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1.
《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
2.
在日本西南部的南海海槽多次发生过俯冲带大地震 ,菲律宾海板块正在这里向日本俯冲。这些地震的复发时间及所影响的地区自１７世纪以来均有文字记载。根据历史文献 ,几乎整个南海海槽（５００ｋｍ长）每１００到２００ａ就被一两个继发性的大地震破坏而产生断裂。１９４４年Ｔｏｎａｎｋａｉ和１９４６年Ｎａｎｋａｉｄｏ的最新地震事件是被详细研究过的南海海槽大地震。关于１９４６年Ｎａｎｋａｉｄｏ地震的断裂过程、地震资料和大地测量资料得出了两个不一致的结果。大地测量资料表明一个面积为２．５×１０４ｋｍ２、滑移量为５至１８ｍ… 相似文献
3.
浊积层——海底沉积物中残留的古代大地震记录 总被引：1，自引：0，他引：1
始于骏河湾的海底大峡谷在伊豆半岛西南海域向南西西转向 ,然后一直延伸到四国海域。骏河湾的谷段被称为骏河海槽 ,转向后的谷段叫南海海槽。这个峡谷状海沟是菲律宾海板块与欧亚板块的汇合带 ,充填着来自日本列岛中部山地的大量泥沙。沿着这条板块汇合带每隔约１００～１５０ａ就发生一次大地震 ,在四国海域叫做南海（道）地震 ,东海海域称为东南海（道）地震 ,在骏河湾谓之东海地震。根据寒川（１９９９）对地震遗迹的考古调查 ,我们了解到在过去的２ｋａ间地震一直以这种间隔持续发生。但是 ,对此之前的地震情况知之甚少。深度超过１ｋｍ… 相似文献
4.
无震脊或海山链俯冲对超俯冲带处的地质效应 总被引：3，自引：1，他引：2
全球海底分布着众多的无震脊或海山链,且在太平洋、印度洋及大西洋均存在靠近俯冲带的海岭。除小安德列斯弧外的巴拉克达脊和蒂勃朗脊起源自转换断层外,一般认为它们由与板块构造动力学迥异的地幔柱动力学所形成的。在板块汇聚边缘处,与扩张脊处所形成的正常洋壳一起,无震脊或海山链俯冲于陆缘弧或洋内弧之下,其对弧及弧后地区的地质效应(构造、地貌、地震以及岩浆作用等)有别于正常洋壳俯冲。无震脊或海山链的俯冲通常造成俯冲带地区的上驮板块的局部异常抬升、俯冲剥蚀作用效应的加强、海沟的向陆迁移以及地震强度的增加。同时,无震脊或海山链俯冲时,其携带的具富集地球化学特征的物质不仅影响着地幔地球化学,也对弧及弧后火山熔岩化学产生明显影响,并对超俯冲地区的热液矿床的形成产生重要影响。最后,本文指出了我国有关无震脊或海山链俯冲的可能的研究方向包括黄岩海山链俯冲对吕宋岛弧的可能影响、印度洋无震脊俯冲对青藏高原局部地区的影响,有我国学者参与的IODP344航次的研究对象——科科斯脊俯冲对哥斯达黎加地震成因的效应以及位于西太平洋地区靠近俯冲带的一些无震脊等。 相似文献
5.
《海洋地质与第四纪地质》2014,(6)
日本南海海槽是菲律宾海板块和欧亚板块俯冲消亡的地带,其东西两段俯冲带的空间重力异常、温度分布和海底热流、地壳结构、应力场特征表现出显著差异。东段四国-纪伊岛下的俯冲带表现出典型的热俯冲带的特征,菲律宾海板块俯冲方向为由南向北,总体特征为俯冲带厚度较薄、俯冲角度小和俯冲深度相当浅等;西段九州岛下的菲律宾海板块由南北方向的俯冲过渡至近东西向,总体表现为俯冲角度大、俯冲深度深、板内震源较浅等特征;这些差异可能是由太平洋板块和菲律宾海板块的运动方向和速率发生了数次的旋转和改变,以及四国海盆的扩张等诸多因素导致的。 相似文献
6.
雅浦俯冲带北段和马里亚纳俯冲带西南端均受加罗林岛脊俯冲影响,但是二者的地球物理特征存在显著差异。通过分析雅浦俯冲带北段和马里亚纳俯冲带的地球物理特征,对比了二者之间的海底地形、重力异常、地震活动和应力场等特征。结果表明：①雅浦海沟北段外缘发育垒堑构造带,马里亚纳海沟西南端加罗林岛脊俯冲区域水深明显变浅,加罗林岛脊俯冲最前端形成凹角。②雅浦岛弧北段和马里亚纳岛弧西南端加罗林岛脊俯冲区域高布格异常值反映了强烈的构造侵蚀可能导致火山弧地壳缺失,岛弧之下高密度物质上涌。③雅浦俯冲带北段和马里亚纳俯冲带西南端地震活动性弱并且缺乏高震级地震,说明加罗林海脊岛脊的俯冲阻塞降低了俯冲带的构造活动性。马里亚纳俯冲带西南端存在少量的中源地震,表明该区域板片俯冲深度比雅浦俯冲带北段更深。④马里亚纳俯冲带西南端的地震存在更多的走滑分量,与加罗林板块的倾斜俯冲、加罗林岛脊的倾斜碰撞有关。⑤加罗林岛脊相对于海沟走向的俯冲角度是造成雅浦俯冲带北段和马里亚纳俯冲带西南端的地球物理特征存在差异的主要原因。 相似文献
7.
数值模拟研究认为洋底高原/洋脊俯冲和弧后扩张能够有效影响俯冲带岩浆活动和岛弧地壳增生。本文以伊豆?博宁?马里亚纳(IBM)俯冲带为实例,论证该结论的有效性。以卫星测高反演重力异常为基础,通过构建地球不同圈层密度模型,反演得到IBM俯冲带莫霍面埋深。本文的莫霍面埋深反演结果与地震解释结果具有一致的分布趋势。结合开源水深和沉积层厚度数据,给出了IBM俯冲带地壳厚度分布。IBM岛弧地壳体积沿走向的分布特征表明:①小笠原洋底高原和相对较小规模达顿洋脊的俯冲,都能够使得相应位置的岛弧变窄、地壳变厚、体积增大;②马里亚纳海槽扩张显著降低了岛弧地壳体积的增生量。 相似文献
8.
《海洋地质与第四纪地质》2007,27(5):8-8,44
9月21日,日本大洋钻探船“地球”号载着科学家离开Shingu港,执行“综合大洋钻探计划”(IODP)第314航次———南海地震区域实验项目(图1)正式开始科学钻探。图1 IODP第134航次钻探位置日本是个地震灾害严重的国家,震源主要来自太平洋的俯冲带。要理解地震如何发生、对地震作预报,必须研究引发地震的源头,监测太平洋板块在海底向下俯冲的运动。位于日本西南海岸的南海海槽,几百万年以来已经引起了多次大规模的地震和海啸,包括1944年和1946年历史上著名的大地震两次地震按里克特震级算分别达到了8·1级和8·级。科学家将从这一俯冲区采集地… 相似文献
9.
岩石生热率是研究地球内热的一个重要的参数。根据自然伽马与岩石生热率的关系,利用盆地4口钻井的自然伽马测井曲线,计算出桑托斯盆地主要岩石或矿物及地层的生热率。统计了2 964个自然伽马测井数据值,主要岩石或矿物的生热率从大到小依次为：泥岩、砂岩、页岩、玄武岩、石灰岩、硬石膏和盐岩;盆地地层的生热率随深度增加显著降低,生热率体现出受控于岩性变化的特征。以S1井为例,根据岩石生热率和热流的关系,计算出盆地中各个组的生热率,Marambaia组、Itajai-Acu组、Itanhaem组、Ariri组、Guaratiba群、Camboriu组生热率分别是（1.36±0.16）μW/m3、（1.52±0.15）μW/m3、（1.30±0.3）μW/m3、（0.46±0.18）μW/m3、（0.64±0.23）μW/m3、（0.37±0.07）μW/m3,盆地沉积地层产生的热量占表层大地热流的13.62%,因此沉积地层具有一定的产热潜力,对区域有机质的成熟度有一定的影响。建立了岩石圈分层生热模型,其中地壳热流贡献为15.38 mW/m2,占表层大地热流的30.76%,地幔热流贡献值为34.62 mW/m2,地壳和地幔的热流比例为0.44,具有“冷壳热幔”的特征。 相似文献
10.
《海洋地质与第四纪地质》2010,(6)
<正>日本南海海槽地震带实验(NanTroSEIZE)是一个并列和复合勘探项目,通过沿俯冲逆掩带的直接取样、现场测量、与实验室相连接的长期监测以及数字模拟,调查和研究断层力学和地震成因。南海海槽地震 相似文献
11.
日本九州俯冲带是菲律宾海板块与欧亚板块汇聚边界上一个独具特色的区域, 也是研究俯冲带内板块构造作用的理想场所。为了解该俯冲带内的板间应力状态和相互作用, 本研究利用震源深度大于20km的97251个地震事件, 通过b值计算详细刻画了该俯冲板片上表面以及垂直海沟走向的剖面特征。结果发现, b值表现出明显的空间变化, 整体上沿南海海槽和琉球海沟从东北往西南方向逐渐增大, 同时在俯冲的九州-帕劳海脊上存在显著的低值区。从b值与应力的负相关性推断, 进入俯冲带的海脊以及海脊东北侧的四国海盆洋壳与俯冲带上覆板片耦合作用较强; 而在海脊西南侧, 俯冲带内汇聚板片的耦合作用相对较弱。究其原因, 本文认为九州-帕劳海脊两侧俯冲洋壳在形成时代和汇聚速率上的差异起着重要作用。对于九州-帕劳海脊来说, 俯冲带浅部的低b值区主要是由于隆起的海脊增强了与上覆板块的耦合作用。随着俯冲深度的增加和俯冲板片倾角的急剧变陡, 沿海脊可能发生了板片撕裂, 从而释放了海脊与上覆板片间的挤压-剪切应力, 使耦合程度大大减弱。 相似文献
12.
Tectonic implications of the subduction of the Kyushu-Palau Ridge beneath the Kyushu,southwest Japan
Chenglong Xia Yanpeng Zheng Baohua Liu Qingfeng Hua Long Ma Xianfeng Li Qiuhong Xie 《海洋学报(英文版)》2021,40(3):70-83
The Kyushu-Palau Ridge(KPR), a remnant arc on the Philippine Sea Plate(PSP), is subducting beneath the Kyushu, southwest Japan. Influenced by the subducting KPR, the Kyushu subduction zone corresponding to the KPR is significantly different from Shikoku subduction zone in terms of gravity anomalies, seismicity, the stress state, and the subducting slab morphology. Significant negative free-air and Bouguer gravity anomalies are observed in a prolonged area of KPR, southeast of the Miyazaki Plain, indicating that this is where KPR overlaps the overriding plate. The gravity anomaly in this area is much lower than that in other areas where the inferred KPR extends, suggesting that the subduction of the buoyant KPR may cause the lower mantle density to decrease.More earthquakes have occurred in Hyuga-nada region where the KPR subducts than in Shikoku forearc and other areas in the Kyushu forearc, indicating that the subduction of the KPR enhances the local coupling between the subducting and overriding plates. The centroid moment tensor(CMT) mechanism of earthquakes shows that stress is concentrated in the accumulated crust beneath the Kyushu forearc corresponding to the KPR, and the shallow thrusting events in the obducting plate are caused by the KPR subduction. The buoyant KPR, with a large volume of low-density sediments, was responsible for the differences of the subduction depth and dip angle of the subducting Philippine Sea(PS) slab between northern Kyushu and Shikoku. The seismic gaps and the sudden change of the dipping angle of the subducting PS slab indicate that slab tear may have occurred along the west side of the KPR beneath southwest Kyushu. A two-tear model was proposed, and the subduction of the buoyant KPR was believed to play an important role in the slab tear. 相似文献
13.
The Philippine Sea Plate has an extremely special tectonic background. As an oceanic plate, it is almost entirely surrounded by subduction zones with complex internal tectonic features. On the basis of enormous published literature, this paper offers a comprehensive overview of the tectonic and evolution history of the Philippine Basin and the Kyushu-Palau Ridge (KPR) in the Philippine Sea Plate, and discusses the geological features of KPR. Referring to relevant definitions of various "ridges" stipulated in United Nations Convention on the Law of the Sea, so the KPR is believed to be a remnant arc formed during the opening of the Parece Vela and Shikoku Basins in the Philippine Sea Plate. It is a submarine ridge on oceanic plate rather than a submarine elevation. And thus, it is not a natural component of the Japan continental margin. 相似文献
14.
Lucia Villar-Muñoz Jan H. Behrmann Juan Diaz-Naveas Dirk Klaeschen Jens Karstens 《Geo-Marine Letters》2014,34(2-3):185-198
Between 33°S and 47°S, the southern Chile forearc is affected by the subduction of the aseismic Juan Fernandez Ridge, several major oceanic fracture zones on the subducting Nazca Plate, the active Chile Ridge spreading centre, and the underthrusting Antarctic Plate. The heat flow through the forearc was estimated using the depth of the bottom simulating reflector obtained from a comprehensive database of reflection seismic profiles. On the upper and middle continental slope along the whole forearc, heat flow is about 30–60 mW m–2, a range of values common for the continental basement and overlying slope sediments. The actively deforming accretionary wedge on the lower slope, however, in places shows heat flow reaching about 90 mW m–2. This indicates that advecting pore fluids from deeper in the subduction zone may transport a substantial part of the heat there. The large size of the anomalies suggests that fluid advection and outflow at the seafloor is overall diffuse, rather than being restricted to individual fault structures or mud volcanoes and mud mounds. One large area with very high heat flow is associated with a major tectonic feature. Thus, above the subducting Chile Ridge at 46°S, values of up to 280 mW m–2 indicate that the overriding South American Plate is effectively heated by subjacent zero-age oceanic plate material. 相似文献
15.
Abyssal currents along the northern periphery of the Shikoku Basin south of Japan were measured by current meters moored off Cape Daio-zaki, Cape Shiono-misaki and Cape Ashizuri-misaki and on the eastern foot of the northernmost part of the Kyushu-Palau Ridge. Total length of observation off Cape Shiono-misaki was about five years including the periods of the Kuroshio large meander and no meander. Analyses of current data show:
- Mean currents with a magnitude of 5–10 cm sec?1 were observed during the whole observation period at all of current meters which were set 400 m above the sea bottom that was deeper than 4,500 m. The mean current for each current meter was parallel to the local bottom contour arond each station and was toward a direction looking the Nankai Trough (a trough located along the northern end of the Shikoku Basin) to the left.
- At each station located above the shelf toe off Cape Daio-zaki and off Cape Shiono-misaki and on the foot of the Kyushu-Palau Ridge, the mean current increases with depth (a bottomward intensification of the mean current), and the vertical extent of the mean current is estimated to be about 2,000 m above the sea bottom.
- At a station located at 2,600 m depth on the continental slope off Cape Shiono-misaki, no bottom-ward intensification of currents was observed.
16.
Tsutomu Nakazawa Akira Nishimura Yasufumi Iryu Tsutomu Yamada Hiroshi Shibasaki Satoshi Shiokawa 《Marine Geology》2008,247(1-2):35-45
Carbonate rock cores drilled on the Kikai Seamount, northern Philippine Sea are examined for better understanding of tectonic history of the northern Philippine Sea. The Kikai Seamount, the summit of which is at 1960 m water depth, is an isolated high on the northwestern part of the Amami Plateau formed by subduction-related arc volcanism, and is situated close to the axis of the Ryukyu Trench in front of the Ryukyu Arc, SW Japan. The seamount is capped with shallow-water carbonates such as coral rudstone. Detailed examinations of lithology, larger foraminiferal assemblages, and Sr isotope composition reveal that the core material comprises Miocene carbonates unconformably overlain by Early Pleistocene carbonates. It indicates rapid subsidence of the Kikai Seamount since the Early Pleistocene. The most probable cause of rapid subsidence is collision and subduction of the Amami Plateau laden with the Kikai Seamount. The rapid subsidence may have started when the western corner of the plateau reached the Ryukyu Trench and began subduction beneath the Ryukyu Arc. The onset of the subsidence is likely to be controlled by a motion change in the Philippine Sea Plate. The latest change in subduction direction from north to northwestward into northwestward to west has been believed to have occurred at 1-2 Ma during latest Pliocene to Early Pleistocene time. The change of direction resulted in the shift from oblique into right-angle subduction of the plate beneath the Ryukyu Arc and also the onset of the collision and subduction of the Amami Plateau. 相似文献
17.
High quality CTD data were collected in the north of the Shikoku Basin where an abyssal boundary current has been observed through direct current measurements. Analyses of hydrographic data showed:
- Colder and saltier water (heavier water) compared to surrounding waters is found above the continental shelf-toe and the eastern flank of the Kyushu-Palau Ridge where the existence of the abyssal boundary current has been expected. The heavier water has a horizontal extent of about 50 km.
- The heavier water has the vertical scale of 2000 m from the sea bottom, and is associated with a thermal wind shear which enhances a component of the flow toward a direction looking the Nankai Trough (a trough located along the northern end of the Shikoku Basin) to the left in the abyss. The assumed “level of no motion” at about 2500 m depth gives the geostrophically estimated current in a good agreement with the directly measured current.
18.
The southwestern margin of the Japan Arc evolved in the geodynamic regime of continental rifting during the Miocene–Pleistocene. This has been verified by broad manifestations of metasomatosis of mantle peridotites that underlie the lithosphere of the Japan Islands and by episodes of deep magmatism (kimberlites and melilitites) in the region. The high enrichment of deep melts in incompatible rare and rare earth elements is partially preserved in melts of regional basalts from smaller depths. In contrast, spreading basalts of the Sea of Japan and subduction basalts from the Nankai trench at the boundary with the Philippine Plate are extremely depleted in rare elements. 相似文献
19.
Dominguez S. Lallemand S. Malavieille J. Schnürle P. 《Marine Geophysical Researches》1998,20(5):383-402
The Gagua Ridge, carried by the Philippine Sea Plate, is subducting obliquely beneath the southernmost Ryukyu Margin. Bathymetric swath-mapping, performed during the ACT survey (Active Collision in Taiwan), indicates that, due to the high obliquity of plate convergence, slip partitioning occurs within the Ryukyu accretionary wedge. A transcurrent fault, trending N95° E, is observed at the rear of the accretionary wedge. Evidence of right lateral motion along this shear zone, called the Yaeyama Fault, suggests that it accommodates part of the lateral component of the oblique convergence. The subduction of the ridge disturbs this tectonic setting and significantly deforms the Ryukyu Margin. The ridge strongly indents the front of the accretionary wedge and uplifts part of the forearc basin. In the frontal part of the margin, directly in the axis of the ridge, localized transpressive and transtensional structures can be observed superimposed on the uplifted accretionary complex. As shown by sandbox experiments, these N330° E to N30° E trending fractures result from the increasing compressional stress induced by the subduction of the ridge. Analog experiments have also shown that the reentrant associated with oblique ridge subduction exhibits a specific shape that can be correlated with the relative plate motion azimuth.These data, together with the study of the margin deformation, the uplift of the forearc basin and geodetic data, show that the subduction of the Gagua Ridge beneath the accretionary wedge occurs along an azimuth which is about 20° less oblique than the convergence between the PSP and the Ryukyu Arc. Taking into account the opening of the Okinawa backarc basin and partitioning at the rear of the accretionary wedge, convergence between the ridge and the overriding accretionary wedge appears to be close to N345° E and thus, occurs at a rate close to 9 cm yr–1. As a result, we estimate that a motion of 3.7 cm yr–1±0.7 cm should be absorbed along the transcurrent fault. Based on these assumptions, the plate tectonic reconstruction reveals that the subducted segment of the Gagua Ridge, associated with the observable margin deformations, could have started subducting less than 1 m.y. ago. 相似文献
20.
The Nankai Trough located southeast of Shikoku Island, Japan, exhibits a zone of exceptionally high heat flow. In the central part of the Nankai Trough the fossil spreading centre of the Shikoku Basin is subducted beneath the southwest Japan arc. We have modelled the temperature and maturation history along the Muroto Transect reaching from the tip of the thrust zone out into nearly undeformed Quaternary and Tertiary sediments seawards of Nankai Trough. We used two balanced cross-sections defining the sections before and after overthrusting as input for 2D-basin modelling. We can show that rapid burial and overthrusting during the Quaternary in combination with a heat flow history following the cooling curve of a 15 Ma old oceanic plate is not sufficient to explain the measured maturity of organic material in the sediments. Several heat flow scenarios derived from theoretical concepts [Yamano, M., Kinoshita, M., Goto, S., Matsubayashi, O., 2003. Extremely high heat flow anomaly in the middle part of the Nankai Trough. Physics and Chemistry of the Earth, Parts A/B/C 28, 487–497.] and previous modelling approaches [e.g. Brown, K.M., Saffer, D.M., Bekins, B.A., 2001. Smectite diagenesis, pore water freshening, and fluid flow at the toe of the Nankai wedge. Earth and Planetary Science Letters 194, 97–109; Spinelli, G.A., Underwood, M.B., 2005. Modeling thermal history of subducting crust in Nankai Trough: constraints from in situ sediment temperature and diagenetic reaction progress. Geophysical Research Letters 32(L09301): doi:10.1029/2005GL022793; Steurer, J., Underwood, M.B., 2003. Clay mineralogy of mudstones from the Nankai Trough reference sites 1173 and 1177 and frontal accretionary prism site 1174. In: H. Mikada et al. (Eds.), pp. 1–37. Available from: <http://www-odp.tamu.edu/publications/190196SR/VOLUME/CHAPTERS/211.PDF>] were tested. The best match between observed maturity levels, temperature and heat flow measurements is reached for a heat flow history which initially assumes the cooling of a 15 Ma old oceanic lithosphere but is reheated to 170–180 mW/m2 during the phase of rapid burial in the Quaternary. This can be achieved either by assuming the onset of hydrothermal circulation in the cooling crust or by reheating caused by off-axis volcanism at about 6 Ma [Yamano, M., Kinoshita, M., Goto, S., Matsubayashi, O., 2003. Extremely high heat flow anomaly in the middle part of the Nankai Trough. Physics and Chemistry of the Earth, Parts A/B/C 28, 487–497.]. 相似文献