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Crustal and upper-mantle structure of the southeastern Tibetan Plateau from joint analysis of surface wave dispersion and receiver functions

机译:从表面波散射与接收函数的联合分析看青藏高原东南部的晶体和上地幔结构

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摘要

Researches on the southeastern Tibetan Plateau provide important insights into the tectonic evolution of the Tibetan Plateau. In this study, we have constructed a high-resolution 3D shear-wave velocity model through joint inversion of receiver functions and surface wave dispersion data. The crustal thickness and Poisson's ratio models are first determined by H-k stacking of receiver functions. The crustal thickness changes from 30 km in the south to 62 km in the north, presenting strong lateral variations. The fundamental mode of Rayleigh wave dispersion data spanning periods from 8 to 65 s were then jointly used to constraint the absolute shear-wave velocity. The shear-wave velocity structure shows lateral variations. There are low velocity zones distributed in the crust and upper mantle. Two continuously distributed low velocity zones are clearly presented in the middle-to-lower crust, which extend from north toward southeast and southwest, respectively, joining together in southern Yunnan. In this study, we deduced the migration model of soft materials in middle-to-lower crust in southeastern Tibetan Plateau, which explains that the resistance from Sichuan Basin separates the flowing materials from Tibetan Plateau into southeast and northwest branches. They flow along the west margin of Sichuan Basin and then extrude out from northeastern and southeastern Tibetan Plateau respectively. The southeast branch is blocked and cannot flow in the entire crust. It is limited in a certain range of depths and channels. The two low velocity zones in this study possibly present two flow channels of the middle-to-lower crustal materials extruded from the Tibetan Plateau. (C) 2015 Elsevier Ltd. All rights reserved.
机译:对青藏高原东南部的研究为青藏高原的构造演化提供了重要的见识。在这项研究中,我们通过接收函数和表面波频散数据的联合反演,构建了高分辨率的3D剪切波速度模型。地壳厚度和泊松比模型首先由接收函数的H-k叠加确定。地壳厚度从南部的30 km变化到北部的62 km,呈现出强烈的横向变化。然后联合使用跨越8到65 s周期的瑞利波频散数据的基本模式来约束绝对剪切波速度。横波速度结构显示出横向变化。在地壳和上地幔中分布着低速带。在中下地壳中清楚地显示了两个连续分布的低速带,分别从北向东南和西南延伸,在云南南部汇合在一起。在这项研究中,我们推导了软物质在青藏高原东南部中下地壳的迁移模型,这说明四川盆地的阻力将青藏高原的流动物质分为东南和西北分支。它们沿着四川盆地的西缘流动,然后分别从东北高原和东南高原挤出。东南分支被阻塞,无法在整个地壳中流动。它被限制在一定深度和通道范围内。本研究中的两个低速带可能呈现出从青藏高原挤出的中低层地壳物质的两个流动通道。 (C)2015 Elsevier Ltd.保留所有权利。

著录项

  • 来源
    《Journal of Asian earth sciences》 |2016年第1期|52-63|共12页
  • 作者单位

    Wuhan Univ, Sch Geodesy & Geomat, Dept Geophys, Wuhan 430079, Peoples R China;

    Wuhan Univ, Sch Geodesy & Geomat, Dept Geophys, Wuhan 430079, Peoples R China|Wuhan Univ, Minist Educ, Key Lab Geospace Environm & Geodesy, Wuhan 430079, Peoples R China|Wuhan Univ, Collaborat Innovat Ctr Geospace Informat Sci, Wuhan 430079, Peoples R China;

    Wuhan Univ, Sch Geodesy & Geomat, Dept Geophys, Wuhan 430079, Peoples R China;

    Wuhan Univ, Sch Geodesy & Geomat, Dept Geophys, Wuhan 430079, Peoples R China;

    Wuhan Univ, Sch Geodesy & Geomat, Dept Geophys, Wuhan 430079, Peoples R China;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Southeastern Tibetan Plateau; Joint analysis; Receiver function; Surface wave dispersion; Crustal flow;

    机译:青藏高原东南部;联合分析;接收函数;地表波频散;地壳流;

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