塔里木盆地晚泥盆世及石炭纪岩相古地理

塔里木盆地上泥盆统及石炭系包括5个组，自下而上分别为上泥盆统东河塘组和甘木里克组，石炭系巴楚组、卡拉沙依组和小海子组。其中东河塘组和甘木里克组地质时代为晚泥盆世，巴楚组地质时代为早石炭世杜内早中期，卡拉沙依组地质时代为晚杜内中期至巴什基尔期，小海子组地层时代为巴什基尔末期至莫斯科早期。岩石类型有碎屑岩和碳酸盐岩，还有膏盐岩，并夹薄层火山碎屑岩。沉积相主要为海陆过渡相组合，包括河流、三角洲、滨岸、浅海、碳酸盐岩台地、台地边缘6种相和12种亚相及33种微相。晚泥盆世东河塘期至石炭纪发生过4次较大的海侵，海侵范围由下而上逐渐增大，至晚石炭世小海子期海侵规模最大。东河塘期开始海侵，海水由西而东侵入，此时周缘碎屑物质供应充分，主要为无障壁海岸和障壁海岸沉积，西南缘为浅海相沉积。巴楚期晚期，海侵范围进一步扩大，物源向北或北东方向退却，陆源碎屑物质注入急剧减少，形成了一套富含生屑的碳酸盐岩地层，发育了开阔台地和局限台地亚相沉积。卡拉沙依期中期海侵规模比巴楚期更大，海水深度加大，西部为开阔台地亚相沉积，其余地区为局限台地亚相沉积。卡拉沙依期晚期和小海子期海侵达最大，向东扩展，大部分地区为开阔台地亚相沉积，东部地区为局限台地亚相沉积，塔北大部分地区缺失。     

基于被动微波遥感的青藏高原雪深反演及其结果评价

采用修正的张氏雪深反演算法，用ＳＳＭ／Ｉ３７ＧＨz和19GHz水平极化亮温值计算了青藏高原及其毗邻地区的积雪深度，对其精度进行了评价，并对误差来源进行了分析，结果显示，此算法能够较好地反映研究区的雪深分布，但局部地区误差较大，总体上雪深被高估，其误差主要来源于冻土，深霜层，植被以及雪层中液态水含量，雪粒的形状和粒径的变化带来的影响，SSM／I数据较低的分辨率和研究区复杂的地形使反演的雪深与观测的雪深缺少可比性，给精度的评价带来影响。     

Developing a bivariate spatial association measure: An integration of Pearson's r and Moran's I

 This research is concerned with developing a bivariate spatial association measure or spatial correlation coefficient, which is intended to capture spatial association among observations in terms of their point-to-point relationships across two spatial patterns. The need for parameterization of the bivariate spatial dependence is precipitated by the realization that aspatial bivariate association measures, such as Pearson's correlation coefficient, do not recognize spatial distributional aspects of data sets. This study devises an L statistic by integrating Pearson's r as an aspatial bivariate association measure and Moran's I as a univariate spatial association measure. The concept of a spatial smoothing scalar (SSS) plays a pivotal role in this task. Received: 07 November 2000 / Accepted: 02 August 2001     

雷达卫星SAR与防卫气象卫星SSM/I对渤海海冰的观测研究

用雷达卫星(RADARSAT)合成孔径雷达(SAR)和防卫气象卫星(DMSP)特别微波成像辐射计(SSM/I)在1999年1月23日同一天对中国渤海区域海冰的观测数据，进行了主动SAR与被动SSM/I的组合研究.用一层海冰电磁散射辐射的建模与数值模拟，分析了中纬度渤海沿岸海冰的特征性变化，提出用SSM/I辐射亮度温度的散射指数、极化指数、极化比率来识别渤海海冰；用RADARSAT高分辨率SAR数据(水平极化后向散射系数)对渤海海冰物理特征进行识别与分类.这些特征指数在时间与空间尺度上的相关变化可有效地应用于渤海海冰的监察.     

The initial subevent of the 1994 Northridge, California, earthquake: Is earthquake size predictable?

We examine the initial subevent (ISE) of the M 6.7, 1994 Northridge, California, earthquake in order to discriminate between two end-member rupture initiation models: the preslip and cascade models. Final earthquake size may be predictable from an ISE's seismic signature in the preslip model but not in the cascade model. In the cascade model ISEs are simply small earthquakes that can be described as purely dynamic ruptures. In this model a large earthquake is triggered by smaller earthquakes; there is no size scaling between triggering and triggered events and a variety of stress transfer mechanisms are possible. Alternatively, in the preslip model, a large earthquake nucleates as an aseismically slipping patch in which the patch dimension grows and scales with the earthquake's ultimate size; the byproduct of this loading process is the ISE. In this model, the duration of the ISE signal scales with the ultimate size of the earthquake, suggesting that nucleation and earthquake size are determined by a more predictable, measurable, and organized process. To distinguish between these two end-member models we use short period seismograms recorded by the Southern California Seismic Network. We address questions regarding the similarity in hypocenter locations and focal mechanisms of the ISE and the mainshock. We also compare the ISE's waveform characteristics to those of small earthquakes and to the beginnings of earthquakes with a range of magnitudes. We find that the focal mechanisms of the ISE and mainshock are indistinguishable, and both events may have nucleated on and ruptured the same fault plane. These results satisfy the requirements for both models and thus do not discriminate between them. However, further tests show the ISE's waveform characteristics are similar to those of typical small earthquakes in the vicinity and more importantly, do not scale with the mainshock magnitude. These results are more consistent with the cascade model.     

Differences Between Mode I and Mode II Crack Propagation

Although mode I and mode II crack propagation show many similarities, in particular when analysed by linear elastic fracture mechanics, they differ significantly in the micro-structural behaviour. These differences, which are clearly noticeable in the fracture surface morphology, lead to fundamental differences in the macroscopic behaviour. Thus, mode II crack expansion under remote loading, appears to obey micro-structural scaling laws, implying that the dimensions of the process region stay essentially constant during crack expansion, rather than increasing with crack length. Therefore, expanding mode II cracks can almost reach the Rayleigh velocity, and actually also intersonic velocities. An expanding mode I crack, on the other hand, seems to obey continuum scaling laws, implying that the dimensions of the process region increase in proportion to crack length, leading to self-similar crack expansion at a velocity significantly below the Rayleigh speed and dependent on the remote load.     

东亚南北地震带大震活动性研究

根据中国南北地震带与青藏-印尼“歹”字型构造带在成因上的联系，提出东亚南北地震带的观点，认为该地震带包含蒙古、中国西部、缅甸和印尼苏门答腊地区。研究了该带大地震活动的同步性、主体活动区的有序转移、大地震之间的多次相关迁移与重复等特征，并划分出了该带的5个大震活跃幕：1887-1912年、1913-1937年、1938-1957年、1958-1976年、1977-2005年。苏门答腊2004年12月26日8．7级和2005年3月29日8．5级巨震标志着该地震带最近一次以主体活动区南移到苏门答腊为特征的活跃时段即将结束。尽管未来一、两年内地震带的中部存在发生7级地震的有利时段，但结合强震图像异常指标反映的孕震状况分析，未来7级地震危险区尚不明朗。     

冀北红旗营子杂岩的锆石、独居石年代学及地质意义

较为详细的SHRIMP、LA-ICPMS锆石U-pb年代学和独居石电子探针Th-U-b化学法定年揭示，隆化-山地块的石英闪长质片麻岩和石榴黑云二长花岗质片麻岩分别形成于2484Ma和2180Ma，同时存在3164～2553Ma的锆石记录和约1854Ma的变质改造事件；细粒二长花岗岩形成于413Ma，独居石内核记录了约628Ma的继承年龄。凤山-宁地块的钾长花岗质糜棱片麻岩、角闪黑云石英闪长质片麻岩和黑云母二长花岗岩分别形成于1876Ma、1838Ma和1810Ma，其中存在2042-1904Ma的捕获锆石，遭受了1756Ma、1694Ma和313．5Ma的多期改造，其中晚古生代的构造-浆-质事件的改造尤为强烈。赤城-礼地块的角闪黑云花岗闪长质片麻岩分别形成于2535Ma和2529-2480Ma，石榴英云闪长质片麻岩和石榴黑云斜长变粒岩分别形成于1871Ma和1841Ma，发现有约2602Ma的继承锆石，并记录了从古元古代到晚古生代多阶段的改造事件，尤其清楚地记录了343-320Ma的地质事件。结合前人的年代学资料，综合分析上述地质年代学的特征，认为红旗营子杂岩从东到西可能由不同来源的微陆块组成，这些微陆块都经历了晚古生代的构造-岩浆-变质事件，可能在古生代晚期才与华北克拉通北缘拼贴。     

伊春地区晚印支期I型花岗岩带特征及其构造背景

晚印支期花岗岩岩石类型主要为一套含角闪石黑云母二长花岗岩及含黑云母正长花岗岩，岩石中暗色闪长质岩包体发育较普遍，富含角闪石及镁质黑云母，副矿物以榍石、磁铁矿、磷灰石常见，Al2O3／（Na2O十K2O＋CaO）〈1．1，显示出I型花岗岩特征。利用岩石矿物组合、岩石化学特征判别其产于碰撞后构造环境，认为造山后伸展体制是这期花岗岩形成的重要原因。岩石（^87 Sr／^86 Sr）；及δEu值反映其源区为壳幔过渡区，氧同位素（δ^18 O）测定值在5．5‰-10‰之间，具壳幔混源的特点，表明岩石来源于下地壳或壳幔过渡部分，与下地壳的部分熔融或壳幔过渡区部分熔融作用有关。     

Do stratocumulus clouds detrain? FIRE I data revisited

Analyses of aircraft observations of the stratocumulus-topped boundary layer during the First ISCCP (International Satellite Cloud Climatology Project) Regional Experiment (FIRE I) show the frequent presence of clear, but relatively moist, air patches near the stratocumulus cloud-top interface. A conditional sampling of measurements in these clear air patches shows that their thermodynamic properties do more resemble boundary-layer air characteristics than those of free troposphere air. From an aircraft leg through cloud tops it is demonstrated that turbulent mixing across the cloud-top interface can lead to the local dissipation of the cloud top. Analogous to the terminology used for shallow cumulus parameterizations this process can be considered as detrainment, with which we mean that after a mixing event across the cloud-top boundaries, mixed unsaturated parcels become part of the clear environment of the cloud.