日本至中国东北区域构造应力场分布与Benioff带的形态关系研究

收集2 291个来源于NIED F-net宽频带地震台网中心M_W≥3.0地震的震源机制解,采用MSATSI构造应力反演方法,得到反映应力相对大小的R值的量θ和3个主应力轴的方位角与倾伏角,同时反演出每个网格的极射赤平投影P、T轴。以3D应力反演为导向,采用矩阵网格分区的方法,以纬度、经度、深度为坐标,将发生在每一区域的震源机制解投射到相应的矩阵区中,并反演出每个矩阵网格点的应力场变化及分布情况。反演结果表明,与板块交接的浅部区域不仅受到太平洋板块的挤压俯冲,同时也受北美板块的斜插作用;东北区域的深震为Benioff带俯冲作用的结果。     

Toward policy integration: Assessing carbon capture and storage policies in Japan and Norway

The objective of this paper is to develop independent and systematic criteria for assessing CCS policy in terms of its level of policy integration. We believe that we should assess CCS policy in terms of the distance to an ideal integrated CCS policy in order to keep track of its trajectory toward sustainable development. After reviewing the existing literature of environmental policy integration, an assessment framework for integrated CCS policy is developed based on Arild Underdal's notion of ‘integrated policy’ then, its usefulness is demonstrated by applying it to CCS policies in Japan and Norway. In the final part, we summarize the findings of the cases and conclude with some observations regarding explanatory factors of the difference in terms of the achieved level of policy integration between Japan and Norway's CCS policies, and some policy implications derived from the analysis based on the framework.     

2011年6—8月T639、ECMWF及日本模式中期预报性能检验

为更好地应用数值模式中期预报产品,对2011年6—8月T639模式进行天气学检验,并与ECMWF、日本模式进行了对比分析。结果表明：三家模式均对亚洲中高纬环流形势的调整和演变具有较好的预报性能。综合来看,ECMWF模式对大尺度环流形势、影响天气系统及要素的预报最接近实况;日本模式和T639模式稍差,稳定性也不如ECMWF模式。对1109号台风梅花（MUIFA）的路径及强度预报,三家模式的预报效果均不理想,T639模式对＂梅花＂登陆后的预报与零场较接近,而ECMWF模式及日本模式预报相对较差。     

宁波台动水位与垂直摆对印尼8.9和日本9.0级地震的同震响应

分析认为宁波台ZK03井动水位与VS垂直摆倾斜仪出现的异常可能是印尼8.9和日本9.0级地震的同震响应.印尼8.9级地震后,动水位表现为地震波引起的脉冲和阶跃变化并抬高水位.垂直摆表现为形变波引起的脉冲和阶跃变化,EW向最大幅度约为408.328×10-3"的脉冲式向E振荡波,并向W出现阶跃变化;NS向最大幅度约为29...     

日本海域9.0级地震的深刻启示与防灾减灾对策

从日本成功的防震减灾经验中受到启示,通过详细分析日本的救灾体系、防灾减灾教育、抗震标准、灾区人口密度和应对福岛核电站问题的相关措施,提出目前我国在这些方面存在的主要问题及应对策略。     

Geological comparative studies of Japan Arc System and Kyushu-Palau Arc

Based on the published data of structure geology,geochronology,petrology and isotope geochemistry,the authors of this paper have conducted studies on the tectonic evolution history of Japan arc system and Kyushu-Palau ridge(KPR) . The studies show that the initial Japan arc system was resulted from the subduction of ancient Pacific plate beneath Eurasian Plate in Permian. It was part of an Andean-type continental volcanic arc which occurred in the offshore in the east of Asian during late Mesozoic era. The formation of tertiary back-arc basin(Japan Sea) resulted in the fundamental tectonic framework of the present arc system. Since Quaternary the system has been lying at E-W compression tectonic setting due to the eastward subduction of Amur Plate. It is expected that Japan arc system will be juxtaposed with Asian continent,which is similar to the present Taiwan arc system. The origin of Philippine Sea Plate(PSP) is still in debate. Some studies argued that it is a trapped oceanic crust segment,while the others insisted that it is a back-arc basin accompanied with ancient IBM arc. However,it is all agreed that the tectonic evolution of PSP started since 50 Ma,i.e.,PSP has drifted from the site around equator at 50 Ma to the present site,and the subduction of PSP along Nankai trough-Ryukyu Trench beneath the Japan arc system during 6-2 Ma led to the formation of the present Ryukyu arc system. Of the PSP,the KPR has been found with the oldest rocks formed at 38 Ma. Combining with its geochemical characteristics of oceanic arc tholeiite,it is suggested that KPR is an intraoceanic volcanic arc,more specifically,a relic arc(i.e.,rear arc of the ancient IBM) after rifting of ancient IBM. In addition,Amami-Daito province is of arc tectonic affinity,but has been affected by mantle plume. Therefore,based on their respective tectonic evolution history and geochemical characteristics of rock samples,it is inferred that there is no genetic relationship between Japan arc system and KPR. It is noted that rocks reflecting continental crust basement feature have been collected on the northern tip of KPR,which may be related to the process of KPR accreting on Japan arc,but the arc-continent accretion process are still at initial stage of modern continental crust accretion model. However,due to the scarcity of data of the northern tip of KPR,crustal structure of this location and its adjacent Nankai trough need to be further constrained by geophysical studies in the future.     

Structural-stratigraphic control on the Umitaka Spur gas hydrates of Joetsu Basin in the eastern margin of Japan Sea

Integrated geological, geochemical, and geophysical exploration since 2004 has identified massive accumulation of gas hydrate associated with active methane seeps on the Umitaka Spur, located in the Joetsu Basin on the eastern margin of Japan Sea. Umitaka Spur is an asymmetric anticline formed along an incipient subduction zone that extends throughout the western side of the Japanese island-arc system. Seismic surveys recognized chimney structures that seem strongly controlled by a complex anticlinal axial fault system, and exhibit high seismic amplitudes with apparent pull-up structures, probably due to massive and dense accumulation of gas hydrate. Bottom simulating reflectors are widely developed, in particular within gas chimneys and in the gently dipping eastern flank of the anticline, where debris can store gas hydrates that may represent a potential natural gas resource. The axial fault system, the shape of the anticline, and the carrier beds induce thermogenic gas migration to the top of the structure, and supply gas to the gas hydrate stability zone. Gas reaching the seafloor produces strong seepages and giant plumes in the sea water column.     

日本海主要海峡体积输运的季节变化特征

利用变分资料同化技术对P矢量方法进行优化处理,并采用此优化后的P矢量方法优化计算了日本海环流和日本海主要海峡的体积输运.日本海的主要环流系统,比如对马暖流(TWC)及其分支,东朝鲜暖流(EKWC)和日本近岸分支(JNB),极地锋海流(PFC),和日本海中的反气旋式涡,都能够被很好地一一反映出来.另外,优化后的P矢量方法...     

帕米尔东北侧地壳结构研究

1998年在帕米尔东北侧伽师及其周边地区完成了两条深地震宽角反射/折射剖面. 结果表明,西昆仑、塔里木和天山在地壳速度结构、构造特征上显示出较大差异. 塔里木块体具有稳定地块的地壳结构特征,地壳平均速度较高(6.5km/s). 向南进入西昆仑,地壳明显增厚,厚度可达0km左右,且地壳平均速度偏低(6.0-6.2km/s),偏低的地壳平均速度主要来源于相对低速度的下地壳结构,反映了西昆仑褶皱系下地壳介质的特征. 向北进入天山后,地壳同样明显增厚,但增厚的程度低于西昆仑下,约为50-55km. 天山地壳同样具有明显低的平均速度(6.2km/s),显示了天山地壳相对"软"的特征,但天山地壳偏低的平均速度来源于广泛分布于中地壳的低速度层和速度偏低的下地壳. 在印度块体向北强烈推挤的作用下,该区地壳遭受强烈的不均匀变形,塔里木块体向南插入西昆仑下,向北插入天山下,形成了该区强烈地震频繁发生的深部构造环境.     

Geochronological Records of Oil-Gas Accumulations in the Permian Reservoirs of the Northeastern Ordos Basin

Geochronology of oil-gas accumulation （OGA） is a challenging subject of petroleum geology in multi-cycle superimposed basins.By K-Ar dating of authigenic illite （AI） and fluid inclusion （FI） analysis combined with apatite fission track （AFT） thermal modeling,a case study of constraining the OGA times of the Permian reservoirs in northeast Ordos basin （NOB） has been conducted in this paper.AI dating of the Permian oil-gas-bearing sandstone core-samples shows a wide time domain of 178-108 Ma.The distribution of the AI ages presents 2-stage primary OGA processes in the Permian reservoirs,which developed in the time domains of 175-155 Ma and 145-115 Ma with 2-peak ages of 165 Ma and 130 Ma,respectively.The FI temperature peaks of the samples and their projected ages on the AFT thermal path not only present two groups with a low and a high peak temperatures in ranges of 90-78℃ and 125-118℃,respectively corresponding to 2-stage primary OGA processes of 162-153 Ma and 140-128 Ma in the Permian reservoirs,but also appear a medium temperature group with the peak of 98℃ in agreement with a secondary OGA process of c.～30 Ma in the Upper Permian reservoirs.The integrated analysis of the AI and FI ages and the tectono-thermal evolution reveals that the Permian reservoirs in the NOB experienced at least 2-stage primary OGA processes of 165-153 Ma and 140-128 Ma in agreement with the subsidence thermal process of the Mid-Early Jurassic and the tectono-thermal event of the Early Cretaceous.Then,the Upper Permian reservoirs further experienced at least 1-stage secondary OGA process of c.～30 Ma in coincidence with a critical tectonic conversion between the slow and the rapid uplift processes from the Late Cretaceous to Neogene.