Global P and PP traveltime tomography: rays versus waves   总被引：2，自引：1，他引：2  

R. Montelli  G. Nolet  G. Masters  F. A. Dahlen  S.-H. Hung 《Geophysical Journal International》2004,158(2):637-654

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The effect of small‐scale heterogeneity on the arrival time of waves     

Jesper Spetzler  Roel Snieder 《Geophysical Journal International》2001,145(3):786-796

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Sensitivities of seismic traveltimes and amplitudes in reflection tomography   总被引：2，自引：0，他引：2  

Yanghua Wang  R. Gerhard Pratt 《Geophysical Journal International》1997,131(3):618-642

Seismic traveltimes and amplitudes in reflection-seismic data show different dependences on the geometry of reflection interfaces, and on the variation of interval velocities. These dependences are revealed by eigenanalysis of the Hessian matrix, defined in terms of the Fréchet matrix and its adjoint associated with different norms chosen in the model space. The eigenvectors and eigenvalues of the Hessian clearly show that for reflection tomographic inversion, traveltime and amplitude data contain complementary information. Both for reflector-geometry and for interval-velocity variations, the traveltimes are sensitive to the model components with small wavenumbers, whereas the amplitudes are more sensitive to the components with high wavenumbers. The model resolution matrices, after the rejection of eigenvectors corresponding to small eigenvalues, give us some insight into how the addition of amplitude information could potentially contribute to the recovery of physical parameters.
In order to cooperatively invert seismic traveltimes and amplitudes simultaneously, we propose an empirical definition of the data covariance matrix which balances the relative sensitivities of different types of data. We investigate the cooperative use of both data types for, separately, interface-geometry and 2-D interval-velocity variations. In both cases we find that cooperative inversions can provide better solutions than those using traveltimes alone. The potential benefit of including amplitude-data constraints in seismic-reflection traveltime tomography is therefore that it may be possible to resolve the known ambiguity between the reflector-depth uncertainty and the interval-velocity uncertainty better.  相似文献   

Finite-frequency sensitivity kernels for head waves   总被引：2，自引：0，他引：2  

Zhigang Zhang  Yang Shen  Li Zhao 《Geophysical Journal International》2007,171(2):847-856

Head waves are extremely important in determining the structure of the predominantly layered Earth. While several recent studies have shown the diffractive nature and the 3-D Fréchet kernels of finite-frequency turning waves, analogues of head waves in a continuous velocity structure, the finite-frequency effects and sensitivity kernels of head waves are yet to be carefully examined. We present the results of a numerical study focusing on the finite-frequency effects of head waves. Our model has a low-velocity layer over a high-velocity half-space and a cylindrical-shaped velocity perturbation placed beneath the interface at different locations. A 3-D finite-difference method is used to calculate synthetic waveforms. Traveltime and amplitude anomalies are measured by the cross-correlation of synthetic seismograms from models with and without the velocity perturbation and are compared to the 3-D sensitivity kernels constructed from full waveform simulations. The results show that the head wave arrival-time and amplitude are influenced by the velocity structure surrounding the ray path in a pattern that is consistent with the Fresnel zones. Unlike the 'banana–doughnut' traveltime sensitivity kernels of turning waves, the traveltime sensitivity of the head wave along the ray path below the interface is weak, but non-zero. Below the ray path, the traveltime sensitivity reaches the maximum (absolute value) at a depth that depends on the wavelength and propagation distance. The sensitivity kernels vary with the vertical velocity gradient in the lower layer, but the variation is relatively small at short propagation distances when the vertical velocity gradient is within the range of the commonly accepted values. Finally, the depression or shoaling of the interface results in increased or decreased sensitivities, respectively, beneath the interface topography.  相似文献   

准噶尔—天山—北山蛇绿岩:对中亚造山带西南缘洋陆格局演化的制约     

高俊  江拓  王信水  李继磊  翟庆国  胡培远  钱青 《地质科学》2022,57(1):1-42

准噶尔、天山和北山52个蛇绿岩的地质特征、地球化学性质和同位素年代学资料系统集成研究表明它们可以分为14条蛇绿(混杂)岩带。绝大多数蛇绿岩呈"岩块+基质"的混杂岩型式沿重要断裂带(构造线)线状分布,少数蛇绿岩以构造岩片叠置方式面状产出。混杂岩的基质有蛇纹岩(碳酸盐化蛇纹岩)和糜棱岩化细碎屑岩两类,岩块既有地幔橄榄岩、基性杂岩和基性火山岩等蛇绿岩组分,也有其它非蛇绿岩组分岩石。堆晶岩出露局限,典型席状岩墙群没有发育。这些蛇绿岩可归类为SSZ(Supra-Subduction Zone)和MORB(Mid-Ocean Ridge)两种类型,前者玄武岩具大离子亲石元素(LILE)富集和高场强元素(HFS)亏损特征,后者不显示该特点;洋岛玄武岩(OIB)既可出现在SSZ型蛇绿混杂岩中,也可为MORB型的组成部分;SSZ型蛇绿混杂岩辉长岩和玄武岩比MORB型具有相对更富集的Sr-Nd同位素组成,但部分形成于弧后(间)盆地的SSZ型蛇绿岩与MORB型一致,具有近亏损地幔的Sr-Nd同位素组成。已确认的最老蛇绿岩为西准噶尔572 Ma玛依勒,次之为北山542~527 Ma月牙山—洗肠井和西准噶尔531 Ma唐巴勒,最年轻蛇绿岩为325 Ma北天山巴音沟和321 Ma北山芨芨台子。根据蛇绿岩证据,结合近年来中亚造山带古地磁、岩浆岩、高压—超高压变质岩和构造地质方面的进展,可以推断埃迪卡拉纪末期—早寒武世,古亚洲洋已达到一定规模宽度,发育洋岛和洋内弧;早古生代时期,多岛洋格局发育至鼎盛期,一系列弧地体分别归属哈萨克斯坦微陆块周缘的科克切塔夫—天山—北山线性弧、成吉思弧、巴尔喀什—西准噶尔弧体系和西伯利亚南部大陆边缘弧体系;晚古生代时期,古亚洲洋于石炭纪末期闭合,增生杂岩和弧地体组成哈萨克斯坦拼贴体系和蒙古拼贴体系两个巨型山弯构造。  相似文献   

洋板块地层学的概念、模式、组成及失序变化^*          下载免费PDF全文

许淑梅  孔家豪  李三忠  舒鹏程  马慧磊  崔慧琪 《古地理学报》2022,24(1):1-10

着重介绍了洋板块地层的概念、模式、组成及失序变化特征。造山带混杂岩和大陆边缘增生复合体是经历俯冲碰撞消亡后的古洋沉积记录,利用微体古生物地层学和同位素年代学方法可以重建造山带混杂岩和大陆边缘增生复合体的原始地层。洋板块地层(学)是用来描述沉淀在洋壳基底之上的沉积岩和火成岩序列的术语,其开始于洋中脊形成,终止于该洋中脊被移入到汇聚边缘增生楔。从造山带混杂岩中重建的古大洋地层的基本组成大体相似,但因大洋岩石圈的岩浆背景不同,造成不同时期和不同类型的洋板块地层组成也会有差异。在前人研究成果的基础上, 笔者通过对不同类型洋板块地层进行分类,介绍了如何从经历碰撞造山过程的增生造山带进行洋板块地层的重建。引入“洋板块地层学”概念的主要目的在于通过对因俯冲增生而消亡的具有洋壳基底的构造洋盆和边缘海盆地的地层单元进行重建,恢复已消失洋的地层组成单元,这对造山带地层解析、造山带构造古地理恢复、重大构造变革期古地理学研究和板块重建等都将起到积极的促进作用。  相似文献   

基于二维VTI拟声波程函方程的椭圆各向异性立体层析反演          下载免费PDF全文

王潇  杨锴 《地球物理学报》2018,61(12):4954-4964

基于二维VTI介质拟声波程函方程,应用射线扰动理论建立了该方程控制下的数据空间各参数对于模型空间各个参数之间的线性关系,从而获得二维VTI介质拟声波程函方程的各向异性立体层析核函数.考虑到拟声波近似程函方程中η参数与ε和δ存在强烈耦合,本文首先探讨椭圆各向异性情形,为二维拟声波程函方程椭圆各向异性立体层析算法奠定了理论基础.同时也为日后推广到非椭圆各向异性情况提供了一种获得高质量初始模型的可靠途径.理论数据算例证实了Fréchet核函数求取的正确性以及在此基础上设计的工作流程实现两参数反演的可行性.  相似文献   

板内扭压造山机制   总被引：5，自引：0，他引：5  

李东旭 《地学前缘》1999,6(4):317-322

据中国大陆板块内部构造特征提出两种扭压造山机制：（１） 扭压滑脱褶皱造山作用;（２） 扭压斜滑断裂岩浆造山作用。前者以扬子板块内的武陵山台褶带为例,后者以华北板块内的太行山断裂岩浆带为例。扭压滑脱褶皱造山作用表现为沉积盖层呈隔档式及隔槽式褶皱;结晶基底呈大型隆起和拗折,莫霍面下降,从而使地壳增厚,构成造山带。值得注意的是,这类滑脱褶皱带的整体形状呈Ｓ状展布,其中的次级褶皱呈雁行状斜列,表明这类造山带的形成除受水平挤压作用外,还伴有左行剪切作用。扭压斜滑断裂岩浆造山作用表现为沿断裂带有一系列花岗质深成岩体展布。这些断裂不仅深切地幔,而且导致下地壳局部融熔形成花岗岩浆,驱动岩浆斜向上升,并控制岩体侵位。与此同时地壳在平面上缩短,垂向上增厚,构成造山带。上述两种造山作用一致表明,东亚大陆在中生代时曾相对太平洋板块向南滑移  相似文献   

新疆可支塔格蛇绿混杂岩的特征及其成因     

张祥信  陈必河  董明星 《华东地质学院学报》2009,32(1):16-21

新疆可支塔格蛇绿混杂岩位于青藏高原北缘东昆仑西段,属于木孜塔格-鲸鱼湖大断裂的西延部分。主要由辉橄岩、辉长岩、闪长岩、斜长花岗岩、辉绿岩、玄武岩及硅质岩等组成,形成时代为早石炭世。其中辉橄岩具有高Mg,贫Al,Ca,低硅、低碱的特点,富集相容元素Cr,Ni,Co。稀土总量低,接近于球粒陨石稀土元素总量,以LREE略富集为特征。闪长岩SiO2,K2O含量较低,MsO,CaO,Na2O较高,稀土总量高,∑REE为90．95×10^-6,LREE富集。斜长花岗岩SiO2 69．8％,Na2O〉K2O,K2O／Na2O为0．78,A／CNK为1．68,具有大洋斜长花岗岩的岩石化学特征。闪长岩、斜长花岗岩的微量元素特征相似,表现为大离子亲石元素K,Sr,Rb,Ba相对富集,高场强元素Nb,Ta,Zr,Hf相对亏损。研究表明,辉橄岩来源于亏损的地幔岩,接近于强烈亏损的方辉橄榄岩,而明显不同于结晶分异作用成因的超镁铁质岩石。闪长岩、斜长花岗岩为蛇绿混杂岩的浅色岩组分,是地幔岩浆结晶分异的产物,但可能受到了围岩的混染和后期热液交代影响。  相似文献   

勉—略混杂岩带构造地质特征与金矿成矿——以陕西省略阳县干河坝金矿床为例     

金文洪  汪志强  高晓宏 《甘肃地质》2011,(3):37-45

勉略带经历俯冲叠置、碰撞造山和陆内造山3个阶段构造演化过程。即俯冲期深层次褶皱与右行顺层（片）剪切变形、碰撞期中—深层次褶皱递进变形和高角度逆冲剪切变形、后主造山期陆内造山期中—浅层次左行走滑变形和低角度逆冲推覆构造4期不同构造变形。其中前两期构造阶段对金矿成矿产生重要影响。通过对陕西省略阳县干河坝金矿研究认为：俯冲期...  相似文献