云南崇山剪切断裂系显微构造特征及其40 Ar-39 Ar年代学约束

野外构造解析和显微构造分析表明:崇山剪切断裂系北部的崇山剪切断裂带为一条左旋走滑剪切带,变形温度为300～550℃,为绿片岩相至低角闪岩相;而南部的临沧剪切带是一条带有NWW-SEE向地壳缩短变形的左旋走滑剪切带,普遍为绿片岩相,变形温度为300～450℃,存在向SE的推覆事件。对采自崇山和临沧韧性剪切带内糜棱岩样品中矿物的40Ar-39Ar年代学研究表明:崇山韧性剪切带凤庆至小湾公路26km处02DX-139样品中黑云母40Ar-39Ar坪年龄为28.3±0.1Ma,临沧韧性剪切带双江粟义剖面02DX-51样品白云母给出了31.5±0.2Ma的坪年龄。崇山-临沧剪切断裂带变形运动学和变形时序与哀牢山-红河剪切断裂带具有很好的一致性,这为理解滇西地区新生代构造演化和亚欧-印度块体的拼合效应及南海海盆的打开提供了新的信息。     

海南公爱NW向韧性剪切带构造特征及其40Ar-39Ar年代学约束

在海南岛西部公爱地区识别出NW向韧性剪切带,其野外构造解析和显微构造分析表明,公爱NW向韧性剪切带早期为右旋剪切,变形温度约300～450℃。对该韧性剪切带糜棱岩样品中白云母单矿物的40Ar39Ar定年结果表明:样品04HN17和04HN18分别给出了250.0±1.0Ma和248.0±1.0Ma的40Ar/39Ar坪年龄,为印支早期变形产物。海南公爱NW向韧性剪切带变形运动学和变形时序与印支北部NW向韧性剪切带(如SongMa地区)具有很好的一致性,这为理解公爱地区早中生代构造演化及华南陆块和印支半岛印支期构造演化提供了新的信息。     

基于3种生物指数的三沙湾养殖活动底栖环境效应研究

为考察我国东海区最为典型养殖海湾三沙湾养殖活动的底栖环境效应,本研究根据2016年8月航次41个样品采集站位的数据,分析香农-威纳多样性指数（Shannon-Wiener index,H'）、海洋生物指数AMBI（AZTI's Marine Biotic Index）和多变量海洋生物指数M-AMBI（Multivariate-AMBI）在4种典型水域（网箱、海藻、鲍鱼养殖和无养殖水域）间的差异及其与沉积物环境因子（δ15N、δ13C、C/N比、总有机碳、总氮、总磷、硫化物、含水率和粉粒-黏粒比例）的相关性。结果表明,航次共采集74种大型底栖生物,H'介于0~3.51;物种多属环境敏感类型（AMBI方法中EGⅠ和EGⅡ生态组）,AMBI指数介于0~4.13,M-AMBI指数介于0.30~0.77。3种生物指数的分布水平表明此海域总体底栖生态质量良好,仅在局部水域存在显著扰动。Kruskal-Wallis检验显示仅H'在不同类型水域之间存在显著差异（P<0.05）,后续配对检验（Pairwise comparision）显示大黄鱼养殖水域H'显著高于海藻养殖水域（P<0.01）。基于斯皮尔曼秩相关系数（Spearman correlation coefficient）的相关性分析表明仅H'和M-AMBI指数分别与总磷存在显著相关性（P<0.05）。聚类分析（Cluster analysis）结果显示不同类型站位在聚类图中随机分布,聚类结果未体现出采样水域的差异性。综上,基于3种生物指数的分析结果显示三沙湾内网箱等典型养殖活动未对区域底栖生境质量造成显著影响。     

济南市农地流转市场发育程度评价研究

农地流转中市场发育情况的研究可以较好地判断未来农地利用可能发生的风险,以济南市农地流转中的市场发育程度评价指标为例,研究农地流转市场的发育程度,以采取切实可行的措施完善农地流转制度。运用特尔菲法确定市场发育程度评价指标体系,并对指标数据进行无量纲处理,用熵值法计算指标权重,利用线性加权法计算市场发育综合评价值,采用正态分布"3σ"方法确定市场发育程度阈值。在统计年限内,济南市2009年、2010年土地流转市场处于过冷区间,2011年偏冷,2012年、2013年正常,2014年、2015年过热,说明农地流转市场发育较快,但滞后于流转量的变化。所选取的评价指体系能够较好的反映济南市农地流转市场发育情况,市场发育程度阈值计算比较科学合理。在当前农地流转市场的培育阶段,当流转量开始下降的时候,需要采取措施以防止流转量的继续下滑,以避免对农地流转市场的发展产生不利影响,进而影响农业经济的发展。     

库鲁克塔格基性岩墙群K—Ar等时年龄测定及其有关问题讨论

新疆库鲁克塔格基性岩墙群的四个样品的Ｋ－Ａｒ表观年龄为４５５－６７３Ｍａ,等时年龄为２８７±１３Ｍａ。这一年龄与近几年报道的沿天山构造带的早二叠世火山岩年龄一致。氩初始值为５０８,在Ｐ型岩浆范围内,结合稀土、微量元素特征,认为岩墙群与地幔热柱有成因联系。     

华南山字型构造体系的厘定及意义

华南山字型的前弧展布于中国大陆南缘和越南北部,南抵西沙纬向带北侧。西翼反射弧出现于念青唐古拉-伯舒拉岭及其南侧,东翼反射弧位于南黄海地区,沿弧形带以中、新生代岩浆岩和构造动力变质带的弧形展布为显著特色。它的脊柱在川、黔、滇、桂毗邻地区,以近SN向褶皱带为主体。华南山字型是印支期发生发展,燕山期成型和定型,喜马拉雅期仍有较强活动的构造体系。该体系的确定,对研究华南地质构造格架与矿产资源的形成和分布规律具有重要意义。实际上,它是特提斯构造域与太平洋构造域间的纽带.      

地球自转速率变化引起的全球应力场

本文用有限元方法计算了地球自转变化引起的全球应力,包括离心惯性力和纬向惯性力引起的应力。离心惯性力变化引起的应力其主方向为SN向和EW向,应力的大小随着地球自转角速度的持续增加而积累,其量级可能达到几十到几百兆帕或更大。纬向惯性力引起的应力,在均匀地球的情况下,主应力方向为NE向和NW向。在地壳厚度按一定规律分布时,应力场的分布沿EW方向具有分带性,并且与全球大洋中脊的分布有对应关系,但应力幅度很小。      

The Earth's natural pulse electromagnetic fields for earthquake time–frequency characteristics: Insights from the EEMD–WVD method

Monitoring the Earth's natural pulse electromagnetic field (ENPEMF) signal is a geomagnetic detection approach for the Earth internal and external studies, and it provides a reference for earthquake prediction. In this paper, the Ensemble Empirical Mode Decomposition–Wigner Ville Distribution (EEMD–WVD) method is used to process the time sequences of the ENPEMF signal detected by GR‐01 receiving devices during the Lushan M_S7.0 earthquake (April 20th, 2013). By obtaining the intrinsic mode function (IMF), the time–frequency–amplitude joint distribution and the energy spectrum of the ENPEMF signal, the suspected anomalies before the earthquake could be shown. The results illustrate the ENPEMF signal before an earthquake and its time–frequency characteristics based on an EEMD–WVD algorithm, proving useful information about the anomalies around the time of the earthquake.     

3D P‐wave traveltime computation in transversely isotropic media using layer‐by‐layer wavefront marching

Subsurface rocks (e.g. shale) may induce seismic anisotropy, such as transverse isotropy. Traveltime computation is an essential component of depth imaging and tomography in transversely isotropic media. It is natural to compute the traveltime using the wavefront marching method. However, tracking the 3D wavefront is expensive, especially in anisotropic media. Besides, the wavefront marching method usually computes the traveltime using the eikonal equation. However, the anisotropic eikonal equation is highly non‐linear and it is challenging to solve. To address these issues, we present a layer‐by‐layer wavefront marching method to compute the P‐wave traveltime in 3D transversely isotropic media. To simplify the wavefront tracking, it uses the traveltime of the previous depth as the boundary condition to compute that of the next depth based on the wavefront marching. A strategy of traveltime computation is designed to guarantee the causality of wave propagation. To avoid solving the non‐linear eikonal equation, it updates traveltime along the expanding wavefront by Fermat's principle. To compute the traveltime using Fermat's principle, an approximate group velocity with high accuracy in transversely isotropic media is adopted to describe the ray propagation. Numerical examples on 3D vertical transverse isotropy and tilted transverse isotropy models show that the proposed method computes the traveltime with high accuracy. It can find applications in modelling and depth migration.     

Effects of anisotropic diffusion on onset of rotating magnetoconvection in plane layer; stationary modes

ABSTRACT

Turbulence in the Earth's outer core not only increases all diffusive coefficients, but it can lead to their anisotropic properties. Therefore, the model of rotating magnetoconvection in horizontal plane layer rotating about vertical axis and permeated by homogeneous horizontal magnetic field, influenced by anisotropic diffusivities, viscosity and thermal diffusivity, is advanced by considering the magnetic diffusivity as anisotropic too. The case of full anisotropy, i.e. all coefficients anisotropic, is compared with both the case possessing isotropic diffusion coefficients and the case of partial anisotropy, i.e. mixed case with isotropic and anisotropic diffusive coefficients (viscosity and thermal diffusivity anisotropic and magnetic diffusivity isotropic). The existence and preference of instabilities is sensitive to all non-dimensional parameters, as well as on anisotropic parameter, the ratio of horizontal and vertical diffusivities. Two types of anisotropy, BM (introduced by Braginsky and Meytlis) and SA (stratification anisotropy) are studied. BM as well as SA were applied by ?oltis and Brestenský to the study of the partial anisotropy; this study is extended, in this paper, to full anisotropy cases (full SA and full BM) and it is shown that the style of convection given by the onset of stationary modes is more affected by anisotropic diffusivities in BM than in SA anisotropy. The important influence of strong anisotropies in the Earth's core dynamics is stressed.