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1.
延边地区渤海地块与兴凯地块之间古缝合带的初步研究 总被引：8，自引：0，他引：8
延边地区地处吉林省的东部。研究区南部为渤海地块，北部为兴凯地块，东部与朝鲜和俄罗斯相毗邻，西部与吉中地区以敦化－密山断裂为界。本文着重介绍延边地区渤海地块北缘及兴凯地块南缘的大陆增生历史和这两个古板块之间的古板块缝合带的地质特征。 相似文献
2.
敦化-密山断裂带的平移距离:来自松嫩-张广才岭-佳木斯-兴凯地块古生代-中生代岩浆作用的制约 总被引：1，自引：0，他引：1
敦化-密山断裂带是郯庐断裂北段的重要分支之一,其大规模左行走滑发生的时限以及平移距离一直存在较大争议。本文系统地总结了松嫩-张广才岭地块东缘、佳木斯地块以及兴凯地块之上古生代-中生代火成岩的锆石U-Pb年代学资料,结合其空间分布特征,对敦化-密山断裂带的平移时限及距离提供了制约。研究表明,松嫩-张广才岭地块东缘与兴凯地块在古生代-中生代期间具有类似的岩浆活动历史,两个地块之上该时期的岩浆作用可以划分为8个主要期次:中-晚寒武世(ca.500~516Ma)、早奥陶世(ca.480~486Ma)、晚奥陶世(ca.450~456Ma)、中志留世(ca.426~430Ma)、早二叠世(ca.285~292Ma)、晚二叠世(ca.255~260Ma)、晚三叠世(ca.202~210Ma)和早侏罗世(ca.185~186Ma)。相比之下,佳木斯地块中的古生代-中生代早期岩浆事件则集中在晚寒武世(~492Ma)、晚泥盆世(~388Ma)、早二叠世(~288Ma)、晚二叠世(~259Ma)和早侏罗世(~176Ma),而晚奥陶世-志留纪和晚三叠世的岩浆活动在佳木斯地块未见报道。早白垩世晚期(ca.105~110Ma)和晚白垩世(ca.90~94Ma)的岩浆活动在三个地块均存在。上述结果表明兴凯地块东缘与松嫩-张广才岭地块东缘在早古生代经历了共同的地质演化历史,而中生代早期,兴凯地块西缘与松嫩-张广才岭地块东缘经历了同样的岩浆作用历史。上述结果暗示,敦化-密山断裂可能经历了至少两次平移,分别发生在中-晚二叠世-早三叠世和中-晚侏罗世-早白垩世,推测其总的平移距离约400km。结合研究区中生代期间的构造演化历史,敦化-密山断裂中生代的左行平移应与中-晚侏罗世-早白垩世期间古太平洋板块(Izanagi板块)的斜向俯冲相联系。 相似文献
3.
延边地区花岗岩的成因类型及其形成的大地构造环境 总被引：9，自引：0，他引：9
延边地区地处吉林省的东部。研究区南部为渤海地块,北部为兴凯地块,东部与朝鲜和俄罗斯相毗邻,西部与吉中地区以敦化－密山断裂为界。本文主要讨论本区寡蠊乖煅莼锥嗡纬傻? 岗岩类问题,并据此对渤海地块与兴凯地块之间的增生、碰撞、缝合等问题进行探讨。 相似文献
4.
中国东北地块群及其构造演化 总被引：4，自引：0，他引：4
东北地块群主要有额尔古纳、兴华、松嫩、佳木斯和兴凯等地块,它们都不是从西伯利亚克拉通分裂出来的,而都具有独立的演化史.额尔古纳、兴华地块参与到西伯利亚板块东南大陆边缘古亚洲洋弧盆体系中,组成岛弧-山弧或弧后盆地的一部分;松嫩、佳木斯和兴凯地块分别为泛古洋和古太平洋作用区内亲西伯利亚和亲华北的地块,具有前白垩纪较复杂的演化史.在较详细讨论了东北地块群的构造演化的基础上,认为东北大地构造格架,除可以划分出西伯利亚板块和华北板块外,还应划分出滨太平洋松嫩-佳木斯联合地块、环太平洋兴凯地块、胶辽地块和那丹哈达地体. 相似文献
5.
郯庐断裂带的前身是3条重要的边界断裂（古郯庐断裂、辽渤断裂和敦化-密山断裂）,因而前白垩纪其两侧的“盆”“山”发育分属不同的造山动力学和成盆动力学系统。其西．扬子微大陆与华北微大陆之间的秦岭-大别造山带是印支期的碰撞造山带,兴-蒙造山带是海西期的阿尔泰型（增生弧型）造山带,燕山运动时两者都成为陆内造山带。“郯庐断裂带”以东,苏鲁造山带是苏皖地块与胶辽微大陆之间的燕山期碰撞造山带,延吉-清津造山带是胶辽微大陆与兴凯地块之间的印支期碰撞造山带;更北则是由一系列外来地体沿敦化-密山断裂拼贴在西伯利亚次大陆之上而形成的斜向汇聚-剪切造山带（属板间造山带）。在此基础上,分为海西-印支期、侏罗纪和白垩纪3个时代,详细剖析了“郯庐断裂带”两侧与上述造山作用耦合的典型的磨拉石盆地和火山岩盆地的演化及其对比,证实前白垩纪“郯庐断裂带”两侧的盆地各有其独立的发育史,不是被郯庐断裂带左行平移错断的同一个盆地。对“郯庐断裂带”两侧古生代-三叠纪陆表海的研究进一步证实其西的扬子微大陆、华北微大陆、布列亚-佳木斯地块与其东的苏皖地块、胶辽微大陆、兴凯地块曾分属独立的构造单元。早白垩世时,随着新特提斯洋的部分闭合,亚洲大陆的雏形出现,上述3条边界断裂连接成郯庐断裂带并成为陆内的左行走滑断层。 相似文献
6.
从郯庐断裂带两侧的“盆”“山”耦合演化
看前白垩纪“郯庐断裂带”的性质 总被引：9，自引：1，他引：8
郯庐断裂带的前身是3条重要的边界断裂（古郯庐断裂、辽渤断裂和敦化-密山断裂）,因而前白垩纪其两侧的“盆”“山”发育分属不同的造山动力学和成盆动力学系统。其西．扬子微大陆与华北微大陆之间的秦岭-大别造山带是印支期的碰撞造山带,兴-蒙造山带是海西期的阿尔泰型（增生弧型）造山带,燕山运动时两者都成为陆内造山带。“郯庐断裂带”以东,苏鲁造山带是苏皖地块与胶辽微大陆之间的燕山期碰撞造山带,延吉-清津造山带是胶辽微大陆与兴凯地块之间的印支期碰撞造山带;更北则是由一系列外来地体沿敦化-密山断裂拼贴在西伯利亚次大陆之上而形成的斜向汇聚-剪切造山带（属板间造山带）。在此基础上,分为海西-印支期、侏罗纪和白垩纪3个时代,详细剖析了“郯庐断裂带”两侧与上述造山作用耦合的典型的磨拉石盆地和火山岩盆地的演化及其对比,证实前白垩纪“郯庐断裂带”两侧的盆地各有其独立的发育史,不是被郯庐断裂带左行平移错断的同一个盆地。对“郯庐断裂带”两侧古生代-三叠纪陆表海的研究进一步证实其西的扬子微大陆、华北微大陆、布列亚-佳木斯地块与其东的苏皖地块、胶辽微大陆、兴凯地块曾分属独立的构造单元。早白垩世时,随着新特提斯洋的部分闭合,亚洲大陆的雏形出现,上述3条边界断裂连接成郯庐断裂带并成为陆内的左行走滑断层。 相似文献
7.
鲁西金刚石原生矿床成矿背景复杂,由于缺乏地壳结构、岩浆侵入体位置、断裂规模等信息作为参考依据,深部构造特征及其在成矿过程中的作用尚不明确。本文基于重磁数据和地震剖面资料,采用Parker Oldenburg界面法、功率谱法和2. 5D重磁震联合反演等方法,获得了鲁西地区地壳结构、断裂规模、岩浆侵入体位置等信息,在此基础上,探讨了金刚石原生矿床的深部构造背景。结果表明：鲁西金刚石原生矿床分布于区域布格重力异常低值区、磁异常中 低值区,布格重力异常平均值低于-100×10-5m/s2,磁异常变化范围较大,介于-160~60 nT之间;矿床位于莫霍面、居里面等值线密集的梯度带,即稳定区域与活化区域的过渡带,莫霍面深度约为31. 2~32. 2 km,居里面深度约27. 5~30 km;矿床分布区NW向断裂构造切割深度均超过20 km,其中蒙山断裂切割深度为35 km,深达上地幔,新泰 垛庄断裂切割深度为28. 5 km,深达居里面,泰山 铜冶店断裂切割深度为20. 5 km;金伯利岩于古生代形成后,受中生代伸展构造影响,被NW向断裂逐级抬升、剥蚀,直至出露地表。金刚石品位自南向北逐渐降低是由于北部抬升幅度大,剥蚀接近金伯利岩根部的结果,指示南部矿带找矿潜力大。 相似文献
8.
青藏高原东北缘六盘山—鄂尔多斯盆地深地震测深剖面沿近东—西向布设长约420km,跨越鄂尔多斯盆地、六盘山和秦祁地块。本文根据沿测线爆破地震的6炮记录截面图中,6个震相的到时资料,结合地震记录中的振幅信息,确定了沿剖面的二维纵波地壳速度结构。鄂尔多斯盆地的地壳平均速度为6.38~6.40km/s,地壳厚度为41.7~48.2km。六盘山地区的地壳平均速度最高为6.40~6.42km/s,地壳厚度最大为53~54km。六盘山以西秦祁地块的地壳平均速度最低为6.32~6.40km/s,地壳厚度为50.3~53km。整个莫霍面形态东浅西深,明显向西倾斜。鄂尔多斯盆地东侧的莫霍面深度最浅为41.7km,六盘山下方莫霍面的深度最深为54km。莫霍面首波Pn在220km之后出现,速度为7.8~8.1km/s。最后讨论了本区的深部特征和盆山结构关系。 相似文献
9.
淮南-溧阳大地电磁剖面与地质结构分析 总被引：8，自引：5，他引：3
研究跨长江中下游成矿带宽频大地电磁测深剖面得出,华北板块与扬子板块的电性差异明显,二者以张八岭隆起为界线,其西侧为合肥沉积盆地,主体电阻率较低。合肥盆地上地壳深度约12km,电阻率约50~500Ω·m,为相对高阻,中下地壳为大片低电阻率,约10~20Ω·m,推测与高温、含盐度、结晶水有关。电性莫霍面深度约34~38km。在张八岭隆起以东,扬子板块导电性较差,电阻率较高,约500~5000Ω·m,主要原因与火山岩侵入活动和中生代灰岩出露地表有关;宁芜盆地和溧阳盆地上地壳电阻率相对较低,中下地壳电阻率较高;溧阳盆地电性莫霍面明显,深度约30~32km;宁芜盆地之下电性莫霍面不明显,可能与岩体侵入有关。宁芜盆地成矿带与燕山期多期次火山侵入活动密切相关,大量富含金属离子的岩浆和热液沿地层界面或断层裂隙上涌,并与沉积围岩发生强烈矿化作用,最终形成了铁、铜、银等多金属矿床。 相似文献
10.
南海北部陆缘的磁异常特征及居里面深度 总被引：4，自引：0，他引：4
为了研究南海北部张裂大陆边缘的地壳热结构,利用船载测量磁力数据,通过功率谱方法反演南海北部陆缘居里等温面,并结合深地震剖面、区域断裂及大地热流分布,讨论了深部热结构状态.结果显示研究区居里面深度在13~26 km之间,在上下陆坡转换带处与莫霍面相交,北东向断裂多位于居里面梯度带上,北西向断裂多具有分割、错断的特点,居里面深度和大地热流值具有相关性.结果揭示了陆架、上陆坡地区磁性体可能主要位于上地壳和下地壳上部,下陆坡及洋壳区地壳与地幔顶部有被磁化的迹象.磁静区位于居里面上隆区边缘,F3断裂和F4断裂之间可能是残留古洋壳.潮汕凹陷和台西南盆地中央隆起是发生底侵的主要区域,F2断裂为其北界. 相似文献
11.
12.
长江中下游成矿带及邻区地壳速度结构：来自利辛-宜兴宽角地震资料的约束 总被引：13，自引：4，他引：9
为了理解长江中下游地区在中生代成矿的深部动力学过程,Sinoprobe-03-02项目于2011年9月至10月,在跨宁芜矿集区和郯庐断裂带实施了从安徽利辛至江苏宜兴450km长的宽角反射/折射地震剖面。速度剖面结果显示,Moho面深度和地壳速度结构在郯庐断裂两侧东西方向存在明显的差异:(1)在东部扬子块体内部,地壳覆盖层厚3~5km,西部的合肥盆地下方,则达到4~7km。(2)剖面平均Moho面深度为30~32km左右,在郯庐断裂下方,Moho面深度在35km左右;在宁芜矿集区下方,Moho面整体深度偏浅,达30~31km左右,但局部范围内,Moho面深度至34km左右。(3)剖面的下地壳平均速度在6.5~6.6km/s左右,在宁芜矿集区下方,下地壳速度偏低,为6.4~6.5km/s左右。剖面上地幔顶部的速度结构平均在8.0~8.2km/s。在宁芜矿集区下方,速度偏低,为7.9~8.1km/s左右。(4)郯庐断裂带的下方,从地表开始,还存在20多千米长的低速异常带,一直延伸到Moho面附近。剖面的宁芜矿集区下方Moho面上隆、下地壳及上地幔的低速异常等壳幔结构特征,预示下地壳不以榴辉岩残体为主,支持燕山期地幔岩浆的上涌和侵入并成矿,是热上涌物质的源地。 相似文献
13.
2-D Crustal thermal structure along Thuadara-Sindad DSS profile across Narmada-Son lineament,central India 总被引：1，自引：0，他引：1
Central India is traversed by a WSW-ENE trending Narmada-Son lineament (NSL) which is characterized by the presence of numerous
hot springs, feeder dykes for Deccan Traps and seismicity all along its length. It is divided in two parts by the Barwani-Sukta
Fault (BSF). To the west of this fault a graben exists, whereas to the east the basement is uplifted between Narmada North
Fault (NNF) and Narmada South Fault (NSF). The present work deals with the 2-D thermal modeling to delineate the crustal thermal
structure of the western part of NSL region along the Thuadara-Sindad Deep Seismic Sounding (DSS) profile which runs almost
in the N-S direction across the NSL. Numerical results of the model reveal that the conductive surface heat flow value in
the region under consideration varies between 45 and 47mW/m2. Out of which 23mW/m2 is the contribution from the mantle heat flow and the remaining from within the crust. The Curie depth is found to vary between
46 and 47 km and is in close agreement with the earlier reported Curie depth estimated from the analysis of MAGSAT data. The
Moho temperature varies between 470 and 500°C. This study suggests that this western part of central Indian region is characterized
by low mantle heat flow which in turn makes the lower crust brittle and amenable to the occurrence of deep focused earthquakes
such as Satpura (1938) earthquake. 相似文献
14.
Chi-Chia Tang Lupei Zhu Chau-Huei Chen Ta-Liang Teng 《Journal of Asian Earth Sciences》2011,41(6):549-570
The Chaochou Fault, a major geological boundary in southern Taiwan is considered to be a part of the convergent plate boundary between the Eurasia Plate and the Philippine Sea Plate. We applied the Common Conversion Point stacking technique to teleseismic radial receiver functions and obtained Moho variation and crustal structure across the Chaochou Fault. In the Eurasia Plate to its west, the Moho depth is about 37 km and the crust is subducting to the east beneath the Philippine Sea Plate with a dip angle of about 30° between the Backbone Belt and the Tananao Schist. In the Philippine Sea Plate, the Moho depth is about 17 km. The Longitudinal Valley marks the collision boundary between the Eurasia Plate and the Philippine Sea Plate. The results suggest that the depth extent of the Chaochou Fault is about 30–35 km and the fault becomes a “shallow-angle” thrust fault at depth. The Common Conversion Point image also shows several bending interfaces of velocity contrast in the crust. We proposed a simple model to explain the Philippine Sea Plate and Eurasia Plate collision process and the observed crustal deformations. 相似文献
15.
D. M. Finlayson I. Lukaszyk C. D. N. Collins E. C. Chudyk 《Australian Journal of Earth Sciences》2013,60(5):717-732
The Otway Basin in southeastern Australia formed on a triangular‐shaped area of extended continental lithosphere during two extensional episodes in Cretaceous to Miocene times. The extent of the offshore continental margin is highlighted by Seasat/Geosat satellite altimeter data. The crustal architecture and structural features across this southeast Australian margin have been interpreted from offshore‐onshore wide‐angle seismic profiling data along the Otway Continental Margin Transect extending from the onshore Lake Condah High, through the town of Portland, to the deep Southern Ocean. Along the Otway Continental Margin Transect, the onshore half‐graben geometry of Early Cretaceous deposition gives way offshore to a 5 km‐thick slope basin (P‐wave velocity 2.2–4.6 km/s) to at least 60 km from the shoreline. At 120 km from the nearest shore in a water depth of 4220 m, sonobuoy data indicate a 4–5 km sedimentary sequence overlying a 7 km thick basement above the Moho at 15 km depth. Major fault zones affect the thickness of basin sequences in the onshore area (Tartwaup Fault Zone and its southeast continuation) and at the seaward edge of the Mussel Platform (Mussel Fault). Upper crustal basement is interpreted to be attenuated and thinned Palaeozoic rocks of the Delamerian and Lachlan Orogens (intruded with Jurassic volcanics) that thin from 16 km onshore to about 3.5 km at 120 km from the nearest shore. Basement rocks comprise a 3 km section with velocity 5.5–5.7 km/s overlying a deeper basement unit with velocity 6.15–6.35 km/s. The Moho shallows from a depth of 30 km onshore to 15 km depth at 120 km from the nearest shore, and then to about 12 km in the deep ocean at the limits of the transect (water depth 5200 m). The continent‐ocean boundary is interpreted to be at a prominent topographic inflection point 170 km from shore at the bottom of the continental slope in 4800 m of water. P‐wave velocities in the lower crust are 6.4–6.8 km/s, overlying a thin transition zone to an upper mantle velocity of 8.05 km/s beneath the Moho. Outstandingly clear Moho reflections seen in deep‐marine profiling data at about 10.3 s two‐way time under the slope basin and continent‐ocean boundary place further strong controls on crustal thickness. There is no evidence of massive high velocity (>7 km/s) intrusives/underplate material in the lower crust nor any synrift or early post‐rift subaerial volcanics, indicating that the Otway continental margin can be considered a non‐volcanic margin, similar in many respects to some parts of the Atlantic Ocean margins e.g. the Nova Scotia ‐ Newfoundland margin off Canada and the Galicia Bank off the Iberian Peninsula. Using this analogue, the prominent gravity feature trending northwest‐southeast at the continent‐ocean boundary may indicate the presence of highly serpentinised mantle material beneath a thin crust, but this has yet to be tested by detailed work. 相似文献
16.
川滇地区重力场特征与地壳变形研究 总被引：10，自引：0，他引：10
对川滇地区重力场特征进行了研究,获得了研究区内地壳厚度分布及变形特征。总体上,研究区内地壳厚度从西北向东南逐渐减小。川滇菱形块体中内部出现了广泛的地壳增厚现象,并可能一直延伸至菱形块体的最南端。丽江-小金河断裂带在重力场特征上表现为龙门山断裂带向西南的延伸,其东侧主体构造走向等特征与扬子地块一致,推测丽江-小金河断裂带与龙门山断裂、红河断裂带一起构成了扬子地块的西边界。滇西地区布格重力一阶导数与现今地壳变形格局总体一致,主体构造方向为北北西-近南北向,代表了“新”构造主体构造线的方向;上延至45km后,主体构造上转变为以近东西向为主。 相似文献
17.
南海西北部重磁场及深部构造特征 总被引：9，自引：3，他引：9
通过对南海重磁数据的重新处理,得到南海西北部自由空间重力异常图、布格重力异常图、磁异常图和化极磁异常图,并对所反映的地球物理场特征加以分析。根据重力场资料对研究区的地壳结构进行了反演计算,结果表明地壳厚度在10～38km之间,总的趋势由陆向洋逐渐减薄,对应于地壳类型从陆壳、过渡壳到洋壳的分布特征。根据磁力资料计算了居里面深度,其埋深变化于11～27km之间,在陆区居里面是下地壳顶界面和莫霍面之间的另一个物性界面,而在海区则接近于莫霍面埋深。 相似文献
18.
Two NE-SW trending wide-angle seismic profiles were surveyed across the Chinese side Two NE-SW trending wide-angle seismic profiles were surveyed across the Chinese side of the Yinggehai (莺歌海) basin (YGHB) with ocean bottom hydrophones (OBHs) and piggyback recorded by onshore stations located on the Hainan (海南)Island.Detailed velocity-depth models were obtained through traveltime modeling and partially constrained by amplitude calculations.More than 15 km Tertiary sedimentary infill within the YGHB can be divided in to three layers with distinct velocity-depth distribution.Overall,the upper layer has a high velocity gradient with 3.8-4.1 km/s at its bottom,consistent with progressive compaction and diagenesls.Its thickness increases gradually towards the basin center,reaching 4.5 km along the southern profile.The middle layer is characterized in its most part as a pronounced low velocity zone (LVZ) with average velocity as low as 3.0 km/s.Its thickness increases from 3.0 to over 4.5 km from NW towards SE.The primary causes of the velocity inversion are high accumulation rate and subsequent under-compaction of sediments.The velocity at the top of the lower layer is estimated at about 4.5 km/s.Despite strong energy source used (4 x 12L airgun array),no reflections can be observed from deeper levels within the basin.Towards NE the basin is bounded sharply by a clear and deep basement fault (Fault No.1),which seems to cut through the entire crust.A typical continental crust with low-velocity middle crust is found beneath the coast of the western Hainan Island.Its thickness is determined to be 28 km and shows no sign of crustal thinning towards the basin.The sharp change in crustal structure across Fault No.1 indicates that the fault is a strike-slip fault.The crustal structure obtained in this study clearly favors the hypothesis that the YGHB is a narrow pull-apart basin formed by strike-slip faulting of the Red River fault zone. 相似文献
19.
The crustal depth section obtained from deep seismic soundings along the Koyna II (Kelsi-Loni) profile, which lies near latitude 18°N roughly in the east-west direction in that part of the Deccan Trap Maharashtra State, India, shows a number of reflection segments below the Deccan Traps down to the Moho discontinuity. A deep fault below the Deccan Traps 13 km east of Mahad divides the entire cross-section including the Moho boundary into two crustal blocks. The reflection segments show updip towards the west coast in the western block. The Moho discontinuity which is at a depth of 39 km near the deep fault starts rising towards the coast, reaching a depth of 31.5 km at the west coast. The eastern block is thrown up by 1.5 km with respect to the western block along the deep fault. A structural contour map of the Moho discontinuity for the Koyna reservoir area has been prepared from the present results and the crustal information obtained along the Koyna I profile (Kaila et al., 1979a), shows that the deep fault in the Koyna area is aligned in the NNW-SSE direction.Refraction seismic data analysis by the wave front method reveals that the thickness of the Deccan Trap increases towards the west coast. The Deccan Trap is 600–700 m thick in the eastern region between Nira (SP 130) and Loni (SP 200) and attains a thickness of 1500 m at 10 km east of the west coast. The longitudinal wave velocity in the Deccan Traps along the profile varies from 4.8 to 5.0 km/sec and in the crystalline basement from 6.0 to 6.15 km/sec. A tentative isopach contour map of the Deccan Traps and a tentative structural contour map of the Pre-Deccan Trap contact have been prepared for the Koyna reservoir area from the results along the Koyna II and Koyna I profiles. A flexure aligned in a NNW-SSE direction, in the Pre-Deccan Trap contact, which is an expression of the deep fault into the basement, has been clearly brought out. The flexure coincides in general with the orientation of the Deccan volcanic scarp in this area. 相似文献
20.
Zahra B. Ashena Vahid E. Ardestani Antonio G. Camacho Ali Dehghani José Fernández 《Arabian Journal of Geosciences》2018,11(3):52
Due to its geological and economic importance, the Zagros Mountains have been investigated by many researchers during the last decades. Nevertheless, in spite of all the studies conducted on the region, there are still some controversial problems concerning the structure of the Zagros Mountains, including crustal depths, demanding more insights into understanding the crustal constraints of the region. Accordingly, we have conducted a gravity study to determine Moho depth map of the Zagros Mountains region, including its major structural domains from the coastal plain of the Persian Gulf to central Iran. The employed data are the densest and most accurate terrestrial gravity data set observed until now with the precision of 5 μGal and resolution of 5 arc-minute by 5 arc-minute. To image Moho depth variations, gravity inversion software GROWTH2.0 is used, proposing the possibility to model stratified structures by means of a semi-objective exploratory 3D inversion approach. The obtained results reveal the crustal thickness of ~?30–35 km underneath the southwestern most Zagros Fold-Thrust Belt increasing northeastward to 48 km. The maximum Moho depth is estimated ~?62 km below the Zagros Mountains belt along the Main Zagros Thrust. Northeast of the study area, an average crustal thickness of 46 km is computed beneath Urumieh–Dokhtar magmatic arc and central Iran. 相似文献