔多斯台阵21个宽频带流动台站记录的远震XKS(SKS、SKKS和PKS)波形资料作偏振分析,采用最小切向能量的网格搜索法和"叠加"分析方法求得每一个台站的XKS波的快波偏振方向和快、慢波的时间延迟,并结合该区域出版的122个固定台站的分裂结果,获得了南北构造带北段上地幔各向异性图像.快波方向分布显示青藏高原东北缘、阿拉善块体和鄂尔多斯块体西缘的快波方向主要表现为NW—SE方向,秦岭造山带的快波方向为近E—W方向,鄂尔多斯块体内部的快波方向在北部为近N—S方向,南部表现为近E—W方向.时间延迟分布来看,鄂尔多斯块体的时间延迟不仅明显小于其周缘地区,而且小于其他构造单元,特别是在高原东北缘、阿拉善块体和鄂尔多斯块体的交汇地区的时间延迟很大,反映了构造稳定单元的时间延迟小于构造活跃单元.通过比较快波方向的横波分裂测量值与地表变形场模拟的预测值,并结合研究区地质构造和岩石圈结构特征分析表明,在青藏高原东北缘、阿拉善块体和鄂尔多斯块体西缘各向异性主要由岩石圈变形引起,地表变形与地幔变形一致,地壳耦合于地幔,是一种垂直连贯变形模式;秦岭造山带的各向异性不仅来自于岩石圈,而且其岩石圈板块驱动的软流圈地幔流作用不可忽视;鄂尔多斯块体内部深浅变形不一致,具有弱的各向异性、厚的岩石圈和构造稳定的特征,我们认为其各向异性可能保留了古老克拉通的"化石"各向异性.  相似文献   

19.
青藏高原东北缘上地幔各向异性研究   总被引:21,自引:13,他引:8       下载免费PDF全文
通过分析位于青藏高原东北缘的区域数字地震台网30个台站的远震SKS波形资料,采用最小切向能量的网格搜索法和叠加分析方法求得每一个台站的SKS快波偏振方向和快、慢波的时间延迟,获得了青藏高原东北缘上地幔各向异性图像.从得到结果看,青藏高原东北缘的各向异性快波方向基本上呈NW-SE方向,并有一顺时针旋转趋势,快、慢波时间延迟是0.70~1.51 s.青藏高原东北缘的SKS快波偏振方向与区域内主要构造断裂走向基本一致;各向异性快波偏振方向变化与区域内最小平均主压应力方向变化相似,也与由GPS测量得到的速度场方向变化相似.研究表明青藏高原东北缘上地幔物质在区域构造应力场的作用下,发生了顺时针旋转的形变以至流动,使得上地幔中橄榄岩的晶格排列方向平行于物质形变或流动方向,上地幔变形和上覆地壳变形可能存在垂直连贯变形特征.  相似文献   

20.
本文对布设在华北克拉通东西两块体交界区域的宽频带流动地震观测台阵和部分固定台站的远震波形记录开展了SKS波分裂研究.结果显示,鄂尔多斯块体内部的各向异性比较弱,剪切波分裂导致的时间延迟一般小于0.7s.鄂尔多斯块体东缘的山西断陷带和太行山以及华北平原西部均表现出了比较强的各向异性,时间延迟大于1.0s.特别是在太行山地区观测到的ENE趋向的快波偏振方向明显不同于鄂尔多斯块体和华北平原地区的近E-W和ESE方向的快波偏振方向.在华北克拉通东西两块体交界过渡带的太行山地区观测到的显著上地幔各向异性及变化可能对应于围绕鄂尔多斯块体东南角的局部软流圈绕流,而后者可能起因于鄂尔多斯块体的逆时针旋转以及青藏高原软流圈沿秦岭大别造山带向东的流动.  相似文献   

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