富碱斑岩中超镁铁深源包体岩石的矿物学特征

在云南省鹤庆县六合乡富碱斑岩体中找到超镁铁深源岩石包体，这对于研究富碱斑岩的起源和演化及其成岩成矿作用具有重要意义。本文较系统地研究了深源包体岩石的矿物学特征，揭示该深源包体具有原始上地幔岩在地幔条件下受到一定程度富集地幔流体交代作用改造的特征，具有富集地幔低程度部分熔融属性，为富碱斑岩的成岩成矿演化提供了重要的矿物学依据。     

The Mw = 6.0, 7 September 1999 Athens Earthquake

On 7 September 1999 at 11:56 GMT a destructive earthquake (M_w = 6.0) occurred close to Athens (Greece). The rupture process is examined using data from the Cornet local permanent network, as well as teleseismic recordings. Data recorded by a temporary seismological network were analyzed to study the aftershock sequence. The mainshock was relocated at 38.105°N, 23.565°E, about 20 km northwest of Athens. Four foreshocks were also relocated close to the mainshock. The modeling of teleseismic P and SH waves provides a well-constrained focal mechanism of the mainshock (strike = 105°, dip = 55° and rake = -80°) at a depth of 8 km and a seismic moment M₀ = 1.010²⁵ dyn·cm. The obtained fault plane solution represents normal faulting indicating an almost north-south extension. More than 3500 aftershocks were located, 1813 of which present RMS < 0.1 s and ERH, ERZ < 1.0 km. Two main clusters were distinguished, while the depth distribution is concentrated between 2 and 11 km. Over 1000 fault plane solutions of aftershocks were constrained, the majority of which also correspond to N–S extension. No surface breaks were observed but the fault plane solution of the mainshock is in agreement with the tectonics of the area and with the focal mechanisms obtained by aftershocks. The hypocenter of the mainshock is located on the deep western edge of the fault plane. The relocated epicenter coincides with the fringe that represents the highest deformation observed on the differential interferometric image. The calculated source duration is 5 sec, while the estimated dimensions of the fault are 15 km length and 10 km width. The source process is characterized by unilateral eastward rupture propagation, towards the city of Athens. An evident stop phase observed in the recordings of the Cornet local stations is interpreted as a barrier caused by the Aegaleo Mountain.     

Stability of earthquake moment tensor inversions: effect of the double-couple constraint

We show that spurious large non-double-couple components can be obtained in inversions for the full deviatoric moment tensor for shallow crustal earthquakes due to inaccurate Earth models. The traditional “best double-couple” solution does not in general provide an optimal estimate of a double-couple mechanism, and is only reliable when the non-double-couple component of the full deviatoric solution is small. The inverse problem for the moment tensors of the 1998 Antarctic Plate and 2000 Wharton Basin strike-slip earthquakes is shown in each case to have two well-fitting minima in the misfit function of pure double-couple solutions. Such pairs of solutions are most likely to exist for earthquakes which are close either to vertical strike-slip or to dip-slip on a fault plane dipping at 45°. It is shown theoretically that these pairs of solutions arise from the combination of the pure double-couple constraint and the instability of two elements of the moment tensor. No significant non-double-couple component is found for the shallow thrusting 1996 Biak, Indonesia earthquake.     

玛曲县格尔柯金矿床控矿地质条件及其矿床成因探讨

格尔柯金矿 (即大水金矿 )是产于西秦岭南带西倾山—迭山逆冲褶断带南缘的特大型金矿。矿床控矿地质条件为构造单元界断裂带、深源浅成花岗闪长斑岩小侵入体、下三叠统马热松多组 (T1m)碳酸盐岩沉积建造 ,与金矿关系密切的矿化蚀变有硅化、赤铁矿化、褐铁矿化和方解石化 ;矿床成因类型为层控—热水溶滤构造蚀变岩型。     

甘肃小柳沟钨多金属矿地质特征及成矿模式

小柳沟钨多金属矿于 90年代初发现 ,目前已具大型、超大型规模。共有 4个矿床。成矿主要与长城系朱龙关群和隐伏花岗岩有关。该矿床成矿物质来源具双重性 ,成矿温度为中高温 ,成矿流体为中等盐度 ,同位素计算模式年龄确定其成矿于加里东期。矿床成因属于火山喷发沉积—岩浆热液改造矿床。     

Caractérisation des paragenèses et des paléocirculations fluides dans l'indice d'or de Bleı̈da (Anti-Atlas,Maroc)Characterization of the paragenesis and the fluid palaeo-circulations in the gold showings of Bleida (Anti-Atlas,Morocco)

The gold showings at Bleida are hosted in Late Pan-African N50–80 °E quartz–hematite–chlorite 1 tension lenses that are related to the activity of major sinistral sub-east–west thrusts. Ores result from three superimposed stages of fluid migration. Gold occurs in microcracks offsetting the earlier minerals. Fluids evolved from COHN compositions with a saline component to boiling aqueous fluids. Pressure and temperature decreased from 50 MPa and 300 °C to less than 4 MPa and 150 °C. Thus, the gold showings at Bleida were formed in a typical geothermal (epithermal) setting, likely controlled by the Late Pan-African magmatism. To cite this article: A. Barakat et al., C. R. Geoscience 334 (2002) 35–41     

震源时间函数与震源破裂过程

简要介绍了现代数字地震学的两个重要概念。一个是震源时间函数，另一个是地震震源的时空破裂过程。首先，从地震断层位移表示定量出发，介绍震源时间函数和震源破裂过程的基本概念。然后，分别介绍两种从远场地震记录中提取震源时间函数和获取有限断层面上时空破裂过程图像的反演方法。     

科技期刊发展的挑战与机遇

中国加入世贸组织后 ,面对开放的世界性大市场的直接冲击 ,我国出版发行行业的竞争必将更加激烈。优胜劣汰 ,会直接考验每个出版社、每份期刊。为了使我国的期刊在竞争中成为胜者 ,探讨了科技期刊参与竞争的困难与优势 ,提出了如何提高我国科技期刊竞争力的粗浅看法     

漾濞地震震源位置分析

采用一致的地震震相和台网布局，应用昆明数字地震台网资料，对2002年月1月4日－1月7日的漾濞地震及序列作进一步核定，得出了更精确的地震震源位置，并作出三维空间图。     

2001年1月2 6日印度古杰拉特(Gujarat)Ｍem>Ssub>7.8地震时空破裂过程

从全球数字地震台网的长周期记录中，选择了震中距小于90的27个台站的54个P波震相和44个S波震相资料．首先，用波形反演方法确定了2001年1月26日印度古杰拉特(Gujarat)ＭS7.8地震的地震矩张量、震源机制、震源时间函数和时空破裂过程等震源参数．通过矩张量反演，并根据Kutch Mainland断层的走向、地震烈度的空间分布、余震震源的空间分布和震害的空间分布，确认2001年1月26日印度古杰拉特ＭS7.8地震的发震断层的走向为92、倾角为58、滑动角为62，即一走向近东-西向、断层面向南倾斜、以逆冲为主的左旋-逆断层．这次地震所释放的地震矩为3.51020 Nm，矩震级ＭW＝7.6．然后，借助合成地震图，采用频率域求谱商的方法，得到了依赖于台站方位的27个P波震源时间函数、22个S波震源时间函数以及平均的P波震源时间函数和S波震源时间函数．对震源时间函数的分析表明，这次地震是一次连续的破裂事件，开始比较急遽，但结束比较迟缓，总持续时间约19 s．最后，以所提取的P波和S波震源时间函数为资料，采用时间域的反演技术得到了断层面上滑动的时空分布．滑动量在断层面上的静态分布表明，断层面上的最大滑动量约为7 m．断层面上的最大应力降约为30 MPa，平均应力降约为7 MPa．滑动量大于0.5 m的区域在走向方向长85 km，在断层面倾斜方向宽约60 km(相应地，在深度方向约51 km)．破裂向东扩展约50 km，向西扩展约35 km．滑动量大于0.5 m的区域的主要部分呈椭圆形，其长轴取向与断层滑动方向一致．表明此区域破裂扩展的方向即是断层错动的方向．这种现象对于走滑断层情形是多见的，但对逆冲断层情形却少见．断层面上初始破裂点以东、以上部分面积大于初始破裂点以西、以下部分的面积，这是破裂非对称性的表现，表明破裂具有自西向东、自下向上单侧破裂的特征．从滑动率随时空变化的快照可以看出，滑动率在第4 s达到最大值，此时滑动率约为0.2 m/s，滑动基本上发生在破裂起始点及其周围．从第6 s开始，起始点的破裂基本结束，破裂开始向外围扩展．破裂向西的扩展速度明显小于向东的扩展速度．在第15 s，这种环形的扩展基本结束．自16 s以后，主要是一些零星的破裂点分布在破裂区的外围．从滑动量随时空变化的快照看，破裂自起始点开始后，逐渐向四周扩展．主要的破裂(滑动量大于5 m的区域)在6～10 s，具有明显的自西向东、向上的单侧破裂特征．在第11～13 s，破裂的西端向西、向下有所扩展．整个破裂过程持续约19 s．在整个破裂过程中的平均破裂速度约为3.3 km/s．