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1.
南极布兰斯菲尔德海峡及周边区域是南极大陆火山、地震等新构造活动最活跃的地区,与南设得兰海沟、南设得兰群岛一同构成南极大陆边缘现存唯一的"沟-弧-盆"构造体系。本文基于"雪龙"船第28、第30航次实测数据及两个航次的国际共享资料,利用均衡改正数据处理方法获得布兰斯菲尔德海峡的莫霍面深度及其分布规律,分析深部构造-断裂的区域分布及其重力异常特征等。布兰斯菲尔德海峡内的空间重力异常呈条带状分布,走向总体与地形相近,布格重力异常则由两侧向中间升高,大致在坡折处形成异常场值为100×10-5 m/s2的分界线,在中央次海盆和东部次海盆海山处形成两个异常高值圈闭,异常值最高为150×10-5 m/s2。莫霍面深度以弧后扩张中心为最低值,向南设得兰群岛和南极半岛两个方向递增,深度从12 km递增至陆坡位置的24 km。 相似文献
2.
《海洋地质与第四纪地质》2017,(6)
南海东部古扩张脊处于欧亚板块和太平洋板块的汇聚地带,其东侧为马尼拉海沟、北吕宋海槽和西吕宋海槽,由于受到多个构造单元的相互作用,使其处于复杂的构造环境中。南海东部古扩张脊俯冲过程的研究对深入理解南海海盆构造演化、火山及地震活动等具有重要意义,同时也是今后南海构造研究的重要方向之一。在总结前人研究基础之上,探讨南海东部古扩张脊俯冲时间、俯冲深度及动力学过程。南海板块在16 Ma之后,由于菲律宾板块NW向仰冲的作用,使南海东部古扩张脊被动地沿马尼拉海沟进行俯冲,形成了现今马尼拉海沟中段的构造格局。古扩张脊俯冲深度为200~300km,并且在约100km处发生板片撕裂,造成古扩张脊两侧俯冲角度的不同。 相似文献
3.
华北-扬子板块碰撞是中国东部中生代最重要的地质事件之一,碰撞形成了世界最大的超高压变质带秦岭-大别-苏鲁造山带。在苏鲁造山带向海域延伸部分,一直缺乏相关地球物理资料来约束碰撞造山带的深部特征。本文总结了华北-扬子板块碰撞的经典模型,根据南黄海海域最新二维地震反射资料和前人的研究成果,认为在造山带南缘南黄海盆地中,扬子板块上、下地壳发生拆离,形成类似"鳄鱼嘴式"形态,华北板块向南楔入到扬子板块之中。在区域重磁异常图中,千里岩隆起带与苏鲁造山带具有相似的重磁异常分布,认为千里岩隆起带为华北-扬子碰撞造山带在海域上的延伸;在南黄海盆地北缘二维地震剖面中,千里岩隆起与南黄海盆地具有完全不同的地震反射特征,南黄海盆地发育完整地层层序,而千里岩隆起内部反射杂乱,变形强烈。在南黄海盆地自西向东三条南北向地震剖面中,南黄海盆地与千里岩隆起带边界反射均具有南倾特征,表明扬子板块物质置于造山带之上;南黄海盆地北部烟台坳陷发育中侏罗统,约束华北-扬子碰撞所导致的挤压活动主要发生于晚三叠世。在千里岩隆起内部反射特征整体上具有背形形态,具有向北逆冲挤压特征,千里岩隆起内反射断续自南黄海盆地基底之下延伸至造山带近地表位置,形态类似于变质核杂岩从深部拆离到地表;千里岩隆起深部,在10 s深度附近可识别一系列近水平反射,具有莫霍面反射特征,莫霍面反射延伸至南黄海盆地北缘消失,推测千里岩隆起之下为华北板块地壳,而华北-扬子板块碰撞过程导致南黄海盆地之下莫霍面反射缺失。多方面的证据支持南黄海海域内扬子板块的"鳄鱼嘴式"地壳形态,以及华北板块地壳向南楔入到扬子板块地壳中。 相似文献
4.
《海洋地质与第四纪地质》2017,(2)
南薇隆起区地处南沙地块西北部,紧邻西南次海盆,周围发育大量陆缘裂解盆地。裂陷盆地拥有丰富的油气资源。地块经历了中生代末期至古近纪裂谷拉张,并随晚始新世的海底扩张向南漂移至现今位置。结合区域以往地震剖面和钻井数据,分析了2013年中科院南海海洋研究所"实验2号"采集的高分辨率单道地震数据(Nan-1),总结了南薇隆起区的地震反射特征。认为南薇隆起区主要由南部裂陷下沉带和北部埋藏火山隆起带两个结构单元组成。从北到南,埋藏火山隆起带跨越约63km的范围,裂陷下沉带跨越约58km的范围。地震剖面清晰地揭示了该区向海盆侧隆起且在SE向成带的特征。南薇区具有拉张背景,其形成与演化主要是与西南次海盆的扩张作用,以及南沙地块与婆罗洲地块的碰撞作用等有关。自上新世以来,整个南薇隆起区进入构造活动相对稳定阶段,地壳稳定性较好。 相似文献
5.
1 俯冲区最古老的地壳构造板块在俯冲区的相互作用是研究得最少的地质问题之一。很明显 ,被吸收的物质应当改变位于俯冲区的岛弧火山岩的地球化学参数。但是不知道这个物质的哪一部分参与了喷发产物的形成 ,而哪一部分在地幔中被再改造。在俯冲区被改造的地球陆壳成分在很大程度上决定于海洋板块沉积盖层中的化学元素(如稀土元素、Ｔｈ、Ｂａ、Ｂｅ) ,而在其火山基底最上部氧化带则为Ｋ、Ｂ、Ｖ、ＣＯ2 和Ｈ2 Ｏ。因此 ,研究海洋板块和位于俯冲区的大陆板块边缘部分剖面的地球化学参数 ,可以提供计算物质平衡及其在这些地区被改造的必需的… 相似文献
6.
东海莫霍面起伏与地壳减薄特征初步分析 总被引：3，自引：0，他引：3
收集、整理大量由地震剖面提供的沉积层厚度资料,得到东海沉积层等厚图。对完全布格重力异常进行沉积层重力效应改正后,得到剩余重力异常,利用地震资料揭示的莫霍面深度值来约束界面反演得到东海莫霍面埋深。结果表明,东海陆架盆地莫霍面深度在25～28 km之间平缓变化,地壳厚度为14～26 km,西厚东薄;冲绳海槽盆地莫霍面深度为16～26 km,地壳厚度为12～22 km,北厚南薄。东海陆架盆地东部与冲绳海槽盆地南部地壳减薄明显,拉张因子分别达到2.6和3。初步分析认为冲绳海槽地壳以过渡壳为主,并未形成洋壳。 相似文献
7.
在前人勘探解释的基础上,通过三维高分辨率地震资料,应用相干属性分析等技术对区域断裂进行精细化解释。研究表明盆地内发育着典型的犁式、花状构造、旋转正断层等伸展构造样式,在珠三南断裂影响下,南部边界断裂以阶梯状排列形成断阶构造。始新世—中中新世,断裂走向在持续右旋张扭应力场下以NE→EW→NWW顺时针方向旋转,张裂强度逐渐减弱。晚始新世—早渐新世,盆地在太平洋板块俯冲后退、印亚板块碰撞、古南海向南俯冲下发育EW向断裂,晚渐新世在南海扩张事件影响下前期右旋应力场得到加强,形成大量近EW向断裂,中新世后演化为NWW向断裂。文昌A凹陷断裂构造的演化、成因机制与南海北部陆缘应力场变化一致。该研究有利于进一步了解南海北部陆缘含油气盆地的构造特征和演化规律,提高油气勘探开发的效率。 相似文献
8.
9.
南海西北部与红河地区地球物理场及其地壳深部结构特征 总被引：10，自引：0，他引：10
分析了南海西北部与红河地区地球物理场特征，计算了研究区重、磁资料的一阶小波细节变换、四阶小波逼近变换。根据重力场资料以及南海北部盆地钻井取样的测试结果，同时参考在研究区进行的地震勘探结果，对研究区的地壳结构进行了反演计算。结果表明，研究区域地壳结构较为复杂，地壳厚度在17—38km之间，总的趋势由陆向洋地壳厚度逐渐减薄，反映出该区域地壳具有陆壳、过渡壳的性质，同时存在上地幔隆起区及凹陷区。用地震层折成像结果与重力资料计算出的地壳分布趋势进行了对比验证。根据地幔对流结果探讨了研究区深部地球动力学特征及其与深部地壳结构的关系。 相似文献
10.
太平洋板块向北美板块俯冲,在北美洲阿拉斯加大陆边缘形成了碰撞造山带和俯冲构造带,前人对该区域阿拉斯加俯冲带地幔转换带的研究存在分歧,一种观点认为太平洋板块俯冲至阿拉斯加中南部下方的地幔转换带内部,引起地幔转换带增厚,另一种观点则认为地幔转换带增厚是由于库拉板块残留造成的。因此,研究阿拉斯加俯冲带区域地幔转换带的精确成像对于厘清太平洋板块俯冲机制和俯冲过程具有重要意义。本文利用美国地震联合学会（IRIS）在阿拉斯加区域布设的USArray部分固定台站接收到远震事件的波形资料,采用天然地震P波接收函数与共转换点道集叠加的方法,反演得到了阿拉斯加山脉和育空高原410 km、660 km间断面和地幔转换带的厚度结构。结果表明：由于太平洋板块俯冲至地幔转换带内部,使得410 km间断面在阿拉斯加山脉东部和育空高原与阿拉斯加山脉交界处的弧形区域出现了抬升现象,抬升幅度为0～20 km,进而导致在该区域出现不同程度的地幔转换带增厚的现象,验证了第一种观点。另外,该地区地幔转换带结构显示,660 km间断面在阿拉斯加山脉东部以及阿拉斯加山脉与育空高原交界的东部出现下沉现象,故此推测阿拉斯加中南部部分区... 相似文献
11.
Pablo Sangrà Carmen GordoMónica Hernández-Arencibia Angeles Marrero-DíazAngel Rodríguez-Santana Alexander Stegner Antonio Martínez-MarreroJosep L. Pelegrí Thierry Pichon 《Deep Sea Research Part I: Oceanographic Research Papers》2011,58(4):390-402
We use hydrographic data collected during two interdisciplinary cruises, CIEMAR and BREDDIES, to describe the mesoscale variability observed in the Central Basin of the Bransfield Strait (Antarctica). The main mesoscale feature is the Bransfield Front and the related Bransfield Current, which flows northeastward along the South Shetland Island Slope. A laboratory model suggests that this current behaves as a gravity current driven by the local rotation rate and the density differences between the Transitional Zonal Water with Bellingshausen influence (TBW) and the Transitional Zonal Water with Weddell Sea influence (TWW). Below the Bransfield Front we observe a narrow (10 km wide) tongue of Circumpolar Deep Water all along the South Shetland Islands Slope. At the surface, the convergence of TBW and TWW leads to a shallow baroclinic front close to the Antarctic Peninsula (hereafter Peninsula Front). Between the Bransfield Front and the Peninsula Front we observe a system of TBW anticyclonic eddies, with diameters about 20 km that can reach 300 m deep. This eddy system could be originated by instabilities of the Bransfield Current. The Bransfield Current, the anticyclonic eddy system, the Peninsula Front and the tongue of Circumpolar Deep Water, are the dynamically connected components of the Bransfield Current System. 相似文献
12.
Morphostructure and evolution of the central and Eastern Bransfield Basins (NW Antarctic Peninsula) 总被引：2，自引：0，他引：2
Eulàlia Gràcia Miquel Canals Marcel Lí Farràn Maria José Prieto Jordi Sorribas Gebra Team 《Marine Geophysical Researches》1996,18(2-4):429-448
The Bransfield Basin is a narrow and elongated active rift basin located between the Antarctic Peninsula and the South Shetland Islands. The Bransfield Basin is composed of three small basins, and two of them, the Central and Eastern Bransfield Basins, were surveyed during a recent cruise (GEBRA 93). The full swath bathymetry coverage as well as the single-channel seismic reflection and magnetic profiles that have been acquired, help us to better understand the morphostructure and recent evolution of the Bransfield Basin. Six large volcanic edifices aligned with the basin axis stick out of the sedimented seafloor of the Central Bransfield Basin. In contrast, the Eastern Bransfield Basin is characterised by four deep troughs displaying a rhombic-shape, and small, scattered volcanic cones located in the southwestern half basin. Seamount volcanism plays an important role in the formation of new crust in the Bransfield Basin. The larger seamounts of the Central Bransfield Basin are located at the intersection of the two main orthogonal sets of faults (longitudinal ENE-WSW and transversal NNW-SSE). Morphological analysis of the seamounts indicates a multi-staged volcano-tectonic construction. The distribution and shape of these edifices suggests that both volcanism and extension are concentrated at the same preferential areas through time. This might be related to the fracturation style of the continental crust. The Central and Eastern Bransfield Basins are very different in morphostructure, volcanism, and sedimentary cover. The Central Bransfield Basin shows evidence of NW-SE extensional faulting and focused active MORB-volcanism interpreted as result of incipient seafloor spreading. The Eastern Bransfield Basin is still in a rifting stage, mainly dominated by a NW-SE extension and some left-lateral strike-slip component probably related to the South Scotia Ridge.J. Acosta, J. Baraza, P. Bart, A.M. Calafat, J.L. Casamor, M. De Batist, G. Ercilla, G. Francés, E. Ramos, J.L. Sanz, and A. Tassone. 相似文献
13.
Geophysical investigations of crust-scale structural model of the Qiongdongnan Basin, Northern South China Sea 总被引：2，自引：0，他引：2
Ning Qiu Zhenfeng Wang Hui Xie Zhipeng Sun Zhangwen Wang Zhen Sun Di Zhou 《Marine Geophysical Researches》2013,34(3-4):259-279
Rifting of the Qiongdongnan Basin was initiated in the Cenozoic above a pre-Cenozoic basement, which was overprinted by extensional tectonics and soon after the basin became part of the rifted passive continental margin of the South China Sea. We have integrated available grids of sedimentary horizons, wells, seismic reflection data, and the observed gravity field into the first crust-scale structural model of the Qiongdongnan Basin. Many characteristics of this model reflect the tectonostratigraphic history of the basin. The structure and isopach maps of the basin allow us to reconstruct the history of the basin comprising: (a) The sediments of central depression are about 10 km thicker than on the northern and southern sides; (b) The sediments in the western part of the basin are about 6 km thicker than that in the eastern part; (c) a dominant structural trend of gradually shifting depocentres from the Paleogene sequence (45–23.3 Ma) to the Neogene to Quaternary sequence (23.3 Ma–present) towards the west or southwest. The present-day configuration of the basin reveals that the Cenozoic sediments are thinner towards the east. By integrating several reflection seismic profiles, interval velocity and performing gravity modeling, we model the sub-sedimentary basement of the Qiongdongnan Basin. There are about 2–4 km thick high-velocity bodies horizontal extended for a about 40–70 km in the lower crust (v > 7.0 km/s) and most probably these are underplated to the lower stretched continental crust during the final rifting and early spreading phase. The crystalline continental crust spans from the weakly stretched domains (about 25 km thick) near the continental shelf to the extremely thinned domains (<2.8 km) in the central depression, representing the continental margin rifting process in the Qiongdongnan Basin. Our crust-scale structural model shows that the thinnest crystalline crust (<3 km) is found in the Changchang Sag located in the east of the basin, and the relatively thinner crystalline crust (<3.5 km) is in the Ledong Lingshui Sag in the west of the basin. The distribution of crustal extension factor β show that β in central depression is higher (>7.0), while that on northern and southern sides is lower (<3.0). This model can illuminate future numerical simulations, including the reconstruction of the evolutionary processes from the rifted basin to the passive margin and the evolution of the thermal field of the basin. 相似文献
14.
Moo Hee Kang Hyun-Chul Han Hyesu Yun Gee Soo Kong Kyong O. Kim Youn Soo Lee 《Marine Geophysical Researches》2007,28(3):257-269
A seamount chain with an approximately WNW trend is observed in the northeastern Ulleung Basin. It has been argued that these
seamounts, including two islands called Ulleung and Dok islands, were formed by a hotspot process or by ridge related volcanism.
Many geological and geophysical studies have been done for all the seamounts and islands in the chain except Anyongbok Seamount,
which is close to the proposed spreading ridge. We first report morphological characteristics, sediment distribution patterns,
and the crustal thickness of Anyongbok Seamount using multibeam bathymetry data, seismic reflection profiles, and 3D gravity
modeling. The morphology of Anyongbok Seamount shows a cone shaped feature and is characterized by the development of many
flank cones and flank rift zones. The estimated surface volume is about 60 km3, and implies that the seamount is smaller than the other seamounts in the chain. No sediments have been observed on the seamount
except the lower slope, which is covered by more than 1,000 m of strata. The crustal structure obtained from a 3D gravity
modeling (GFR = 3.11, SD 3.82 = mGal) suggests that the seamount was formed around the boundary of the Ulleung Plateau and
the Ulleung Basin, and the estimated crustal thickness is about 20 km, which is a little thicker than other nearby seamounts
distributed along the northeastern boundary of the Ulleung Basin. This significant crustal thickness also implies that Anyongbok
Seamount might not be related to ridge volcanism. 相似文献
15.
本文基于中国南极考察第30航次、第32航次所获得的实测重力资料,结合NGDC资料,开展12个航次重力场数据的平差融合工作,全部386个交点平差后标准差减小为±1.53×10−5 m/s2,与卫星重力差值平均值为1.49×10−5 m/s2,均方差为±3.81×10−5 m/s2,并在此基础上采用频率域界面反演法计算莫霍面深度。研究发现,与沉积盆地对应重力异常低值相悖,在罗斯海北部盆地、维多利亚地盆地、中央海槽、东部盆地4个主要盆地腹地却表现为重力异常高值,跨度达100 km以上。莫霍面深度分布整体呈南深北浅之势,范围为10~28 km。伴随着罗斯海西部盆地的多次拉张及岩浆活动,该区域的地壳厚度和莫霍面深度高值和低值相间分布,并表现出越来越大的差异性。综合剖面结果表明,罗斯海重力异常值的长波长变化与莫霍面的起伏呈正相关关系,但是反演的莫霍面深度与区域重力场特征并非完全对应,所以岩浆底侵和地壳侵入仍不足以导致罗斯海盆地的重力异常或盆地几何形状。 相似文献
16.
Lithospheric structure below the eastern Arabian Sea and adjoining West Coast of India based on integrated analysis of gravity and seismic data 总被引：1，自引：0，他引：1
Four uniformly spaced regional gravity traverses and the available seismic data across the western continental margin of India, starting from the western Indian shield extending into the deep oceanic areas of the eastern Arabian Sea, have been utilized to delineate the lithospheric structure. The seismically constrained gravity models along these four traverses suggest that the crustal structure below the northern part of the margin within the Deccan Volcanic Province (DVP) is significantly different from the margin outside the DVP. The lithosphere thickness, in general, varies from 110–120 km in the central and southern part of the margin to as much as 85–90 km below the Deccan Plateau and Cambay rift basin in the north. The Eastern basin is characterised by thinned rift stage continental crust which extends as far as Laxmi basin in the north and the Laccadive ridge in the south. At the ocean–continent transition (OCT), crustal density differences between the Laxmi ridge and the Laxmi basin are not sufficient to distinguish continental as against an oceanic crust through gravity modeling. However, 5-6 km thick oceanic crust below the Laxmi basin is a consistent gravity option. Significantly, the models indicate the presence of a high density layer of 3.0 g/cm3 in the lower crust in almost whole of the northern part of the region between the Laxmi ridge and the pericontinental northwest shield region in the DVP, and also below Laccadive ridge in the southern part. The Laxmi ridge is underlain by continental crust upto a depth of 11 km and a thick high density material (3.0 g/cm3) between 11–26 km. The Pratap ridge is indicated as a shallow basement high in the upper part of the crust formed during rifting. The 15 –17 km thick oceanic crust below Laccadive ridge is seen further thickened by high density underplated material down to Moho depths of 24–25 km which indicate formation of the ridge along Reunion hotspot trace. 相似文献
17.
Some seismic refraction observations undertaken during the IGY are reported here together with a summary of other refraction studies carried out within the Transkei Basin, the Mozambique Ridge and the South African continental shelf area.A 2.5 km section of Cretaceous and younger rocks is associated with profiles observed on the continental shelf; directly below this group are rocks with velocities in the range 4.0–5.5 km s-1, probably representatives of the Karroo and Cape supergroups. The basement material velocity variations were from 5.3 to 6.5 with an average of 5.9 km s-1, and is correlated with granite or Malmesbury Formation plus granite. This crustal structure is similar to that found on the eastern continental shelf of southern South America.The profiles in the Transkei Basin show a thick layer of sediment with velocity range 1.50 to 3.50 km s-1, underlain by a refracting layer in which the average velocity is 4.5 km s-1. The velocity of 6.6 km s-1 obtained for the oceanic layer is similar to the velocities of the crustal layer measured in the Argentine Basin. The mantle velocity (8.1 km s-1) is consistent with the average mantle velocity for the Indian Ocean but significantly lower than the Pacific Ocean average of 8.20 km s-1. The depth to Moho is about 12.0 km and the crustal section is typical oceanic. A plate tectonic model of the early opening of the South Atlantic is used to describe the evolution of the Transkei Basin.On the Mozambique Ridge the thin sediments (0.7 km) are underlain by rocks with velocities averaging 5.6 km s-1. This is more than 1.0 km s-1 faster than the velocity for layer 2 from the Transkei Basin and the Agulhas Plateau, indicating rocks of a younger age or of a different type. Moreover the crustal section of the Ridge has a thickness in excess of 22 km and is in isostatic equilibrium when compared with the adjacent Transkei Basin and Agulhas Plateau. DSDP site 249, situated on the Ridge, penetrated basalt at a depth of 0.4 km. Whether this is continental or oceanic basalt is not known; when this site 249 basalt was compared to the cored basalts of the adjacent Mozambique Basin, inconclusive results were obtained. The essential constitution of the Mozambique Ridge remains an enigma, but solution of this problem is vital for the proper understanding of the Mesozoic history of this oceanic region. 相似文献
18.
Structures of the northeasternmost South China Sea continental margin and ocean basin: geophysical constraints and tectonic implications 总被引：2，自引：0，他引：2
Chun-Feng Li Zuyi Zhou Jiabiao Li Hujun Hao Jianhua Geng 《Marine Geophysical Researches》2007,28(1):59-79
The northeastern part of the South China Sea is a special region in many aspects of its tectonics. Both recent drilling into
the Mesozoic and new reflection seismic surveys in the area provide a huge amount of data, fostering new understanding of
the continental margin basins and regional tectonic evolution. At least four half-grabens are developed within the Northern
Depression of the Tainan Basin, and all are bounded on their southern edges by northwestward-dipping faults. One of the largest
half-grabens is located immediately to the north of the Central Uplift and shows episodic uplift from the late Oligocene to
late Miocene. Also during that period, the Central Uplift served in part as a material source to the Southern Depression of
the Tainan Basin. The Southern Depression of the Tainan Basin is a trough structure with deep basement (up to 9 km below sealevel
or 6 km beneath the sea bottom) and thick Cenozoic sedimentation (>6 km thick). Beneath the Southern Depression we identified
a strong landward dipping reflector within the crustal layer that represents a significant crustal fault. This reflector coincides
with a sharp boundary in crustal thicknesses and Moho depths. We show that the northeasternmost South China Sea basin, which
may have undergone unique evolution since the late Mesozoic, is markedly different from the central South China Sea basin
and the Huatung Basin, both geologically and geophysically. The Cenozoic evolution of the region was largely influenced by
pre-existing weaknesses due to tectonic inheritance and transition. The South China Sea experienced multiple stages of Cenozoic
extension. 相似文献