渭河断理解盆地带的形成演化及断块运动

渭河盆地和灵宝盆地的形成始于始新世，中新世运城盆地开始形成，到上新世时期渭河断陷带统一。早更新世断陷带内形成广阔的“三门湖”，中更新世时期“三门湖”逐渐萎缩消亡。晚更新世以来断陷带继承性的发展。由于受秦岭、华山山前断裂带等相关阶状正断层的正倾滑运动的控制，断陷带演化过程主要表现为大幅度的沉陷、扩张并接受巨厚的堆积，在其内部产生了一系列向南掀斜的断块差异运动。断陷带新地质时期垂直差异运动十分强烈，是一强地震活动区。     

鄂尔多斯块体东部边界带新地质构造与地震活动的几个特点

鄂尔多斯块体东部边界带为南起渭河盆地、运城盆地,经临汾盆地、太原盆地,忻定盆地,北至大同盆地及怀来延庆盆地等新生代断陷盆地带。亦称山西裂谷带或山西隆起断陷带。     

鄂尔多斯周缘断陷盆地带垂直形变场分析

鄂尔多斯块体是一个内部结构完整作整体不对称隆起运动的块体。主要构造运动发生在块体周缘断陷盆地带和断裂带上。除块体的西南侧为挤压构造带以外,四周被规模不等的断陷盆地所围陷,块体与盆地之间均有区域构造控制,而断陷盆地带均有多个地堑或半地堑作一定斜列式排列,形成于新生代以来不同时期。     

罗布泊捷山子断裂晚第四纪活动特征

位于罗布泊的捷山子断裂,在航、卫片上线性影像清晰,平面上由2-3条断层组成。罗布泊东台地以东,断裂在地貌上构成较宽阔的断裂谷地或断陷盆地的边界,同时也构成了元古界、花岗岩体与古近系、新近系以及第四系的分界。在罗布泊东台地断裂切割由中更新世—晚更新世湖积物构成的东台地（雅丹地貌）。在赛里克沙依断陷盆地,断裂断错了晚更新世晚期洪积扇及冲沟Ⅰ、Ⅱ级阶地,并形成长约40 km的断层陡坎。捷山子断裂的中、西段在晚更新世有过显著的活动。     

青海湖的地质构造前景及形成演化

青海湖地区位于３个构造单元及多条深断裂的交汇部位,结构复杂,强度较弱。上新世出现断陷,中更新世成湖。湖盆可划分为３个地垒和３个次级断陷盆地。其形成和演化受中祁连南缘大断裂带、宗务隆山－青海南山大断裂带和黑马河－达晶大带重新活动及其它ＮＷＷ,ＮＷ,ＮＮＷ,ＳＮ,ＮＥ抽断裂的活动及伴随的差异隆升所控制,与青藏高原的隆升演化有密切关系,尤其是可能与青藏高原发生后造山伸展作用有关的应力场转变造成的负反转构     

汾渭断裂带近10年GPS观测获得的剖面变形与应变积累分析

利用1999～2009年汾渭断裂带GPS速度场观测资料,研究了跨断裂剖面变形动态演化特性、应变积累的分段差异性以及汶川大地震等的可能影响.结果表明:近10年来山西断陷带南段、渭河盆地中东部应变积累相对较快,山西断陷带北端的蔚广盆地南缘断裂、渭河断裂西段也存在一定程度应变积累.汶川大地震影响相对明显,2007～2009年...     

鄂尔多斯高原河曲段黄河阶地构造变形研究

通过对河曲县城一带出露较好的黄河阶地剖面进行研究,认为河曲一带黄河三、四级阶地形成于中更新世时期,晚更新世早期形成二级阶地,全新世形成一级阶地。本区中更新世抬升速率为0．14mm／a,晚更新世抬升速率为0．18mm／a,全新世抬升速率为0．70mm／a,晚更新世和全新世抬升速率的突然加大,可能与黄河下游三门湖的贯通、区域侵蚀基准面突然降低、河流侵蚀加大有关。     

怒江断裂带南段道街盆地第四纪构造活动特征

上新世末以来滇西地区发生大面积掀斜隆升构造运动, 同时伴随块体的差异性升降运动。 在这种构造背景下, 怒江断裂带南段形成了一系列断陷盆地, 其中道街盆地是面积最大的一个盆地。 本文利用野外地质考察、 钻探和后差分GPS实测剖面等方法对该盆地第四纪地层和控盆断裂进行研究, 认为道街盆地控盆断裂最新活动时代为中—晚更新世之间, 而盆地内部断层晚更新世以来仍有活动表现。     

秦岭北缘断裂带的重要分支——桃川-户县断层的浅部结构与第四纪活动性

秦岭北缘断裂带是渭河盆地南缘重要的活动构造,含有多条分支断层,其中近EW向的桃川-户县断层位于该断裂带的北侧,其东段隐伏于渭河盆地内。已有研究对该断层隐伏段的中段开展了浅层人工地震勘探,并推断其为正断兼走滑运动性质的晚更新世活动断层,但未能确定断层最晚活动的年代与活动速率。文中通过开展新的浅层地震勘探和钻孔联合剖面探测,进一步研究了桃川-户县断层西段(太白盆地段)与东段(渭河盆地隐伏段)的浅部结构构造和几何展布、第四纪活动的最晚时代及活动速率。探测剖面揭示出桃川-户县断层的西段可向W延伸至少20km至太白盆地,而东段自眉县起延入渭河盆地,经周至、户县,隐伏于渭河盆地第四系中。断层西段在太白盆地断错早第四系及下伏结晶基底,控制了太白盆地南缘,其N倾的正断作用断错第四系约300m,断层带内保留老的逆冲构造残余。断层东段(渭河盆地隐伏段)在周至和户县附近的主断面倾向N,断层带分别表现为宽约6km的断陷带和宽约4km的阶梯状构造带,断错了上更新统顶界;在渭河盆地南缘,断层断错全新统标志层黑垆土S₀,垂直断距为4～5m,对应的全新世活动速率为0.4～1.3mm/a。综合浅层...     

山西晚新生代古地理环境变迁与新构造运动响应

系统解读了山西晚新生代古地理古环境特征,结合近年来笔者的研究给出了各时代古地理分布图。上新世的构造运动和地理环境演化奠定了现今地理环境的基础,尤其是奠定了现今地貌、水系的轮廓。早更新世地理环境最突出的事件是各断陷盆地中的湖泊广泛发育,出现淹没整个盆地的大湖景观;黄土广泛发育,但主要堆积于吕梁山分水岭以西;黄河在早更新世已经发育,并形成5级阶地。中更新世古地理的主要事件是湖泊的衰退,黄土堆积范围几乎遍布全省,厚可达200 m左右,表明气候较早更新世进一步明显变干。晚更新世古地理的主要特征是湖泊消亡,其地理环境更加接近现代。最后,笔者预测未来山西断陷盆地将持续断陷,各盆地内水系不再外流,形成贯通的大湖景观,类似现今的贝加尔湖。     

向错-位错组合模型模拟渭河盆地地壳水平变形特征

基于向错-位错组合模型模拟渭河盆地内主要断层的滑动与转动运动变形,通过数值计算获得断层滑动及转动变形引起的地表水平位移,并与盆地内实测GPS水平位移进行了对比。结果表明:采用向错-位错组合模型能够完整地描述断层实际的滑动与转动运动变形状态,组合模型模拟断层滑动与转动引起的地表水平位移与实测GPS水平位移,无论在量级或是运动趋势上均具有较好的一致性特征。     

VELOCITY CHARACTRISTICS OF SHANXI AND ADJACENT AREA AND ITS TECTONIC SIGNIFICANCE

In order to acquire a better velocity structure of the crustal and uppermost mantle beneath Shanxi area, we obtain the group and phase velocities of Rayleigh wave of the periods 8s to 50s in Shanxi and adjacent area using ambient seismic noise recorded at 216 broad-band stations. All available vertical-component time series for 2014 have been cross-correlated to yield estimates of empirical Rayleigh wave Green's function. Group and phase velocity dispersion curves for Rayleigh wave are measured for each interstation path by applying frequency-time analysis. It describes finer velocity structure of the crust and upper mantle in Shanxi, which reflects the geological structure characteristics at different depths. The resolution is within 50km and the resolution of part periods can reach 40km.The Rayleigh wave group and phase speed maps at short periods(8~18s and 10~22s)show clear correlations with shallow geological structures. Mountain areas on both sides of Shanxi depression zone show apparent high-velocity anomaly, except for low-velocity anomaly in the Taiyuan Basin, Linfen-Yuncheng Basin and Weihe Basin. Especially, the areas of Youyu County-Pianguan County-Kelan County-Shuozhou City and Jingle County-Lishi District of Lüliang City in Lüliang Mountains, and Yu County-Fuping County-Yi County and Yangcheng County-Licheng County in Taihang Mountains, present higher velocity anomaly. In addition, the velocity is lowest in the Weihe Basin, and the amplitude of low velocity decreases gradually from the south to the north of the basins in Shanxi, which probably is related to the process of gradual stretching and development of the Shanxi rift zone from the southwest to the northeast. The obvious velocity difference across the latitude of 38°N exists at 18~30s period of phase and 24~35s period of group velocity maps, which is probably related to the deep and shallow Moho depth variation in the south and north of Shanxi and the suture zone of ancient blocks including "hard" southern block and "soft" northern block. At the same time, the research result of receiver function reveals that partial melting of the lower crust occurs in the northern Taihang Mountains, while the southern section remains stable(Poisson's ratio is above 0.3 in the northern Taihang Mountains and 0.25~0.26 in the southern section). The phase velocity map at 30~50s period clearly shows NW velocity gradient belt, and the low velocity anomaly in the northeast side may be related to Cenozoic volcanism. Meanwhile, the eastern border of Ordos block is the western faults of central basins in Shanxi depression zone. However, some research results indicate that the above border is Lishi Fault in the surface, inferring that the Ordos block shows a shape of wide in the upper and narrow in the lower part from the surface to deep. The Datong volcanic area at 18~45s period of phase and 24~35s period of group velocity maps shows low velocity of trumpet shape from shallow to deep, related to the upwelling of hot material from lower mantle in the Cenozoic causing a large area of intense magmatic activity. It indicates the more specific upwelling channel of Datong volcanoes simultaneously.     

渭河盆地岩石圈热结构与地热田热源机理

岩石圈热结构是盆地现今地温场研究的重要延伸和扩展,是了解大陆岩石圈构造变形及演化等大陆动力学问题的重要窗口,更是地热田热源机理研究的核心问题.本次工作,在系统分析渭河盆地现今地温场和水动力系统基础上,编制了渭河盆地大地热流分布等值线图;通过实测生热率等热物性参数,利用一维稳态热传导方程计算了研究区岩石圈热结构,并分析了渭河盆地岩石圈热结构特征和地热田热源机理.结果表明,渭河盆地现今大地热流值分布范围为62.5~80.2mW·m-2,平均为70.8±4.8mW·m-2,西部明显高于东部,西安坳陷最高,咸礼凸起次之;渭河断裂并不是控热断裂,其沟通作用引起的水热循环一定程度上影响了浅部热量再分配,对渭河盆地地温场并没有起到明显的控制作用.西安坳陷—咸礼凸起地壳热流介于32.2~37.5mW·m-2之间,平均为34.6mW·m-2;地幔热流分布范围为33.8~38.9mW·m-2,平均为36.0mW·m-2;地壳热流和地幔热流的总体变化趋势一致,西安坳陷高于咸礼凸起,分析认为西安坳陷沉积层厚度大于后者,且沉积层放射性生热率更大,是造成西安坳陷地壳热流高于咸礼凸起的原因,而西安坳陷相比咸礼凸起更高的地幔热流,表明西安坳陷深部活动性强于咸礼凸起.西安坳陷和咸礼凸起地壳/地幔热流比值相近,介于0.93~1.01之间,平均为0.96,"热"岩石圈厚度约为95~101km.渭河盆地岩石圈热结构特征与鄂尔多斯盆地在很大程度上具有相似性,暗示着二者具备相似的深部稳定性,这与渤海湾盆地为代表的中国东部中—新生代主动裂谷盆地岩石圈热结构特征截然不同,表明渭河盆地为被动伸展裂陷.从鄂尔多斯盆地、渭河盆地、山西裂谷到华北盆地,"热"岩石圈厚度的有序变化表明太平洋板块俯冲引起的地幔对流对华北地块深部动力学行为的影响主要发生在太行山以东,而太行山以西的鄂尔多斯盆地和渭河盆地则影响甚微,这种空间差异影响从侧面暗示着华北克拉通破坏过程的有序性.综合分析渭河盆地地质—地球物理资料认为,岩石圈表层伸展破裂、深部重力均衡调整进而引起软流圈被动上涌,其产生的相对高地幔热流的热传导和深大断裂沟通的水体热对流相互叠加作用,共同构成了渭河盆地中—低温地热田的热源机理.     

构造和气候共同控制下的藏南热隆盆地中更新世以来的演化

热隆盆地是亚东－谷露裂谷系南部, 由宁金抗沙西麓断裂控制的断陷盆地, 根据野外地质调查、 遥感(RS)和数字高程模型(DEM)分析, 盆地内发育有三期洪积扇, 形成时代分别在中更新世中期(第一期)、 中更新世中期至晚更新世早期(第二期)、 晚更新世晚期(第三期)。 这三期洪积扇的发育分别对应于间冰期和间冰阶的高温大降水时期, 表明在第四纪以来, 由于间冰期与间冰阶期的到来, 温度升高, 降雨量增加, 地表径流作用增强, 先成洪积扇被破坏, 新洪积扇形成。 盆地内自中更新世中晚期以来剥蚀程度自北向南减弱, 表明在整体抬升的背景下, 由于宁金抗沙西麓断裂的活动, 使得盆地北部基岩抬升速率大于南部, 形成自北向南的掀斜。     

兰州马衔山北缘断裂带的新活动特征

通过详细地质填图研究获得了兰州马衔山北缘断裂带的几何学、新活动性、断错微地貌及滑动速率等的定量资料。马衔山北缘断裂为一条历史悠久的区域性活动断裂 ,其几何形态较简单 ,总体走向N6 0°W ,全长约 115 .5km。根据断裂分叉、拐弯及不连续阶区等几何特征和活动性的差异 ,大致可以将该断裂划分为 4条次级断层段 ,自东向西分别称为内官营段、马衔山段、七道梁段和雾宿山段。断裂的新活动具分段性 ,其中的内官营段为具逆断特性的晚更新世活动段 ,而马衔山段、七道梁段和雾宿山段均为全新世活动段。该断裂早期具逆断特性 ,大约自中更新世以来以左旋走滑为主兼具倾滑运动分量 ,形成了一系列山脊、冲沟、阶地等的左旋断错 ,断距几米至几百米。沿断裂带的水平位移具分组现象 ,可能反映了断裂的黏滑活动特性。根据Ⅰ ,Ⅱ级阶地的左旋断错值及其年代 ,得到了马衔山北缘断裂带晚更新世以来的平均水平滑动速率约为 3.73mm/a。同时沿断裂带还保存有断崖和断坎等 ,其中Ⅰ级阶地上的断坎高 1～ 1.5m左右     

Influence of Neoproterozoic tectonic fabric on the origin of the Potiguar Basin,northeastern Brazil and its links with West Africa based on gravity and magnetic data

The Potiguar Basin is a ∼6,000 m thick aborted NE-trending rift that was formed during the Cretaceous in the continental margin of northeastern Brazil. Its ∼E–W-trending offshore faults form part of the successful continental margin rift that evolved into the South Atlantic Ocean. The region represents one of the most significant pre-Pangea breakup piercing points between eastern South America and West Africa. We used gravity, aeromagnetic, and geological data to assess the role of reactivated Precambrian shear zones and major terrain boundaries in the development of the Potiguar Basin from the Cretaceous to the Cenozoic. We also looked for possible links between these structures in northeastern Brazil and their continuation in West Africa. Our results indicate that the major fault systems of the Potiguar Basin were superimposed on the Precambrian fabric. Both gravity and magnetic maps show lineaments related to the shear zones and major terrain boundaries in the Precambrian crystalline basement, which also characterize the architecture of the rift. For example, the Carnaubais fault, the master fault of the rift system, represents the reactivation of the Portalegre shear zone, the major tectonic boundary between Precambrian terrains in the crystalline basement. In addition, part of the Moho topography is controlled by these shear zones and developed during the period of main rift extension in the Neocomian. The shear zones bounding the Potiguar rift system continue in West Africa around and underneath the Benue Basin, where fault reactivation also took place.     

Dynamics of continental rift propagation: the end-member modes

An important aspect of continental rifting is the progressive variation of deformation style along the rift axis during rift propagation. In regions of rift propagation, specifically transition zones from continental rifting to seafloor spreading, it has been observed that contrasting styles of deformation along the axis of rift propagation are bounded by shear zones. The focus of this numerical modeling study is to look at dynamic processes near the tip of a weak zone in continental lithosphere. More specifically, this study explores how modeled rift behavior depends on the value of rheological parameters of the crust. A three-dimensional finite element model is used to simulate lithosphere deformation in an extensional regime. The chosen approach emphasizes understanding the tectonic forces involved in rift propagation. Dependent on plate strength, two end-member modes are distinguished. The stalled rift phase is characterized by absence of rift propagation for a certain amount of time. Extension beyond the edge of the rift tip is no longer localized but occurs over a very wide zone, which requires a buildup of shear stresses near the rift tip and significant intra-plate deformation. This stage represents a situation in which a rift meets a locked zone. Localized deformation changes to distributed deformation in the locked zone, and the two different deformation styles are balanced by a shear zone oriented perpendicular to the trend. In the alternative rift propagation mode, rift propagation is a continuous process when the initial crust is weak. The extension style does not change significantly along the rift axis and lengthening of the rift zone is not accompanied by a buildup of shear stresses. Model predictions address aspects of previously unexplained rift evolution in the Laptev Sea, and its contrast with the tectonic evolution of, for example, the Gulf of Aden and Woodlark Basin.     

Arc–arc collision in the Izu collision zone, central Japan, deduced from the Ashigara Basin and adjacent Tanzawa Mountains

The Pleistocene Ashigara Basin and adjacent Tanzawa Mountains, Izu collision zone, central Japan, are examined to better understand the development of an arc–arc orogeny, where the Izu–Bonin – Mariana (IBM) arc collides with the Honshu Arc. Three tectonic phases were identified based on the geohistory of the Ashigara Basin and the denudation history of the Tanzawa Mountains. In phase I, the IBM arc collided with the Honshu Arc along the Kannawa Fault. The Ashigara Basin formed as a trench basin, filled mainly by thin-bedded turbidites derived from the Tanzawa Mountains together with pyroclastics. The Ashigara Basin subsided at a rate of 1.7 mm/year, and the denudation rate of the Tanzawa Mountains was 1.1 mm/year. The onset of Ashigara Basin Formation is likely to be older than 2.2 Ma, interpreted as the onset of collision along the Kannawa Fault. Significant tectonic disruption due to the arc–arc collision took place in phase II, ranging from 1.1 to 0.7 Ma in age. The Ashigara Basin subsided abruptly (4.6 mm/year) and the accumulation rate increased to approximately 10 times that of phase I. Simultaneously, the Tanzawa Mountains were abruptly uplifted. A tremendous volume of coarse-grained detritus was provided from the Tanzawa Mountains and deposited in the Ashigara Basin as a slope-type fan delta. In phase III, 0.7–0.5 Ma, the entire Ashigara Basin was uplifted at a rate of 3.6 mm/year. This uplift was most likely caused by isostatic rebound resulting from stacking of IBM arc crust along the Kannawa Fault which is not active as the decollement fault by this time. The evolution of the Ashigara Basin and adjacent Tanzawa Mountains shows a series of the development of the arc–arc collision; from the subduction of the IBM arc beneath the Honshu Arc to the accretion of IBM arc crust onto Honshu. Arc–arc collision is not the collision between the hard crusts (massif) like a continent–continent collision, but crustal stacking of the subducting IBM arc beneath the Honshu Arc intercalated with very thick trench fill deposits.     

东秦岭卢氏盆地最新活动特征及铁炉子断裂尾端构造特点

利用区域水系形态研究构造活动特征已有丰富经验,可知铁炉子—栾川—南召断裂带西段——铁炉子断裂,晚更新世以来左旋走滑速率为1.25 mm/a,而东段——栾川—南召断裂则为早—中更新世活动段,2段具有明显的活动性差异,研究二者的构造转换方式,有助于了解块体运动在该断裂带内不同段落间的平衡方式。铁炉子段在洛南盆地分为南北两支,南支断裂下盘发育的冲沟普遍流向北,呈“平行状”水系,而北支断裂下盘发育的冲沟则流向南,并在断层附近有左旋扭动迹象;卢氏盆地中部发育NE走向的沉降中心,剖面分析结果表明,该沉降中心东侧普遍高出西侧70—80 m,结合遥感影像,初步认为卢氏盆地的最新活动或已由盆地边缘向盆地内部迁移,并与铁炉子段尾端组成伸展转换区,最终导致铁炉子断裂与栾川—南召断裂的活动性差异。     

Research on Formation Mechanism of Asymmetric Basins, Taking the Weihe Basin as an Example

Asymmetry of the Weihe Basin is discussed in the paper,and also the master control fault,secondary control fault of asymmetric basin is proposed in the paper.The asymmetry of the Weihe Basin is expressed as follows:(1) its shape of the cross sections is asymmetrical;(2) the tectonic activity of the southern margin fault and the northern margin one is apparently different;(3) its deep tectonics is asymmetrical.Finally,we use the Weihe Basin as an example to establish a "cantilever-beam" model for calculations.The results show that:(1) flexure leads to stress accumulation and forming extensional fractures;(2) fractures slope steeply towards the free end;(3) when the length of beam becomes longer,it is possible that new extensional fractures will occur in the fixed end.