冀北发现具鬣刺结构的超基性岩

冀北具鬣刺结构的超基性岩呈透镜状，产于华北克拉通北缘的早元古宙红旗营子群黑云斜长片麻岩之中。富MgO，贫CaO，A12O3和FeO*＝0．86，TiO2介于0．01％-0．02％之间，与SSZ型蛇绿岩中相应岩石的TiO2含量相当。原始地幔标准化的过渡元素配分型式表现为不对称的“W”型，在TiO2和Cu处形成两个明显的负异常“谷”。据此地球化学特征意味着它们可能来自于消减带之下上地幔，为上地幔高度部分熔融的残余物。岩石中鬣刺结构可能是叶蛇纹石高压分解的结果，表明研究区某些变质橄榄岩岩块曾经受过俯冲—消减作用。     

庐山星子群变质岩的变质作用P-T条件研究

对分布于扬子块体南缘古元古代星子群变质宏的变质作用研究表明，它们普遍经历了角闪岩相的变质，其变质温度为480℃-580℃，压力在300MPa-500MPa之间。这与扬子块体南缘其他元古代地层仅经历了轻微变质的事实截然不同，表明星子群变质岩具有独特的构造演化历史。越来越多的研究发现，星子群变质岩是由地壳伸展作用引发的、来源于下地壳的前寒武纪变质基底，它并不是来源于华夏块体的“飞来峰”。     

巴音宝力格隆起带中新生代盆地砂岩型铀矿成矿地质条件及远景分析

本根据野外调查及室内系列编图成果，分析了巴音宝力格隆起带中新生代盆地砂岩型铀矿成矿地质条件，认为下白里统巴彦花组是中新生代盆地的找矿目的层位，并存在古河道与潜水层间氧化带两种砂岩型铀矿类型。巴彦毛都、准巴彦塔拉、乌里雅斯太和伊勒门盆地是形成砂岩型铀矿的远景盆地。     

河北平山湾子群夕线石英集合体的地质地球化学特征及成因

河北平山地区早前寒武纪湾子群及相关岩石中夕线石英集合体成因存在长期争论。根据地质地球化学研究，本文将它们划分为3种不同类型。(1)球状和团块状夕线石英集合体，其形成与钾长浅粒岩的深熔作用有关。(2)面状夕线石英集合体，与钾长浅粒岩在应力状态下的变质分异作用有关。两者地球化学组成及与相邻浅色体关系受母岩和作用过程双重因素制约。(3)层状夕线石英集合体，为变质沉积成因，地球化学上反映了变质原岩的组成特征。     

长江源各拉丹冬地区三叠纪结扎群沉积特征及层序地层研究

三叠纪结扎群分布于长江源各拉丹冬地区南北两侧，根据基本层序、沉积环境和层序界面特征，结扎群至少可划分出四个三级层序。沉积古地理格局显示出南浅北深的特点。南部靠近羌塘盆地中央隆起带，陆源物质供应丰富。北部雀莫错一带因远离中央隆起，陆源物质供应相对较少，以泥岩、灰岩为主，生物化石丰富，沉积环境以陆棚为主，在相对稳定的沉积水体中以双壳类、菊石类等生物群得以快速发展。     

辽西朝阳盆地早白垩世一新的无齿翼龙化石

采自辽西朝阳盆地早白垩世九佛堂组的一翼龙化石被记述。化石材料是一接近完整骨架的无齿的翼龙，带有一不完全的头骨。作者将其归于翼手龙类(Pteroclactyloidea)，并建一新属、新种一无齿吉大翼龙(Jidapterus edentus gen．et sp．nov．)。     

内蒙古固阳渣尔泰山群层序地层学及其控制因素

渣尔泰山群是华北地台北缘中元古代裂陷槽沉积,主要为一套遭受绿片岩相区域变质的碎屑岩-碳酸盐岩建造。根据岩性、岩相、相序和不整合界面的综合研究,对这套地层进行了详细的层序界面分析和层序划分,识别出Ⅰ型、Ⅱ型和暴露-淹没复合型(Ⅲ型)3种类型层序界面,共划分出1个超层序、2个大层序和7个层序。总结了渣尔泰山群在碎屑滨岸、台缘碳酸盐岩与碎屑岩混积、碳酸盐台地、台前斜坡和陆棚盆地等不同古地理背景下的层序发育模式及其内部构成特征,并探讨了复合海平面变化、构造活动、沉积物供给、古地形等因素对层序形成和演化的控制作用。     

新疆普鲁一带下古生界地层岩石组合及构造环境

西昆仑地块是西昆仑造山带的重要组成部分，南北边界分别为康西瓦—苏巴什华力西期缝合带和库地—其曼于特加里东期缝合带。新疆普鲁一带下古生界地层，分布于西昆仑地块东部，主要由一套海相火山岩和浅海陆棚相细碎屑岩组成，并遭受了绿片岩相的变质作用。通过1：25万《于田一伯力克幅)区调工作，将新疆普鲁一带下古生界地层厘定为下古生界奥陶—志留系，认为形成的大地构造环境为大陆活动边缘。     

Practical VTI approximations: a systematic anatomy

Transverse isotropy (TI) with a vertical symmetry axis (VTI) often provides an appropriate earth model for prestack imaging of steep-dip reflection seismic data. Exact P-wave and SV-wave phase velocities in VTI media are described by complicated equations requiring four independent parameters. Estimating appropriate multiparameter earth models can be difficult and time-consuming, so it is often useful to replace the exact VTI equations with simpler approximations requiring fewer parameters. The accuracy limits of different previously published VTI approximations are not always clear, nor is it always obvious how these different approximations relate to each other. Here I present a systematic framework for deriving a variety of useful VTI approximations. I develop first a sequence of well-defined approximations to the exact P-wave and SV-wave phase velocities. In doing so, I show how the useful but physically questionable heuristic of setting shear velocities identically to zero can be replaced with a more precise and quantifiable approximation. The key here to deriving accurate approximations is to replace the stiffness a₁₃ with an appropriate factorization in terms of velocity parameters. Two different specific parameter choices lead to the P-wave approximations of Alkhalifah (Geophysics 63 (1998) 623) and Schoenberg and de Hoop (Geophysics 65 (2000) 919), but there are actually an infinite number of reasonable parametrizations possible. Further approximations then lead to a variety of other useful phase velocity expressions, including those of Thomsen (Geophysics 51 (1986) 1954), Dellinger et al. (Journal of Seismic Exploration 2 (1993) 23), Harlan (Stanford Exploration Project Report 89 (1995) 145), and Stopin (Stopin, A., 2001. Comparison of v(θ) equations in TI medium. 9th International Workshop on Seismic Anisotropy). Each P-wave phase velocity approximation derived this way can be paired naturally with a corresponding SV-wave approximation. Each P-wave or SV-wave phase velocity approximation can then be converted into an equivalent dispersion relation in terms of horizontal and vertical slownesses. A simple heuristic substitution also allows each phase velocity approximation to be converted into an explicit group velocity approximation. From these, in turn, travel time or moveout approximations can also be derived. The group velocity and travel time approximations derived this way include ones previously used by Byun et al. (Geophysics 54 (1989) 1564), Dellinger et al. (Journal of Seismic Exploration 2 (1993) 23), Tsvankin and Thomsen (Geophysics 59 (1994) 1290), Harlan (89 (1995) 145), and Zhang and Uren (Zhang, F. and Uren, N., 2001. Approximate explicit ray velocity functions and travel times for P-waves in TI media. 71st Annual International Meeting, Society of Exploration Geophysicists, Expanded Abstracts, 106–109).     

西藏南部郎杰学群碎屑物质来源的古水流证据

新近对西藏山南琼果和贡嘎地区(特提斯喜马拉雅北亚带)弱变质的上三叠统深海—半深海沉积地层——郎杰学群地质填图调查,在出露槽模沉积构造的37个古水流点获得了43组数据。赤平投影数据恢复后发现,这一地区主力古水流有南东140°～160°和南西190°～210°两个方向。这一分析结果为郎杰学群沉积物来自北边(未知块体)而非印度次大陆的观点提供了有力证据。