根据i—f—j模式估计山西平陆地区的长期强震潜势

山西省平陆地区位于山西地震带南端，为了分析该地区未来的长期强需求潜势，本较系统地分析当地的破坏性地震及１５００年以来的有地震地震资料，并进一步应用中国在陆特征的地震轮回模式及其复发时间概率模型估算法当前特征地震轮回的平均时间间隔，以及从１９９５年起未来百年内复发强震的概率，结果表明：未来１００年来该地区复发强震的危险性很高，未来５０年内复发强震的危险性也不能排除。     

1997年4月6日、11日、16日新疆伽师4次6.3～6.6级地震烈度分布及震害特征

1997年4月6日、11日、16日新疆伽师继1月21日和3月1日3次6级以上地震之后又连续发生了4次6级以上地震。极震区烈度达Ⅷ度．极震区内的英买里乡所有Ⅰ类房屋几乎全部倒塌或严重破坏；江巴孜乡、和夏阿瓦提乡、克孜勒苏乡和巴仁镇的大部分房屋倒塌或严重破坏。在地下水位高、土质松散地区出现大面积喷水冒砂与地裂缝。根据震害评估与宏观考察资料，介绍了各烈度区的震害特征。     

唐山地震的超晚期强余震估计

根据华北历史地震的重复性和免疫性，认为在唐山周围８５ｋｍ，２００年内，对６级地震具有一定的免疫性；在研究了唐山地震序列自身的衰减规律后，认为在今后几十几强余震的最大活动水平为５级，发生６级以上土地震的可能性很小。     

地下水宏观异常与强震临震预报

阐述了如何利用地下水宏观异常作强烈地震的临震预报，详细叙述了利用地下水宏观异常预报地震三要素的方法。     

中强地震前油井动态异常机理研究

在分析油井映震特征的基础上，着重对油井动态异常的形成机理进行了研究。认为：映震灵敏井孔的空间分布主要受应力易于集中的构造条件的控制，特别是断层的又汇处、转折端和断裂带，这是与其他流体观测项目的相同之处；在本研究中，首次提出了油井动态前兆异常形成的三种力学过程，即岩土力学过程、水动力学过程和气体动力学过程以及油井特有的二种”放大”作用（变径和气体膨胀）的观点；解释了油井动态震前多为正异常的力学机制。     

大陆地震的动力学模型研究

应用非线性动力学模型，以大陆构造构体为参照对象，对大陆地震的成组孕育和发生过程进行模拟研究，通过对６×８弹簧－滑块－阻尼器组合单元非线性动力学模型的理论计算及其结果的分析，得到了一系列与实际地震较类似的人工地震图像，如模型中的地震活动在时间上有轮回怀，在地点上有条带性，并在不同轮回中有条过移的现象。模型中应力变化十分复杂，但仍能为预测地震提供概略性的信息。     

Modelling the compliance of crustal rock—II. Response to temporal changes before earthquakes

There have been several claims that seismic shear waves respond to changes in stress before earthquakes. The companion paper develops a stress-sensitive model (APE) for the behaviour of low-porosity low-permeability crystalline rocks containing pervasive distributions of fluid-filled intergranular microcracks, and this paper uses APE to model the behaviour before earthquakes. Modelling with APE shows that the microgeometry and statistics of distributions of such fluid-filled microcracks respond almost immediately to changes in stress, and that the behaviour can be monitored by analysing seismic shear-wave splitting. The physical reasons for the coupling between shear-wave splitting and differential stress are discussed.
In this paper, we extend the model by using percolation theory to show that large crack densities are limited at the grain-scale level by the percolation threshold at which interacting crack clusters lead to pronounced increases in rock-matrix permeability. In the simplest formulation, the modelling is dimensionless and almost entirely constrained without free parameters. Nevertheless, APE modelling of the evolution of fluid-saturated rocks under stress reproduces the observed fracture criticality and the narrow range of shear-wave azimuthal anisotropy in crustal rocks. It also reproduces the behaviour of temporal variations in shear-wave splitting observed before and after the 1986, M = 6, North Palm Springs earthquake, Southern California, and several other smaller earthquakes.
The agreement of APE modelling with a wide range of observations confirms that fluid-saturated crystalline rocks are stress-sensitive and respond to changes in stress by critical fluid-rock interactions at the microscale level. This means that the effects of changes in stress and other parameters can be numerically modelled and monitored by appropriate observations of seismic shear waves.     

The Zihuatanejo, Mexico, earthquake of 1994 December 10 (M= 6.6): source characteristics and tectonic implications

An analysis of the Zihuatanejo, Mexico, earthquake of 1994 December 10 ( M = 6.6), based on teleseismic and near-source data, shows that it was a normal-faulting, intermediate-depth ( H = 50 ± 5 km) event. It was located about 30 km inland, within the subducted Cocos plate. The preferred fault plane has an azimuth of 130°, a dip of 79° and a rake of −86°. The rupture consisted of two subevents which were separated in time by about 2 s, with the second subevent occurring downdip of the first. The measured stress drop was relatively high, requiring a Δσ of about a kilobar to explain the high-frequency level of the near-source spectra. A rough estimate of the thickness of the seismogenic part of the oceanic lithosphere below Zihuatanejo, based on the depth and the rupture extent of this event, is 40 km.
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event.