龙门山地区上地壳的拱曲冲断作用及其深部动力学机制探讨

地形地貌与区域地质构造分析揭示,龙门山一带上地壳的汇聚作用表现为松潘－甘孜块体东缘的褶皱拱曲与扬子克拉通西缘的高角度叠瓦状冲断,近地表形成了一个巨大的北东向展布的拱曲冲断构造带。松潘－甘孜块体东缘的拱起预示着可能有来自深部的顶托。人工地震测深得到的地壳P波速度结构剖面也揭示,松潘－甘孜块体东缘上地壳普遍有较大范围的拱起,上地壳底部的低速层也同步抬升,其隆起范围与近地表的拱曲冲断带比较一致,说明很可能存在来自中下地壳的上拱作用。面波层析成像揭示松潘－甘孜块体与扬子克拉通具有截然不同的壳幔结构,扬子克拉通速度较高,且不存在低速夹层; 而松潘－甘孜块体速度偏低,地壳明显增厚,且下地壳及地幔上部存在S波低速层,地幔低速层上涌至壳幔过渡带,甚至侵入四川盆地之下,且上涌的范围与地表拱曲冲断带恰巧吻合,推测地幔盖层与下地壳塑性软弱物质的局部上涌促成了上地壳的拱曲。2008年汶川8.0级地震发生在拱曲冲断带中段,最大同震位移场位于龙门山拱曲冲断带及四川盆地西缘,揭示松潘－甘孜块体东缘的拱曲与扬子克拉通西缘的冲断共同受制于两大块体最新的汇聚作用。认为龙门山拱曲冲断构造带是陆内汇聚与壳幔通道流上涌联合作用的结果。爆破地震测深与地震层析成像不显示陆内俯冲图像,两大地块之间中地壳以下似为一近直立的汇聚带,这一构造格架将物质迁移主要限于垂向上,有利于龙门山保持大地形高差,而四川盆地一侧则因难以形成大的构造负载,前陆凹陷作用不显著。     

The Deep Geophysical Structure of the Middle Section of the Longmen Mountains Tectonic Belt and its Relation to the Wenchuan Earthquake

Investigation of the deep geophysical structure of the Longmen Mountains tectonic belt and its relation to the Wenchuan Earthquake is important for the study of earthquakes. By using magnetotelluric sounding profiles of the Luqu–Zhongjiang and Anxian–Suining; seismic sounding profiles of the Sichuan Maowen–Chongqing Gongtan, the Qinghai Huashi Gorge–Sichuan Jianyang, and the Batang–Zizhong; and magnetogravimetric data of the Longmen Mountains region, the deep geophysical structure of the Songpan–Ganzi block, the western Sichuan foreland basin, and the Longmen Mountains tectonic belt and their relation was discussed. The eastward extrusion of the Qinghai–Tibet Plateau thrusts the Songpan–Ganzi block upon the Yangtze block, which obstructs the eastward movement of the Qinghai–Tibet Plateau. The Maoxian–Wenchuan, Beichuan–Yingxiu, and Anxian–Guanxian faults of the Longmen Mountains fault belt dip to northwest with different dip angles and gradually converge in the deeper parts. Geophysical structure suggests that an intracrustal low-velocity, low-resistivity, and high-conductivity layer is common between the middle and upper crust west of the Longmen Mountains tectonic belt but not in the upper Yangtze block. The Sichuan Basin has a thick low-resistance sedimentary layer on a stable high-resistance basement; moreover, there are secondary paleohighs and depression structures at the lower part of the western Sichuan foreland basin with characteristic of high magnetic anomalies, whereas the Songpan–Ganzi block has a high resisitivity cover of upper crust and continues to a low-resistance layer. Considering the Longmen Mountains tectonic belt as the boundary, there are Bouguer gravity anomalies of "one belt between two zones." Thus, we infer that there is a corresponding relation between the inferred crystalline basement of the Songpan block and the underlying basin basement of the Longmen Mountains fault belt. Furthermore, there may be an extensive ancient Yangtze block, which is west of the Ruoergai block. In addition, the crust–mantle ductile shear zone under the Longmen Mountains tectonic belt is the main fault, whereas the Beichuan–Yingxiu and Anxian–Guanxian faults at the surface are earthquake faults. The Wenchuan Ms 8.0 earthquake might be attributed to the collision of the Yangtze block and the Qinghai–Tibet Plateau. The eastward obduction of the eastern edge of the Qinghai–Tibet Plateau and eastward subduction of its deeper part under the influence of the collision of the Indian, Pacific, and Philippine Plates with the Eurasia Plate might have caused the Longmen Mountains tectonic belt to cut the Moho and extend to the middle and upper crust; thus, creating high stress concentration and rapid energy release zone.     

长江中下游及其邻区深部地球物理背景与含金夕卡岩矿床的分布

长江中下游地区是我国重要的铁铜矿产基地。近十年来,我国所发现的含金夕卡岩矿床和铜伴生金夕卡岩矿床也主要产在长江中下游地区。作者借助12条大地电磁测深剖面、5条地震剖面、层析成像速度结构资料、重磁场等区域的和深部的地球物理资料进行综合对比研究,给出长江中下游及其邻区的三维深部构造格架及其与含金夕卡岩矿床和铜伴生金夕卡岩矿床的分布关系。作者认为,上地幔隆起带(岩石圈地幔减薄带)、上地幔异常区(相对低速区)、壳内高导层隆起带、深断裂(岩石圈剪切带)、地壳上地幔不均匀性块体的边缘、重力高反映的基底隆起区、跳跃磁场反映的岩浆岩带和构造交汇处等诸多因素的共同作用控制着含金夕卡岩矿床和铜伴生金夕卡岩矿床的分布。     

长江中下游成矿带及邻区地壳结构——MASH成矿过程的P波接收函数成像证据？

利用长江中下游成矿带多学科深部探测剖面于2009年11月至2011年3月间采集的天然地震数据,通过天然地震接收函数成像等分析研究,得到了研究区地壳和上地幔结构的清晰图像。接收函数成像结果显示研究区内Moho面深度存在着明显的起伏变化,在长江中下游成矿带(指剖面穿过的长江中下游成矿带宁芜矿集区,下同)下方存在着"幔隆构造"。在剖面东南端(即扬子克拉通北缘),Moho面相对稳定,深度约为30km;在茅山和江南断裂附近,Moho面存在上下起伏现象;在剖面中部或宁芜矿集区下方,Moho面存在明显隆起,深度只有28km;在郯庐断裂带下方,Moho面明显加深,深度达到36km;进一步向北到华北地台南缘,Moho面深度逐渐恢复到了32km左右的平均深度水平。其次,我们在接收函数成像结果中发现,长江中下游成矿带与其周边下地壳结构存在着明显的差异,成矿带的下地壳具有显著的地震波方位各向异性。扬子克拉通北缘的下地壳呈高速的近水平状结构,地震波各向异性特征不明显;与此相比,长江中下游成矿带的下地壳虽然也呈近水平状结构特征,但是,对于沿成矿带走向方向传播的地震波,其下地壳具有高速特征,而对于垂直于成矿带走向方向上传播的地震波,其下地壳却又表现为低速特征,这意味着成矿带的下地壳存在着平行于成矿带走向(即近北东—南西)方向的地震波各向异性,我们解释其是下地壳熔融并沿成矿带走向水平流动导致矿物晶体定向排列的结果。最后,在郯庐断裂以西的华北地台南缘观测到一条从上地壳延伸到中下地壳的南南东向倾斜的转换震相,我们推测它可能是合肥盆地内地壳伸展构造的反映。此外,我们发现接收函数成像结果中观测到的"幔隆构造"与远震P波层析成像结果在成矿带下方150km深度上显示的上地幔低速异常(江国明等,另文发表)存在着良好的对应关系,我们解释它们是软流圈物质上涌的遗迹。综合天然地震接收函数成像、远震P波层析成像和前人关于岩浆岩等方面的研究成果,我们认为长江中下游成矿带现今的下地壳可能是中生代发生成矿作用的多级岩浆房系统的一部分,成矿带的形成可能是类似MASH过程的产物。首先,软流圈物质上涌导致了长江中下游成矿带及其周边拉张环境的形成,在其上部地壳中形成了一系列伸展构造;然后,软流圈物质通过底侵进入长江中下游成矿带的原下地壳并与原下地壳物质发生同化作用,形成类埃达克质岩浆;接着,类埃达克质岩浆沿着伸展、拆离构造上升到地壳浅部形成不同层次的岩浆房和侵入岩体,并与围岩作用形成矿床。     

长江中下游地区中生代陆内构造作用与成因分析

长江中下游地区多期构造叠加、复合联合作用明显,中生代以来地壳运动频繁、构造活动强烈,地表为桐柏-大别造山带,九岭-江南隆起带,其间为对冲样式构造组合的长江复合构造带。大别造山带前陆深地震反射剖面揭示长江中下游深部为“双鳄鱼构造”状态,大量前陆断褶带的物质被掩盖在大别造山带之下,岩片叠置、断裂交错的镶嵌构造极为发育,下地壳切过莫霍面向北俯冲,是后期岩浆的活动通道和就位空间。综合地球物理剖面揭示下扬子地区南北岩石圈结构差异明显,上地壳南北对冲构造发育;下地壳为向北倾斜的构造带,北部仍向南逆冲,南部切过莫霍面向北俯冲。长江中下游地区上述构造的形成受控于长江陆内异化带的作用,该带是一条陆内岩石圈规模的向北倾斜的破裂带,发生在中国大陆形成之后,不受早期板块界线的控制,是岩石圈规模的大陆异化、物质重建、结构重组的产物;主要结构特征为上地壳对冲式逆断层组合,中地壳为水平流变层,下地壳切过莫霍面由南向北俯冲;形成过程是印支晚期-燕山早期中国陆内近南北向挤压,地壳破碎,岩石圈加厚;燕山晚期大规模伸展拉张,岩浆活动,壳幔混熔。特殊成因机制和演化过程的综合效应是长江陆内异化带的地质内涵。深部物质沿长江陆内异化带上升,在上部地壳内多期叠加构成的构造格架中就位,岩体形态在深部近东西向呈带状,中部状态复杂,浅表受控于多种构造组合形式,见空即灌。     

Lithospheric structure and dynamic processes of the Tianshan orogenic belt and the Junggar basin

Located at the center of the Eurasian continent and accommodating as much as 44% of the present crustal shortening between India and Siberia, the Tianshan orogenic belt (TOB) is one of the youngest (<20 Ma) and highest (elevation>7000 m) orogenic belts in the world. It provides a natural laboratory for examining the processes of intracontinental deformation. In recent years, wide angle seismic reflection/refraction profiling and magnetotelluric sounding surveys have been carried out along a geoscience transect which extends northeastward from Xayar at the northern margin of the Tarim basin (TB), through the Tianshan orogenic belt and the Junggar basin (JB), to Burjing at the southern piedmont of the Altay Mountain. We have also obtained the 2D density structure of the crust and upper mantle of this area by using the Bouguer anomaly data of Northwestern Xinjiang. With these surveys, we attempt to image the 2D velocity and the 2D electric structure of the crust and upper mantle beneath the Tianshan orogenic belt and the Junggar basin. In order to obtain the small-scale structure of the crust–mantle transitional zone of the study area, the wavelet transform method is applied to the seismic wide angle reflection/refraction data. Combining our survey results with heat flow and other geological data, we propose a model that interprets the deep processes beneath the Tianshan orogenic belt and the Junggar basin.Located between the Tarim basin and the Junggar basin, the Tianshan orogenic belt is a block with relatively low velocity, low density, and partially high resistivity. It is tectonically a shortening zone under lateral compression. A detachment exists in the upper crust at the northern margin of the Tarim basin. Its lower part of the upper crust intruded into the lower part of the upper and the middle crust of the Tianshan, near the Korla fault; its middle crust intruded into the lower crust of the Tianshan; and its lower crust and lithospheric mantle subducted into the upper mantle of the Tianshan. In these processes, the mass of the lower crust of the Tarim basin was carried down to the upper mantle beneath the Tianshan, forming a 20-km-thick complex crust–mantle transitional zone composed of seven thin layers with a lower than average velocity. The thrusting and folding of the sedimentary cover, the intrusive layer in the upper and middle crust, and the mass added by the subduction of the Tarim basin into the upper mantle of the Tianshan are probably responsible for the crustal thickening of the Tianshan. Due to the important mass deficiency in the crust and the upper mantle of the Tianshan, buoyancy must occur and lead to rapid ascent of the Tianshan.The episodic tectonic uplift of the Tianshan and tectonic subsidence of the Junggar basin are closely related to the evolution of the Paleozoic, Mesozoic, and Cenozoic Tethys.     

川黔湘构造带构造样式及深部动力学制约

川黔湘构造带可划分为4个不同的构造带,其中雪峰山构造带地理位置特殊,恰位于华南块体南北向重力梯度带上,两侧岩石圈厚度差异显著,其成因机制历来是争论的焦点。雪峰山构造带基底是一个花状结构,与川黔隔槽式褶皱带构成一个整体,为一个厚皮结构。雪峰山基底在沅麻盆地隆升最高,表现为压扭性构造特点。参考深反射剖面,绘制了研究区浅层与深部结构地质剖面。板块受挤压,中、上地壳与下地壳存在不同的耦合方式,对此分析了研究区下地壳的变形过程。雪峰山下地壳向下存在对冲,形成山根,但并没有俯冲至地幔。随地壳加厚,岩石圈发生弯曲,下地壳与上地幔存在瑞利泰勒不稳定性,并下沉至软流圈地幔。晚中生代,伸展背景下的软流圈上涌使雪峰山以东岩石圈发生拆沉,致使两侧岩石圈厚度出现差异。     

峨眉山大火成岩省地壳密度结构及岩浆规模约束

峨眉山大火成岩省(ELIP)出露于扬子板块西缘,其形成以后经历了多期构造运动的破坏,掩盖了峨眉山玄武岩的原始分布状况,导致对ELIP岩浆活动规模的低估。近来一些研究者基于天然地震层析成像反演的研究认为ELIP出露区地壳不显示高速特征,据此推断ELIP岩浆活动规模有限,是下地壳拆沉作用而非地幔柱活动的产物。本文根据横穿峨眉山大火成岩省的丽江-清镇地震剖面所获地壳P波波速,依据P波波速与密度的线性关系计算ELIP内带核心、外围区域和中带、外带的地壳密度结构。结果显示:内带核心区域与中带相比,上地壳密度高79kg/m~3、下地壳上部和下部的密度值分别高出68 kg/m~3和101 kg/m~3;与外带相比,内带核心区域上地壳密度高92kg/m~3、下地壳上部和下部分别高出99 kg/m~3和126 kg/m~3。峨眉山地幔柱活动形成的镁铁质-超镁铁质深成岩在ELIP内带核心区域的侵位和堆积,是ELIP各带之间地壳密度存在显著差异的原因。根据ELIP不同区域的地壳密度差估算得到内带核心区域地壳内的高密度镁铁质侵入岩和超镁铁质侵入岩总体积约为(45~120)×10~4km~3。此结果与峨眉山玄武岩体积[(25~60)×10~4km~3]之和,给出ELIP岩浆活动的规模为(0.7~1.8)×10~6km~3。这一结果支持ELIP的形成与地幔柱活动有关的认识。     

安庆-贵池矿集区及邻区深部电性结构研究

长江中下游地区经历了多期次的地质构造演化具有丰富的矿产资源,对重要矿集区及其邻区的深部电性结构进行研究具有重要意义。通过对穿过安庆—贵池矿集区的一条宽频带大地电磁测深长剖面数据进行分频段以及分区反演,构建了覆盖大别造山带至下扬子地块东缘的二维电性结构模型。发现矿集区的深部电性结构与邻区的构造单元具有显著差异,大别造山带和江南隆起带与浙赣凹陷之间的地壳整体表现为高阻特征,而下扬子坳陷和江南隆起带之间存在岩石圈上地幔尺度的高导电异常体并且与地壳浅部的高导体相连。安庆—贵池矿集区的成矿机制主要为燕山期陆内俯冲以及早白垩时期的伸展作用,矿集区下地壳加厚、拆沉和上地壳丰富的断裂系统起到了重要的控矿作用。     

Joint Inversion of the 3D P Wave Velocity Structure of the Crust and Upper Mantle under the Southeastern Margin of the Tibetan Plateau Using Regional Earthquake and Teleseismic Data

The special seismic tectonic environment and frequent seismicity in the southeastern margin of the Qinghai–Tibet Plateau show that this area is an ideal location to study the present tectonic movement and background of strong earthquakes in mainland China and to predict future strong earthquake risk zones. Studies of the structural environment and physical characteristics of the deep structure in this area are helpful to explore deep dynamic effects and deformation field characteristics, to strengthen our understanding of the roles of anisotropy and tectonic deformation and to study the deep tectonic background of the seismic origin of the block's interior. In this paper, the three-dimensional(3D) P-wave velocity structure of the crust and upper mantle under the southeastern margin of the Qinghai–Tibet Plateau is obtained via observational data from 224 permanent seismic stations in the regional digital seismic network of Yunnan and Sichuan Provinces and from 356 mobile China seismic arrays in the southern section of the north–south seismic belt using a joint inversion method of the regional earthquake and teleseismic data. The results indicate that the spatial distribution of the P-wave velocity anomalies in the shallow upper crust is closely related to the surface geological structure, terrain and lithology. Baoxing and Kangding, with their basic volcanic rocks and volcanic clastic rocks, present obvious high-velocity anomalies. The Chengdu Basin shows low-velocity anomalies associated with the Quaternary sediments. The Xichang Mesozoic Basin and the Butuo Basin are characterised by lowvelocity anomalies related to very thick sedimentary layers. The upper and middle crust beneath the Chuan–Dian and Songpan–Ganzi Blocks has apparent lateral heterogeneities, including low-velocity zones of different sizes. There is a large range of low-velocity layers in the Songpan–Ganzi Block and the sub–block northwest of Sichuan Province, showing that the middle and lower crust is relatively weak. The Sichuan Basin, which is located in the western margin of the Yangtze platform, shows high-velocity characteristics. The results also reveal that there are continuous low-velocity layer distributions in the middle and lower crust of the Daliangshan Block and that the distribution direction of the low-velocity anomaly is nearly SN, which is consistent with the trend of the Daliangshan fault. The existence of the low-velocity layer in the crust also provides a deep source for the deep dynamic deformation and seismic activity of the Daliangshan Block and its boundary faults. The results of the 3D P-wave velocity structure show that an anomalous distribution of high-density, strong-magnetic and high-wave velocity exists inside the crust in the Panxi region. This is likely related to late Paleozoic mantle plume activity that led to a large number of mafic and ultra-mafic intrusions into the crust. In the crustal doming process, the massive intrusion of mantle-derived material enhanced the mechanical strength of the crustal medium. The P-wave velocity structure also revealed that the upper mantle contains a low-velocity layer at a depth of 80–120 km in the Panxi region. The existence of deep faults in the Panxi region, which provide conditions for transporting mantle thermal material into the crust, is the deep tectonic background forthe area's strong earthquake activity.     

大别造山带地壳泊松比结构与超高压变质带—来自宽角反射与近垂直反射剖面的启示

综合宽角反射、近垂直反射的探测结果和有关地质资料，对大别造山带地壳结构和超高压变质带研究显示：大别造山带地壳具有层块结构特征。沿安义－庄墓剖面，上地壳有7个弹性块体，中地壳有5个，下地壳有4个。扬子与华北地块的主缝合带是超高压变质带，扬子地块与大别造山带的现今分界线是与郯庐断裂相交的太湖－马庙断裂，磨子潭－晓天断裂是大别造山带的北界，北淮阳构造带呈楔状向下插入，它与华北地块的分界是肥中断裂。郯庐断裂在中、上地壳近于直立，下地壳向西倾斜。超高压变质带的厚度为5－7km，产状向北插入到北大别块体之下，折返过程是构造就位，不是大别山的均匀抬升，折返的主运动面是水吼－五河高温剪切带。     

长江中下游成矿带及典型矿集区深部结构探测——SinoProbe-03年度进展综述

大陆现今的地壳结构和物质组成是地壳经历了复杂的动力学演化过程形成的"产品",保留着演化过程中重大地质事件留下的痕迹,使用现代地球物理探测技术对这个"产品"进行成像,不仅可以了解现今的构造和物质状态,还可以推演过去曾经发生的动力学过程.长江中下游成矿带是我国重要的铁、铜多金属资源基地,其形成的深部动力学过程一直是矿床学家...     

A Preliminary study on deep geodynamic process of Xar Moron tectonic belt in eastern Central Asia Orogenic BeltSCIEI北大核心CSCD

板块汇聚边缘的陆壳厚度变化与构造和岩浆过程的动态相互作用有着错综复杂的联系,也是对深部地球动力学背景的直接响应。西拉木伦构造带是中亚造山带东部重要的汇聚板块边界,查明其浅部构造变形及深部动力学过程对于理解中亚造山带构造演化具有重要意义。本文通过野外地质工作查明晚二叠世-早三叠世西拉木伦构造带的上地壳发育一系列北东向、轴面向南东倾的宽缓褶皱以及向南东逆冲的断层,变形样式属于薄皮构造,显示出由北西向南东挤压的单向构造应力背景,平衡剖面恢复显示此时期构造变形造成地表~30%的缩短以及~4km的浅部地壳增厚。利用林西地区火成岩全岩La/Yb比值和锆石Eu/Eu*参数构建的年龄-地壳厚度曲线揭示,二叠纪早-中期地壳厚度从49km连续减薄到33km,反映此时期整体处于伸展环境。二叠纪晚期至三叠纪初期,地壳厚度增加了~15km,峰值厚度达~48km,这个迅速的地壳增厚过程可能是岩浆作用导致的地壳垂向增生和构造作用产生的造山带物质堆叠综合作用的结果。本文根据构造带同汇聚期岩浆岩面积和地壳厚度估算造山作用形成了~11%的新生陆壳。同时,两个时期的深部壳幔相互作用方式也有不同,二叠纪早期西拉木伦构造带火成岩锆石的εHf(t)值相对较高(6.1~19.9;均值10.1),δ^(18 )O值较分散(5.1‰~8.3‰),指示岩浆在形成过程中有幔源物质的加入,示踪了林西地区深部与软流圈上涌有关的伸展过程;而晚二叠世至三叠纪初期花岗岩锆石εHf(t)值相对下降(-1.1~17.2;均值9.3),δ^(18 )O值仍高于幔源值(>5.9‰),揭示同源地幔岩浆的持续重融改造过程。综合沉积环境、地壳厚度变化、岩浆岩同位素变化、地壳增生量及地表单向构造应力背景等特征,本文提出西拉木伦构造带可能经历了地幔俯冲;而早-中二叠世的软流圈上涌和晚二叠世-早三叠世的下地壳及岩石圈地幔密度增大,可能是发生地幔俯冲的深部地球动力学原因。     

大陆地震构造系统: 以青藏高原及邻区为例

青藏高原及邻区三角形发震构造域是全球大陆最显著的地震多发区.脆性活动断层及其弹性回跳模式无法合理解释该区深度集中分布在10~40 km的点状震源.针对发震构造和地震机理不明确这一重大科学问题, 以大陆动力学和地球系统动力学新思想为指导, 对青藏高原及邻区发震构造系统进行域、层、带、点相关研究, 阐明大陆地震构造系统的结构型式, 认为下地壳固态流变及其韧性剪切带是提供地震能量的孕震构造, 中地壳韧-脆性剪切带是累积地震能量的发震构造, 上地壳脆性断裂是释放地震能量的释震构造.在研究青藏高原及邻区地震构造系统及其形成背景的基础上, 进一步论证了大陆地震热流体撞击的形成机理: 地幔墙导致大洋中脊之下的软流圈热流物质层流到大陆特定部位汇聚加厚并底辟上升, 造成大陆下地壳部分熔融和固态流变, 并改变莫霍面的产状, 固态流变物质侧向非均匀流动, 形成大陆盆山体系, 流动的韧性下地壳与脆性上地壳之间具有韧-脆性剪切滑脱性质的中地壳不断积累由下地壳热能转换而来的应变能, 形成发震层, 震源定位于下地壳热流物质富集带("热河")中的固态-半固态流变物质撞击到强弱层块之间的构造边界, 不同热构造环境和撞击角度产生5种不同类型的地震.从而为大陆地震的科学预测奠定了全新的理论基础.      

滇西新构造运动时期陆内伸展作用

上新世一第四纪为滇西的新构造运动时期,代表了本区喜马拉雅造山期后的伸展作用时间,除形成区域性的角度不整合外,还形成了一系列小规模的转换拉张盆地,并产生大规模玄武岩浆喷发。洱源—遮放地震深度-速度剖面的P波速度,显示本区岩石圈具4层结构,即上部壳层、韧性壳层、下部固态壳层和地幔岩石圈。各层对比表明,地幔隆起导致热隆伸展作用及热流上涌,并在壳幔界面产生局部混熔,下部壳层发生区域深变质作用;韧性壳层产生强烈纯剪流动,上部壳层则以脆性—脆韧性走滑断层及层圈式滑脱被动地调整;地壳均衡作用不断地调整地幔隆起与地壳厚度的关系。     

大别造山带构造超压形成的碰撞力学机理

提出了大别山构造超压形成的点碰撞模型，简要分析了大陆碰撞带构造运动引起的粘性介质中粘性应力和平均应力随岩石物性的变化规律。探讨了构造压力对超高压的贡献及对成岩深度的重要意义。研究表明：构造运动引起的岩石圈中的附加压力可能与静岩压力有相同的数量级，大陆造山带两陆块不规则边界的碰撞会引起局部应力集中，产生较大的构造压力，岩石介质的流变学分析表明，在相同外力作用下，岩石圈上部的高粘度性质决定了其在构造活动期间增温效果显著，但增压效果有限；而粘性较低的岩石圈下部则增压效果明显，为此，在下地壳与上地幔之间的低粘度带内有可能发生超高压变质作用。     

江西早二叠世晚期—晚二叠世早期的岩相古地理

摘　要　根据地层学研究的新进展‚将原乐平组的官山段和下老山段划归茅口阶‚编制了这 一时期的沉积断面图‚并对这一时期的沉积史进行了阐述。     

秦岭造山带与渭河地堑地电结构研究

秦岭造山带作为典型的陆内复合造山带,发生过强烈的构造变形,与北部的渭河地堑形成独具特色的盆山构造体系,目前其深部结构状态与盆山耦合响应缺乏深层动力学过程的理解,为此以跨越秦岭造山带、渭河地堑布设一条170 km的大地电磁测深剖面,通过宽频带和长周期大地电磁观测,构建秦岭造山带和渭河地堑深部地电结构,研究结果表明:1)秦岭造山带存在多重叠置的巨厚岩石圈,南秦岭与北秦岭地壳尺度存在明显的结构化差异; 2)扬子地块向北楔入到南秦岭岩石圈地幔中,南、北秦岭之间在上地幔存在低阻条带痕迹表明了楔入作用的前缘位置; 3)渭河地堑存在巨厚的沉积盖层,厚度由南向北逐渐减薄,由南侧的7~8 km减到北侧的3~4 km。渭河地堑下地壳至上地幔区域分布的两个低阻块体表明其岩石圈存在明显的电性差异,这种差异性的存在表征了华北地块南向挤压作用背景下软流圈上涌的贡献。     

长江中下游南京（宁）-芜湖（芜）段深部壳幔电性结构——宽频大地电磁测深研究

为了较全面、客观地认识南京(宁)-芜胡(芜)地区岩石圈深部结构,探讨岩石圈热结构和壳、幔物质状态等重要科学问题,为矿集区成矿作用和成矿规律的研究提供依据,我们完成了6条宽频大地电磁测深剖面。通过分析各剖面电性成像结果,讨论了研究区地壳-上地幔导电性的"拟三维"结构,发现测区普遍存在连续的下地壳-上地幔低阻层,仅在巢湖冲褶体断开。结合区域热流结果,我们认为下地壳-上地幔有较好的导电性,可能存在局部"熔融体"或"含水剪切断裂",其物质状态很可能是热的、软弱的。此外,我们通过物质状态和电性界面推断了上地幔隆起的位置和长江深断裂带的分布范围,认为长江断裂带不但存在,而且由多条北深南浅的断裂组成,较为复杂。     

南北地震带南段震源空间分布特征及其构造意义

大陆浅源地震震源空间分布可以看作是一种地球物理特征,大量震源的空间位置数据可用来刻划大陆地壳结构。通过研究南北地震带南段震源的空间分布特征,发现研究区震源深度分布在横向上的疏密变化与地质构造特征相对应。剖面震源分布等密度图显示,中、下地壳不同深度广泛分布着多震层。多震层的分布与地壳低速、低阻层具有相关性,多震层一般位于低速、低阻层的上方。中地壳层次的低速、低阻层很可能是壳内滑脱层,是韧性下地壳与脆性上地壳发生拆离解耦的构造层次;下地壳低速、低阻层是部分熔融、含流体的韧性流变层;壳内多震层的构造属性应是上地壳硬的脆性层,容易发生突然破裂,产生地震。低速、低阻层是大陆板块内部上地壳脆性层构造过程的主控因素,包括对大陆内部浅源地震的控制;因此,在低速、低阻层之上往往形成多震层,越是活动性强的低速、低阻层,其上多震层震源密度越高。南北地震带南段不同层圈和块体之间的差异运动控制了其地壳层次的构造活动,包括大量地震的发生,其中,下地壳流层与上地壳脆性层的差异运动在中地壳层次发生剪切拆离是最重要的因素。