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1.
Siegfried Lallemant Nicolas Chamot-Rooke Xavier Le Pichon Claude Rangin 《Tectonophysics》1989,160(1-4):151-153
During the French-Japanese Kaiko project, Seabeam, seismic and submersible observations were made in the eastern part of the Nankai subduction zone, close to the area of collision between the Izu-Bonin island arc and the Japan margin. The most prominent feature is the Zenisu Ridge, an elongated relief of the Philippine Sea plate running parallel to the Trench. Magnetic anomalies indicate that the crust of the Zenisu Ridge is a part of the Shikoku oceanic basin formed in the Early Miocene, 23 Ma ago and presumably uplifted at a later stage. Structural analysis of seismic data and diving observations lead us to interpret the superficial structure as being due to compressive tectonics. Mapping the acoustic basement reveals that the southeastern flank of the ridge is bounded by a double thrust, both segments being of equal magnitude (vertical offset about 1 to 1.5 km). Geophysical data support the hypothesis of a main thrust cutting through most of the lithosphere and flattening at depth. The overall structure of the surrounding area reveals a compressive deformation zone widening toward the east, the magnitude of the compressive deformation decreasing westward as well as southward of the Zenisu Ridge. 相似文献
2.
Mechanisms of the opening of back-arc systems are analyzed. Limited focal mechanisms of intraplate earthquakes are used to determine the stress regime of an overriding plate. Preliminary analyses show that compressive deviatoric stresses exist in the plate except near the spreading center. Based on this observation “trench suction” does not appear to be the primary force that drives back-arc spreading, since it will result in tensional deviatoric stresses within the overriding plate. Even though “continental pull” is able to satisfy the stress requirements, it does not appear to be a likely mechanism either because of the initiation and subsequent symmetric spreading difficulty associated with such a mechanism. The mechanism we favor is the one that involves the induced convective current in the mantle wedge immediately above the slab. Calculations show that the induced flow is able to generate sufficient stress to break up the overriding lithosphere if the tectonic stresses of the region are favorable. Both trench suction and continental pull may help to provide such a favorable tectonic stress regime. 相似文献
3.
On the role of subducting oceanic plateaus in the development of shallow flat subduction 总被引：2，自引：0，他引：2
Oceanic plateaus, aseismic ridges or seamount chains all have a thickened crust and their subduction has been proposed as a possible mechanism to explain the occurrence of flat subduction and related absence of arc magmatism below Peru, Central Chile and at the Nankai Trough (Japan). Their extra compositional buoyancy could prohibit the slab from sinking into the mantle. With a numerical thermochemical convection model, we simulated the subduction of an oceanic lithosphere that contains an oceanic crustal plateau of 18-km thickness. With a systematic variation, we examined the required physical parameters to obtain shallow flat subduction. Metastability of the basaltic crust in the eclogite stability field is of crucial importance for the slab to remain buoyant throughout the subduction process. In a 44-Ma-old subducting plate, basalt must be able to survive a temperature of 600–700 °C to keep the plate buoyant sufficiently long to cause a flat-slab segment. We found that the maximum yield stress in the slab must be limited to about 600 MPa to allow for the necessary bending to the horizontal. Young slabs show flat subduction for larger parameter ranges than old slabs, since they are less gravitationally unstable and show less resistance against bending. Hydrous weakening of the mantle wedge area and lowermost continent are required to allow for the necessary deformation of a change in subduction style from steep to flat. The maximum flat slab extent is about 300 km, which is sufficient to explain the observed shallow flat subduction near the Nankai Trough (Japan). However, additional mechanisms, such as active overthrusting by an overriding continental plate, need to be invoked to explain the flat-slab segments up to 500 km long below Peru and Central Chile. 相似文献
4.
Two subducting seamounts under inner trench slopes have been identified around Japan on the basis of magnetic anomalies, morphology and geological structure. The first one is located under the foot of the inner trench slope at the junction between the Japan Trench and the Kuril Trench. Another one occurs beneath the slope slightly seaward of the Tosabae (the basement high at the trench slope break along the Nankai Trough off Shikoku). The magnetic anomalies of seamount origin are accompanied by the characteristic morphology of a forearc wedge i.e., a swell landward and a depression seaward. The seamounts beneath the inner trench slopes have preserved magnetization showing reasonably consistent directions, which suggests that the subducting seamounts have kept roughly their original shapes. The morphology of the forearc wedge can be explained by a subducting seamount on the oceanic crust pushing the forearc material forward and upward. Deformation of the forearc wedge by the subducting seamount extends to the forearc basin. The seamounts are stronger and less deformable than the inner slope material and are not offscraped onto inner trench slopes.
Two other examples of deformed inner trench slopes around Japan which can be explained by subduction of topographic highs are presented. One example is a depression on the foot of the inner trench slope northeast of the junction between the Kyushu-Palau Ridge and the Nankai Trough. Another one is an area of complex morphology of the inner trench slope along the Japan Trench around the Daiichi-Kashima Seamount. 相似文献
5.
The 1946 Nankai earthquake (Ms=8.2) at the forearc region of the western Nankai Trough showed slow slip deformation off Cape Muroto, which did not propagate until the western end of the Nankai seismogenic zone. New seismic investigations show a low-velocity layer (LVL) on the subducting oceanic crust in the coseismic area. Two prestack depth-migrated sections show reflectivity events in the clay-rich boundary layer on the oceanic crust. Narrowly spaced imbricated slices develop in the nonrupture area. The reflective boundary layer indicates probably that underplating develops in the nonrupture area rather than the coseismic area. It is suggested that the friction is larger in the nonrupture area than the coseismic area because of the lack of LVL on the oceanic crust, the well developed underplating and the narrowly spaced imbricated thrusts in the nonrupture area. The topographic high of the oceanic crust with about 50 km width and maximum 3 km height is also revealed and is related to bending and thickening of the oceanic crust, the well developed underplating and the narn spaced imbricated thrusts in the nonrupture area. These structural characters may be the reason why the slow slip deformation did not propagate until the western end of the Nankai seismogenic zone and toward the trough side. 相似文献
6.
Tetsuzo Seno Yujiro Ogawa Hidekazu Tokuyama Eiichiro Nishiyama Asahiko Taira 《Tectonophysics》1989,160(1-4):91-116
We discuss several models of the evolution of the trench-trench-trench triple junction off central Honshu during the past 1 m.y. on the basis of plate kinematics, morphology, gravity and seismic reflection profile data available for the area. The study area is characterized by large basins, 7–8 km deep on the inner lower trench slope on the Philippine Sea side and the deep (9 km) Izu-Bonin Trench to the east. Between the basins and the trench, there are 6–7 km-deep basement highs. The triple junction is unstable due to the movement of the Philippine Sea plate at a velocity of 3 cm/yr in WNW direction with respect to Eurasia (Northeast Japan), subparallel to the strike of the Sagami Trough. Generally we can expect the boundary area between the Philippine Sea and Pacific plates to be extended because the Pacific plate is unlikely to follow the retreating Philippine Sea plate due to the obstruction of the southeastern corner of Eurasia. The above peculiar morphology of the junction area could have resulted from this lack of stability. However, there are several possible ways to explain the above morphology.
Our gravity model across the trench-basement high-basin area shows that the basement highs are made of low-density materials (1.8–2 g/cm3). Thus we reject the mantle diapir model which proposes that the basement highs have been formed by diapiric injection of serpentinites between the retreating Philippine Sea plate and the Pacific plate.
The stretched basin model proposes that the basins have been formed by stretching of the Philippine Sea plate wedge. We estimated the extension to be about 10 km at the largest basin. We reconstructed the morphology at 1 Ma by moving the Philippine Sea plate 20 km farther to the east after closing the basins, and thus obtained 8 km depth of the 1 Ma trench, which is similar to that of the present Japan Trench to the north. Although this stretched basin model can explain the formation of the basins and the deep trench, other models are equally possible. For instance, the eduction model explains the origin of the basin by the eduction of the Philippine Sea basement from beneath the basement high, while the accretion model explains the basement highs by the accretion of the Izu-Bonin trench wedge sediments. In both of these models we can reconstruct the 1 Ma trench depth as about 8 km, similar to that of the stretched basin model.
The deformation of the basement of the basins constitutes the best criterion to differentiate between these models. The multi-channel seismic reflection profiles show that the basement of the largest basin is cut by normal faults, in particular at its eastern edge. This suggests that the stretched basin model is most likely. However, the upper part of the sediments shows that the basement high to the east has been recently uplifted. This uplift is probably due to the recent (0.5 Ma) start of accretion of the trench wedge sediments beneath this basement high. 相似文献
7.
The bathymetry and abrupt changes in earthquake seismicity around the eastern end of the Java Trench suggest it is now blocked south–east of Sumba by the Australian, Jurassic-rifted, continental margin forming the largely submarine Roti–Savu Ridge. Plate reconstructions have demonstrated that from at least 45 Ma the Java Trench continued far to the east of Sumba. From about 12 Ma the eastern part of the Java Trench (called Banda Trench) continued as the active plate boundary, located between what was to become Timor Island, then part of the Australian proximal continental slope, and the Banda Volcanic Arc. This Banda Trench began to be obliterated by continental margin-arc collision between about 3.5 and 2 Ma.The present position of the defunct Banda Trench can be located by use of plate reconstructions, earthquake seismology, deep reflection seismology, DSDP 262 results and geological mapping as being buried under the para-autochthon below the foothills of southern Timor. Locating the former trench guides the location of the apparently missing large southern part of the Banda forearc that was carried over the Australian continental margin during the final stage of the period of subduction of that continental margin that lasted from about 12 Ma to about 3.5 Ma.Tectonic collision is defined and distinguished from subduction and rollback. Collision in the southern part of the Banda Arc was initiated when the overriding forearc basement of the upper plate reached the proximal part of the Australian continental slope of the lower plate, and subduction stopped. Collision is characterised by fold and thrust deformation associated with the development of structurally high decollements. This collision deformed the basement and cover of the forearc accretionary prism of the upper plate with part of the unsubducted Australian cover rock sequences from the lower plate. Together with parts of the forearc basement they now form the exposed Banda orogen. The conversion of the northern flank of the Timor Trough from being the distal part of the Banda forearc accretionary prism, carried over the Australian continental margin, into a foreland basin was initiated by the cessation of subduction and simultaneous onset of collisional tectonics.This reinterpretation of the locked eastern end of the Java Trench proposes that, from its termination south of Sumba to at least as far east as Timor, and probably far beyond, the Java-Banda Trench and forearc overrode the subducting Australian proximal continental slope, locally to within 60 km of the shelf break. Part of the proximal forearc's accretionary prism together with part of the proximal continental slope cover sequence were detached and thrust northwards over the Java-Banda Trench and forearc by up to 80 km along the southwards dipping Savu Thrust and Wetar Suture. These reinterpretations explain the present absence of any discernible subduction ocean trench in the southern Banda Arc and the narrowness of the forearc, reduced to 30 km at Atauro, north of East Timor. 相似文献
8.
最近的地震探测表明，在西昆仑和塔里木结合带有岩石圈根存在。据此，本文提出地壳均衡与岩石圈根拖曳共同作用导致“山隆盆降”的动力学机制假说。利用新近中英合作完成的有限元粘弹塑构造数据模拟技术FEVPLIB，模拟研究了青藏高原西部横过西昆仑和塔里木结合带剖面的这一动力学深化过程。这种模式既能解释高原隆升，又能解释边缘沉积盆地的成因。模拟结果表明，两个大陆碰撞到一起，当岩石圈根一旦形成以后，造山水平挤压力主要来源于岩石圈根的向下拖曳，而印度板块向北挤压沦为次要因素。 相似文献
9.
晚新生代中国东部大陆边缘的构造活动主要集中于东海东缘。中新世以来菲律宾海板块俯冲、冲绳海槽弧后张裂、台湾弧-陆碰撞等一系列重大构造过程,塑造了现今琉球沟-弧-盆体系、台湾碰撞造山带和南海东北部的构造-地貌格局。本文基于对重磁和多道地震资料的解译,并结合前人研究成果,恢复了冲绳海槽构造演化史,阐明了冲绳海槽弧后张裂和台湾弧-陆碰撞之间的关系。在此基础上,重建了中新世以来欧亚板块、菲律宾海板块、南海板块之间的相互作用过程模型。本研究有助于进一步理解板块汇聚背景下东亚大陆边缘深部动力-热力过程对浅部构造格局变迁的制约和影响。 相似文献
10.
The Apuseni Mountains are located between the Pannonian Basin and the Transylvanian Basin along a direction of SE convergence with the Carpathian belt. A flexural model based on the cylindrical bending of a semi-infinite, isostatically supported, thin elastic plate is here examined with the Apuseni playing the role of flexural bulge, and under the assumption that the plate is deforming under the action of a vertical shear force and a bending moment applied at the end of the plate, beneath the Carpathians. The model yields estimates of the plate thickness ranging between 13 and 14.5 km, depending on the assumed density contrast between crust/sediments and mantle providing buoyancy. The vertical shear force which is necessary to bend the plate is in the range between 60 and 300 × 1011 N m− 1, depending on the assumed density contrast. This force is shown to be modelled by a gravitational ‘slab pull’ force, using model parameters derived from seismic tomography. If the height of the flexural bulge, after correction for erosion, is allowed to increase, the model yields an estimate of the horizontal strain rate at the top of the bulge. For example, 5 mm/yr vertical change of the flexural bulge of a 14 km thick plate results in a horizontal deformation rate of approximately 7 nanostrain/yr at the top of the bulge, a value which is at the threshold of sensitivity of continuous GPS measurements. Different vertical rates will change the horizontal strain rate almost proportionally. 相似文献
11.
Flexure of the Indian plate and intraplate earthquakes 总被引：2，自引：0，他引：2
The flexural bulge in central India resulting from India's collision with Tibet has a wavelength of approximately 670 km.
It is manifest topographically and in the free-air gravity anomaly and the geoid. Calculations of the stress distribution
within a flexed Indian plate reveal spatial variations throughout the depth of the plate and also a function of distance from
the Himalaya. The wavelength (and therefore local gradient) of stress variation is a function of the effective elastic thickness
of the plate, estimates of which have been proposed to lie in the range 40–120 km. The imposition of this stress field on
the northward moving Indian plate appears fundamental to explaining the current distribution of intraplate earthquakes and
their mechanisms. The current study highlights an outer trough south of the flexural bulge in central India where surface
stresses are double the contiguous compressional stresses to the north and south. The Bhuj, Latur and Koyna earthquakes and
numerous other recent reverse faulting events occurred in this compressional setting. The N/S spatial gradient of stress exceeds
2 bars/km near the flexural bulge. The overall flexural stress distribution provides a physical basis for earthquake hazard
mapping and suggests that areas of central India where no historic earthquakes are recorded may yet be the locus of future
damaging events. 相似文献
12.
在理解岩石圈内部流变分层性和造山带热异常形成与演化多控制因素的基础上，建立了造山带热－应力作用数值模型，研究了不同参数下造山带不同部位蠕动应力场的格局及其演化。其研究结果表明，碰撞终止后岩石圈内部应力调整或热松驰控制了造山带内部不同层次构造样式。在造山带中心，加厚岩石圈在碰撞附加力终止后40Ma，岩石圈应力强度明显减少，可诱发科迪勒拉式后造山伸展作用；在地壳中下层次或岩石圈深部（约40～60km、120～150km）可发生拆沉作用，但非岩石圈地幔的整体拆沉，其动力源自岩石圈套内部相应层位的应力引张；在40Ma以内或在拆沉作用发生前，岩石圈地幔根部及地壳中下层次作为热的应变软化区段，相应控制着Moho面形态及中上地壳构造样式；缝合带及造山带前缘作为应力挤压区，在10Ma可出现局部应力引张，孕育喜马拉雅式伸展。但在宽度巨大的造山带（1000km以上），后造山伸展作用的发生则与带内其它大规模构造活化有关。 相似文献
13.
Jean Benkhelil Mazhar Bayerly Stéphane Branchoux Thierry Courp Eliane Gonthier Christian Hübscher Agnès Maillard Elias Tahchi 《Comptes Rendus Geoscience》2005,337(12):1075-1083
The eastern bend of the Cyprus Arc, at the transition between the submerged Mediterranean subduction and the onshore fault zones that underline the Eurasian, African and Arabic plates boundaries is a submarine feature undergoing a complex tectonic deformation. The BLAC marine geophysical survey helps to better assess the type of the deformation that affects the Messinian to Quaternary sediments along this plate boundary. The deformation, focussed between two tectonic corridors, displays compressive and transpressive features in the central part, becoming thrusting when moving westward in connection with the Cyprus accretionnary wedge. The northeastern end of this submarine range connects with the Latakia Ridge, which is, together with its continental extension, under a tensional tectonic regime. To cite this article: J. Benkhelil et al., C. R. Geoscience 337 (2005). 相似文献
14.
欧亚大陆风云影像线性构造信息提取及其地质分析 总被引：2，自引：1，他引：1
通过欧亚大陆风云影像的空间增强、光谱增强、辐射增强等系列处理和地质解释 ,提取了发育于该区的各种线性构造的相关信息。根据性质和规模将线性构造划分为大洋俯冲带、大陆俯冲带、大陆碰撞带、巨型线性构造、区域线性构造和局部线性构造等六类。文中重点介绍了乌拉尔—阿曼巨型线性构造带和阿尔卑斯大陆碰撞带的影像特征和地质意义。根据各类线性构造的特征和相互关系 ,突出了乌拉尔—阿曼和伊尔库茨克—横断山两条巨型线性构造带的地位 ,并以它们为界划分了三个构造域 :西亚构造域以印度板块的俯冲为特色 ,导致青藏高原的隆升和陆内强烈变形 ;东亚构造域最为重要的特征是太平洋板块的俯冲 ,形成一系列岛弧体系 ,并使大陆内部出现大量岩浆活动和强烈的构造变动 ;欧洲构造域主要为非洲—阿拉伯板块与欧洲板块的碰撞 ,二者之间没有明显的俯冲带 ,而有一个较宽广的接触带 ,强烈的变形集中在这一带内 ,而大陆内部的构造变动比较微弱。这种构造格局在欧亚大地水准面异常图上有明显反映 ,表明与深部地质作用过程有关。三个构造域的主导线性构造的方向组成了一个向南弯曲的弧形 ,弧顶位于西亚构造域。大陆巨型线性构造带呈经向和纬向展布 ,具长期发育特征 ,从更大尺度上看 ,板块边界线性构造也是呈经向和纬? 相似文献
15.
XU Jiren ZHAO Zhixin Institute of Geology Chinese Academy of Geological Science Beijing China Kono Yoshiteru Faculty of Science Kanazawa University Kanazawa - Japan 《Continental Dynamics》2000,(1)
1. IntroductionThe Nankai Trough region (Fig. 1.1) of southwest Japan is one of the most tectonically complex subduction zones in the world. The subduction of the Philippine Sea plate (PH) beneath the Eurasian plate (EU) has caused a series of large and great interplate earthquakes. It is generally accepted that great earthquakes have occurred at intervals of 100-150 years along the Nankai subduction zone since the 684 Hakuho earthquake (Fig. 1.2). However, a large earthquake (M>7.5) has… 相似文献
16.
HUANG Chi-Yue 《地球学报》2009,30(Z1):18-18
Marine surveys show that the submarine Huatung Ridge extends northward to the Lichi Mélange in the southwestern Coastal Range, suggesting that formation of the Lichi Mélange is related to the arcward thrusting of the forearc strata in the western part of the North Luzon Trough during the active arc-continent collision off southern Taiwan. New seismic survey along 21oN transact across over the North Luzon Trough in the in-cipient arc-continent collision zone further reveals that the deformation of the Huatung Ridge occurs soon after the sedimentation in the western forearc basin, while the sedimentation is continuous in the eastern part of the remnant North Luzon Trough until the complete closure of the forearc basin approaching to SE Taiwan. This suggests that the sequence in the Huatung Ridge can just be coeval to the lower sequence of the remnant forearc basin strata. Multiple lines of new evidence, including micropaleontology, clay mineralogy and fis-sion track analyses along the Mukeng River and its tributary key sections, are used to test this thrusting forearc origin hypothesis of the Lichi Mélange. 相似文献
17.
2008年5月12日在青藏高原东缘龙门山断裂带中段发生汶川8.0级特大地震。大震发生时释放应力并对震源区及外围构造应力场产生影响,受汶川地震断层破裂方式和强度空间差异性的影响,震后龙门山断裂带地壳应力场也应表现差异特征,至今鲜有针对该科学问题深入的分析和讨论。经过系统收集、梳理汶川地震后沿龙门山断裂带水压致裂地应力测量数据与2008年汶川地震中强余震序列震源机制解资料,对汶川地震后龙门山断裂带中上地壳构造应力场进行厘定,通过与震前构造应力场对比,深入探讨了汶川8.0级地震对龙门山断裂带地壳应力场的影响,进而对汶川震后应力调整过程及青藏高原东缘龙门山地区深部构造变形模式进行研究,研究结果表明:受汶川8.0级地震的影响,震后龙门山断裂带地壳构造应力场空间分布具有差异性,近地表至上地壳15 km深度范围,映秀—青川段最大主应力方向为北西西向、地应力状态为逆走滑型,青川东北部最大主应力方向偏转至北东东向、应力状态转变为走滑型;15~25km深度范围,龙门山断裂带最大主应力方向仍为北西—北西西向、应力状态以逆冲型为主。汶川8.0级地震后,龙门山断裂带中地壳北西西向逆冲挤压的构造应力特征进一步支持了青藏高原东缘龙门山地区东西两侧刚性块体碰撞挤压、逆冲推覆的动力学模式。 相似文献
18.
The principle of lithostatic pressure is habitually used in metamorphic geology to calculate burial/exhumation depth from pressure given by geobarometry. However, pressure deviation from lithostatic, i.e. tectonic overpressure/underpressure due to deviatoric stress and deformation, is an intrinsic property of flow and fracture in all materials, including rocks under geological conditions. In order to investigate the influences of tectonic overpressure on metamorphic P–T paths, 2D numerical simulations of continental subduction/collision zones were conducted with variable brittle and ductile rheologies of the crust and mantle. The experiments suggest that several regions of significant tectonic overpressure and underpressure may develop inside the slab, in the subduction channel and within the overriding plate during continental collision. The main overpressure region that may influence the P–T paths of HP–UHP rocks is located in the bottom corner of the wedge‐like confined channel with the characteristic magnitude of pressure deviation on the order of ～0.3 GPa and 10–20% from the lithostatic values. The degree of confinement of the subduction channel is the key factor controlling this magnitude. Our models also suggest that subducted crustal rocks, which may not necessarily be exhumed, can be classified into three different groups: (i) UHP‐rocks subjected to significant (≥0.3 GPa) overpressure at intermediate subduction depth (50–70 km, P = 1.5–2.5 GPa) then underpressured at depth ≥100 km (P ≥ 3 GPa); (ii) HP‐rocks subjected to ≥0.3 GPa overpressure at peak P–T conditions reached at 50–70 km depth in the bottom corner of the wedge‐like confined subduction channel (P = 1.5–2.5 GPa); (iii) lower‐pressure rocks formed at shallower depths (≤40 km depth, P ≤ 1 GPa), which are not subjected to significant overpressure and/or underpressure. 相似文献
19.
日本列岛是位于欧亚东缘和西太平洋过渡带上的大陆板块,其来源和成因机制得到了广泛研究,传统上认为其成因是由太平洋俯冲形成的沟弧盆体系的一部分,但仍存在诸多争议。基于地形地貌、地震勘探剖面和盆地构造演化史恢复、古地磁测量和古生物等诸多证据,将南海北部的珠江口盆地、台西南盆地和东海盆地及冲绳海槽的构造迁移进行统一的系统分析,研究结果表明日本大陆板块在新生代由两个区域分别漂移而来。北海道来自赤道附近,而本州、四国和九州来自华南大陆边缘。其成因动力机制与欧亚板块从北大西洋的裂解东漂和印度与欧亚碰撞密切相关,在这个过程中,位于欧亚板块东缘的日本三岛首先发生了裂解,之后发生了漂移。新的大陆漂移模型合理地解释了沟弧盆体系的形成机制和过程,说明了弧状岛弧的成因机制,也给出了所形成的盆地内油气富集的规律。本研究为大陆漂移模式提供了一个新的动力机制。 相似文献
20.
Jean Aubouin 《Tectonophysics》1989,160(1-4):1-3
The main structures of a subduction zone are as follows.
1. (1) On the outer wall: faults, formed either by reactivation of the structural grain of the oceanic plate, when the latter is slightly oblique to the trench, or by a new fault network parallel to the trench, or both. The width of the faulted zone is about 50 miles.
2. (2) On the inner wall: either an accretionary prism or an extensional fault network, or both; collapsed structures and slumps are often associated, sometimes creating confusion with the accretionary structures.
3. (3) The overall structure of the trench itself is determined by the shape of the edge of the continental crust or of the island arc. Its detailed structure, however, is related to the oceanic plate, namely when the structural grain of the latter is slightly oblique to the trench, which then takes an “en echelon” form. Collapsed units can fill up the trench which is, in that case, restricted to an irregular narrow depression; the tectonic framework of the trench can be buried under a sedimentary blanket when the sedimentation rate is high and the trench bottom is a large, flat area.
Two extreme types of active margins can be distinguished: convergent compressive margins, when the accretionary mechanism is strongly active; and convergent extensional margins where the accretionary mechanism is absent or only weakly active.
The status of a given margin between these two extreme types is related to the convergence rate of the plates, the dip of the subduction zone, the sedimentation activity and the presence of a continental obstacle, because oceanic seamounts and aseismic ridges are easily subducted.
Examples are taken from the Barbados, Middle America, Peru, Kuril, Japan, Nankai, Marianna, Manila, New Hebredes and Tonga trenches. 相似文献