西昆仑及邻区岩石圈结构构造演化——塔里木南—西昆仑多学科地学断面简要报道

通过深地震反射剖面,宽频天然深地震探测,广角折射、反射剖面,结合地表地质观察、岩石矿物和地球化学研究,以及弹性模拟计算等,对当前国际上流行的所谓高原北缘向南呈A型俯冲,南缘向北俯冲构成的青藏高原地壳加厚、隆升的“双俯冲”(two-sidedsubduction)模式提出质疑,认为高原北缘至少在西昆仑与塔里木(欧亚板块)之间不存在长距离的俯冲,在新生代以来的强劲挤压中,塔里木起到了一定的阻挡作用,在这里呈现南北向挤压应力场,因而青藏高原西北缘陆-陆碰撞造山、盆山的形成受到“南北双向挤压模式”所控制,也是造成青藏高原西北缘新生代期地壳加厚、隆升的重要动力因素     

TECTONIC EVOLUTION OF THE WESTERN KUNLUN AND KARAKORAM MOUNTAINS—SOME NEW OBSERVATIONS FROM A MULTI-DISCIPLINARY GEOSCIENTIFIC TRANSECT (MGT) IN NW TIBET

TECTONIC EVOLUTION OF THE WESTERN KUNLUN AND KARAKORAM MOUNTAINS—SOME NEW OBSERVATIONS FROM A MULTI-DISCIPLINARY GEOSCIENTIFIC TRANSECT (MGT) IN NW TIBET     

塔里木盆地与天山山脉晚新生代盆山耦合机制

根据塔里木盆地北缘地质构造几何学和运动学资料、油气勘探地震剖面、人工地震测深、地震层析成像以及地热资料,提出了塔里木盆地、准噶尔盆地岩石圈地幔在天山岩石圈之下碰撞并发生拆沉的盆山耦合机制的概念模型。由于印藏碰撞,青藏高原的北部前缘岩石圈地幔与塔里木盆地岩石圈地幔形成V字形碰撞结构,推动塔里木地块的高强度岩石圈向北运动并俯冲到天山岩石圈之下,以水平俯冲作用在中天山北缘岩石圈之下与准噶尔盆地向南俯冲的岩石圈地幔碰撞,并发生后剥拆离。塔里木岩石圈俯冲的过程中,形成库车再生前陆盆地和再生前陆冲断带以及再生天山山脉。冲断量约为塔里木俯冲量的20％。这一盆山耦合模型可以解释盆地构造、盆地沉降、山脉隆升、岩石圈深部构造和热特征。     

A traverse through the western Kunlun (Xinjiang,China): tentative geodynamic implications for the Paleozoic and Mesozoic

The northern part of the western Kunlun (southern margin of the Tarim basin) represents a Sinian rifted margin. To the south of this margin, the Sinian to Paleozoic Proto-Tethys Ocean formed. South-directed subduction of this ocean, beneath the continental southern Kunlun block during the Paleozoic, resulted in the collision between the northern and southern Kunlun blocks during the Devonian. The northern part of the Paleo-Tethys Ocean, located to the south of the southern Kunlun, was subducted to the north beneath the southern Kunlun during the Late Paleozoic to Early Mesozoic. This caused the formation of a subduction-accretion complex, including a sizeable accretionary wedge to the south of the southern Kunlun. A microcontinent (or oceanic plateau?), which we refer to as “Uygur terrane,” collided with the subduction complex during the Late Triassic. Both elements together represent the Kara-Kunlun. Final closure of the Paleo-Tethys Ocean took place during the Early Jurassic when the next southerly located continental block collided with the Kara-Kunlun area. From at least the Late Paleozoic to the Early Jurassic, the Tarim basin must be considered a back-arc region. The Kengxiwar lineament, which “connects” the Karakorum fault in the west and the Ruogiang-Xingxingxia/Altyn-Tagh fault zone in the east, shows signs of a polyphase strike-slip fault along which dextral and sinistral shearing occurred.     

深地震反射剖面揭露青藏高原陆-陆碰撞与地壳生长的深部过程

印度板块与亚洲板块的碰撞使喜马拉雅-青藏高原隆升,地壳增厚并生长扩展。探测青藏高原深部结构,揭露两个大陆如何碰撞以及碰撞如何使大陆变形的过程,是对全球关切的科学奥秘的探索。深地震反射剖面探测是打开这个科学奥秘的最有效途径之一。二十多年来,运用这项高技术探测到青藏高原巨厚地壳的精细结构,攻克了难以得到下地壳和Moho面信息的技术瓶颈,揭露了陆-陆碰撞过程。本文在探测研究成果的基础上,从青藏高原南北-东西对比,再到高原腹地,系统地综述了青藏高原之下印度板块与亚洲板块碰撞-俯冲的深部行为。印度地壳在高原南缘俯冲在喜马拉雅造山带之下,亚洲板块的阿拉善地块岩石圈在北缘向祁连山下俯冲,祁连山地壳向外扩展,塔里木地块与高原西缘的西昆仑发生面对面的碰撞,在高原东缘发现龙日坝断裂(而不是龙门山断裂)是扬子板块的西缘边界,高原腹地Moho面厚度薄而平坦,岩石圈伸展垮塌。多条深反射剖面揭露了在雅鲁藏布江缝合带下印度板块与亚洲板块碰撞的行为,不仅沿雅鲁藏布江缝合带走向印度地壳俯冲行为存在东西变化,而且印度地壳向北行进到拉萨地体内部的位置也不同。在缝合带中部,研究显示印度地壳上地壳与下地壳拆离,上地壳向北仰冲,下地壳向北俯冲,并在俯冲过程中发生物质的回返与构造叠置,这导致印度地壳减薄,喜马拉雅地壳加厚。俯冲印度地壳前缘与亚洲地壳碰撞后沉入地幔,处于亚洲板块前缘的冈底斯岩基与特提斯喜马拉雅近于直立碰撞,冈底斯下地壳呈部分熔融状态,近乎透明的弱反射和局部出现的亮点反射以及近于平的Moho面都反映出亚洲板块南缘处于伸展构造环境。     

东昆仑山南缘大型转换挤压构造带和斜向俯冲作用

东昆仑地体和巴颜喀拉－－松潘甘孜地体之间的会聚边界是一条位于东昆仑南缘的大型转换挤压构造带。研究表明该带的东段（阿尼玛卿段）和西段（东－西大滩段）构造特征不同,阿尼玛卿段的构造以印支期具往南西造山极性的逆冲叠覆岩片和新生代脆性左行走滑构造为特征,东－西大滩段是由220Ma形成的EW向韧性左行走滑剪切带及两则伴生的挤压褶皱断裂带组成,韧性变形持续至20Ma,之后表现为脆性左行走滑构造再活动。因此,东昆仑南缘大型会聚带是一条由东段的“收缩挤压”为主向西段的“转换挤压”逐渐过度的特殊复杂的构造带,它的形成与巴颜喀拉－－松潘甘孜地体往NE方向斜向俯冲于东昆仑地体之下有关。     

深地震反射剖面揭露青藏高原陆-陆碰撞与地壳生长的深部过程

印度板块与亚洲板块的碰撞使喜马拉雅-青藏高原隆升,地壳增厚和生长扩展。探测青藏高原深部结构,揭露两个大陆如何碰撞,碰撞如何使大陆变形的过程,是全球关切的科学奥秘。深地震反射剖面探测是打开这个科学奥秘的最有效途径之一。20多年来,运用这项高技术探测到青藏高原巨厚地壳的精细结构,攻克了难以得到下地壳和Moho清晰结构的技术瓶颈,揭露了陆陆碰撞过程。本文在探测研究成果基础上,从青藏高原南北-东西对比,再到高原腹地,系统地综述了青藏高原之下印度板块与亚洲板块碰撞-俯冲的深部行为。印度地壳在高原南缘俯冲在喜马拉雅造山带之下,亚洲板块的阿拉善地块岩石圈在北缘向祁连山下俯冲,祁连山地壳向外扩展,塔里木地块与高原西缘的西昆仑发生面对面的碰撞,在高原东缘发现龙日坝断裂而不是龙门山断裂是扬子板块的西缘边界,高原腹地Moho 薄而平坦,岩石圈伸展垮塌。多条深反射剖面揭露了在雅鲁藏布江缝合带下印度板块与亚洲板块碰撞的行为,印度地壳不仅沿雅鲁藏布江缝合带存在由西向东的俯冲角度变化,而且其向北行进到拉萨地体内部的位置也不同。在缝合带中部,显示印度地壳上地壳与下地壳拆离,上地壳向北仰冲,下地壳向北俯冲,并在俯冲过程发生物质的回返与构造叠置,使印度地壳减薄,喜马拉雅地壳加厚。俯冲印度地壳前缘与亚洲地壳碰撞后沉入地幔,处于亚洲板块前缘的冈底斯岩基与特提斯喜马拉雅近于直立碰撞,冈底斯下地壳呈部分熔融状态,近乎透明的弱反射和局部出现的亮点反射,以及近于平的Moho都反映出亚洲板块南缘的伸展构造环境。     

西昆仑—塔里木—天山岩石圈深地震探测综述

沿新疆地学断面走廊域实施了3种深地震探测方法：近垂直深地震反射剖面、宽角反射与折射深地震测深剖面和移动式宽频地震观测，揭露出西屁仑-塔里木-天山岩石圈的结构与横向变化，发现了塔里木大陆地块与青藏高原西北部西昆仑造山带碰撞的地震学证据，揭示出天山与塔里木、天山与准噶尔，以及昆仑山与塔里木之间的岩石圈尺度盆山耦合关系。阶段成果发表后引起国内外学者广泛注意，本文结合相关资料对这些新成果进行了系统综述，旨在对比研究青藏高原南北两缘不同的碰撞变形之深部过程。     

西昆仑岩石圈的拆沉作用及其深部构造含义——地震层析成像及航磁异常证据

西昆仑构造带及其邻区的宽频带地震探测和航磁异常研究结果表明,西昆仑构造带的南部(亦即青藏板块)的岩石圈向塔里木盆地下部俯冲,西昆仑的蛇绿岩带是闭合于加里东造山时期的古特提斯洋的残迹;青藏板块在向塔里木盆地俯冲的过程中,受到来自北部坚硬、古老的塔里木地体的强力阻挡,使得向北俯冲的岩石圈产生裂解,发生拆沉;在青藏板块岩石圈发生拆沉作用的同时,南部青藏板块岩石圈的回弹及软流层的浮力作用导致上部地壳发生引张断陷,深部熔岩上涌造成了碱质型熔岩沿断陷裂隙喷溢,同时也形成了构造带两侧反逆冲构造格局;西昆仑中央断裂是青藏高原的“第四缝合带”,北昆仑构造带仅仅是由于在青藏板块岩石圈发生拆沉作用时,西昆仑构造带中地壳浅部物质逆冲于塔里木前陆之上形成的。     

东昆仑大地震的深部构造背景

本文以深地震测深剖面资料揭示的地壳结构形态为切入点 ,探讨东昆仑 8.1级大地震的深部构造背景。沱沱河—小柴旦长 5 0 0km的剖面范围内发现两处大的莫霍面错断 ,分别位于东昆仑 柴达木结合带之下和金沙江断裂之下。青藏高原北部的地壳厚度 6 1～ 75km :莫霍面具有一致南倾 ,逐步加深的产状及弱反射性特征 ;下地壳明显增厚 ,但速度未见明显降低 ;上地壳发育逆冲、走滑断裂 ;地壳中部存在低速层。北邻的柴达木盆地地壳相对刚性 ,厚 5 2± 2km。东昆仑及邻区的壳幔结构有利于强地震孕育。在印度板块向北推挤和柴达木地块的向南插入的区域挤压应力场中 ,青藏高原北部较弱的下地壳缩短增厚 ,变形过程中的蠕滑引起地壳浅部的应力放大。但NE向主压应力的作用不是大地震形成的唯一要素 ,与青藏高原北部各地体侧向运动有关。侧向运动速率和幅度的差异使应力在各地体的边界断裂积累并使其复活。而低速层对形成孕育大地震需要的“立交桥式”的局部应力环境是必不可少的条件。     

新疆西昆仑造山带北缘中元古代帕什托克闪长岩侵入序列及其地质意义

位于塔里木地块西南缘、西昆仑造山带北缘的帕什托克侵入序列由石英闪长岩-石英二长闪长岩组成,类似TTG组合,形成于中元古代晚期。本文从帕什托克侵入序列的地球化学分析出发,通过对该侵入序列两期侵入岩的主量元素和微量元素的研究,讨论了该侵入序列的成因、构造环境和与其相关的板块间地球动力学模式,认为该侵入序列为I型准铝质高钾钙碱性花岗闪长岩系列,属活动板块边缘碰撞前大陆弧花岗岩类,两期侵入岩为同源岩浆演化,母岩浆属壳幔混合源,且岩浆向酸性演化。根据岩浆演化的物理环境和构造环境,推测早古生代库地洋的完全闭合与库地洋壳向塔里木古陆块俯冲消减有关,是塔里木古陆块和柴达木古陆块在Rodinia超级大陆汇聚过程中的产物。     

青藏高原的构造分区及其边界的变形构造特征

宏观构造特征的确立对青藏高原隆升和“动力学建模”具有重要意义。青藏高原是由来自塔里木-中朝板块的北昆仑-阿尔金-祁连地体,华南-东南亚板块的南昆仑地体、可可西里-巴颜喀拉地体和冈瓦纳古陆的羌塘地体、冈底斯地体及喜马拉雅地体等3大板块(或古陆)的6个地体经多次裂解、会聚和陆内俯冲作用拼合而成的巨型“会聚-陆内俯冲型”岩石圈块体,它以青藏高原南缘结合带、青藏高原北缘结合带和青藏高原东缘结合带依次与印度岩石圈块体、塔里木-阿拉善-鄂尔多斯岩石圈块体和扬子岩石圈块体相隔。按现今动力学特征,这一巨型岩石圈块体(一级构造单元)又可进一步划分为喜马拉雅、藏北、青南和昆仑-阿尔金-祁连等4个二级构造单元(地块),它们依次以雅鲁藏布江结合带、西金乌拉-金沙江结合带、中昆仑结合带为界。4个地块又可进一步划分为若干以断裂为界的三级构造单元(地体)。组成青藏岩石圈块体的各构造单元处于统一的地球动力学系统,它总的表现为:在印度板块向欧亚板块持续、强烈俯冲和热的、具柔性流变学特征的青藏块体整体向北北东方向移动的区域构造背景上,其南、北两侧的喜马拉雅地块、昆仑-阿尔金-祁连地块分别向冷的、刚性的印度岩石圈块体和塔里木- 阿拉善-鄂尔多斯岩石圈块体不对称逆冲叠覆。位于青藏高原腹部的藏北地块和青南地块,在深部存在大量低速体向上涌动和整体自西向东扩展的区域构造背景上,前者叠置近南北向挤压,形成以南北向断陷带及北西和北东向共轭走滑为主的构造格局,而青南地块除松潘-甘孜地体显示自北而南的逆冲叠覆外,可可西里-巴颜喀拉地体以逐一向东挤出的左行走滑作用为主,以致整个青南地块呈现向扬子岩石圈块体逆冲扩展和向三江构造带平移扩展。因此,就现今动力学而言,青藏高原在随着时间推移、隆升速度不断加快的同时,还逐渐向外缘的刚性地块扩展,即高原面积在不断增大。因此青藏高原的边界具有扩展性质,按扩展机制可区分两类扩展型动力边界:走滑型扩展边界和逆冲型扩展边界。典型的走滑型扩展边界位于青藏高原北缘的阿尔金山和青藏高原东缘的三江地区,青藏高原南缘的动力边界属典型的逆冲型扩展边界,而位于祁连山和龙门山的动力边界兼有逆冲和走滑双重扩展性质。     

THE EVOLUTIONARY HISTORY OF THE WEST KUNLUN MOUNTAINS: A TECTONIC RECONSTRUCTION BASED ON STUDIES OF MAGMATISM

THE EVOLUTIONARY HISTORY OF THE WEST KUNLUN MOUNTAINS: A TECTONIC RECONSTRUCTION BASED ON STUDIES OF MAGMATISM     

柴达木北缘超高压变质带形成与折返的时限及机制

位于青藏高原北缘的祁连山加里东造山带的形成是阿拉善板块、祁连微板块及柴达木一东昆仑板块在加里东期间汇聚和碰撞的结果。祁连微板块和柴达木一东昆仑板块之间的柴(达木)北缘超高压变质带形成于495～440Ma,是继南祁连洋壳向北俯冲于祁连微板块下形成增生的柴北缘火山岛弧带之后,陆壳深俯冲的产物。柴北缘超高压变质带是在祁连微板块及柴达木一东昆仑板块之间的“正向陆内俯冲”向“斜向陆内俯冲”转化过程中“斜向挤出”机制下折返的,开始折返年龄为470～460Ma,最后的折返时间为400～406Ma。折返构造很好地保存在超高压变质岩石中,并且记录了广泛的退变质作用。     

东昆仑深部结构地震探测研究现状与展望

东昆仑位于青藏高原北部, 是研究青藏高原向北生长的重要地区。该区在印度板块向北俯冲与亚洲阿拉善地块向南挤压下, 新生代构造和地震活动强烈, 是研究青藏高原隆升、构造变形、强震发生机理等问题的极佳试验场。近几十年来, 在东昆仑及邻区开展了大量的地球物理探测, 取得了很多进展, 也存在一些问题。本文通过收集近年来在该研究区开展的人工地震和天然地震探测成果, 综合分析了研究区的壳幔速度结构, 莫霍面形态及各向异性特征, 总结得出以下几点认识: 柴达木盆地南缘上地幔内的北倾界面可能代表早古生代昆仑洋向北俯冲的遗迹; 东昆仑缺乏“山根”, 重力均衡调整对东昆仑莫霍面加深没有起主导作用, 印度板块向北俯冲, 通过青藏高原对柴达木盆地的挤压造成东昆仑地壳垂向增厚。最后我们探讨了东昆仑地区壳幔结构研究的不足, 并对下一步的研究思路和方向进行了展望。     

Late Triassic Granites From the Quxu Batholith Shedding a New Light on the Evolution of the Gangdese Belt in Southern Tibet

The Gangdese magmatic belt formed during Late Triassic to Neogene in the southernmost Lhasa terrane of the Tibetan plateau. It is interpreted as a major component of a continental margin related to the northward subduction of the Neo-Tethys oceanic slab beneath Eurasia and it is the key in understanding the tectonic framework of southern Tibet prior to the India-Eurasia collision. It is widely accepted that northward subduction of the Neo-Tethys oceanic crust formed the Gangdese magmatic belt, but the occurrence of Late Triassic magmatism and the detailed tectonic evolution of southern Tibet are still debated. This work presents new zircon U-Pb-Hf isotope data and whole-rock geochemical compositions of a mylonitic granite pluton in the central Gangdese belt, southern Tibet. Zircon U-Pb dating from two representative samples yields consistent ages of 225.3±1.8 Ma and 229.9±1.5 Ma, respectively, indicating that the granite pluton was formed during the early phase of Late Triassic instead of Early Eocene(47–52 Ma) as previously suggested. Geochemically, the mylonitic granite pluton has a sub-alkaline composition and low-medium K calc-alkaline affinities and it can be defined as an I-type granite with metaluminous features(A/CNK1.1). The analyzed samples are characterized by strong enrichments of LREE and pronounced depletions of Nb, Ta and Ti, suggesting that the granite was generated in an island-arc setting. However, the use of tectonic discrimination diagrams indicates a continental arc setting. Zircon Lu-Hf isotopes indicate that the granite has highly positive εHf(t) values ranging from +13.91 to +15.54(mean value +14.79), reflecting the input of depleted mantle material during its magmatic evolution, consistent with Mg~# numbers. Additionally, the studied samples also reveal relatively young Hf two-stage model ages ranging from 238 Ma to 342 Ma(mean value 292 Ma), suggesting that the pluton was derived from partial melting of juvenile crust. Geochemical discrimination diagrams also suggest that the granite was derived from partial melting of the mafic lower crust. Taking into account both the spatial and temporal distribution of the mylonitic granite, its geochemical fingerprints as well as previous studies, we propose that the northward subduction of the Neo-Tethys oceanic slab beneath the Lhasa terrane had already commenced in Late Triassic(~230 Ma), and that the Late Triassic magmatic events were formed in an active continental margin that subsequently evolved into the numerous subterranes, paleo-island-arcs and multiple collision phases that form the present southern Tibet.     

青藏高原的地幔结构:地幔羽、地幔剪切带及岩石圈俯冲板片的拆沉

通过横穿青藏高原近 80 0 0km长的 4条天然地震层析剖面 ,获得 4 0 0km深度以上的地壳和地幔速度图像及地震波各向异性 ,揭示了青藏高原 4 0 0km深度范围内的地壳和地幔结构特征。地幔速度图像显示 ,青藏高原腹地的深地幔中存在以大型低速异常体为特征的地幔羽 ,其可能通过热通道与大面积分布的可可西里新生代高钾碱性火山作用有成因联系 ;阿尔金、康西瓦、金沙江、嘉黎及雅鲁藏布江等走滑断裂可下延至 30 0～ 4 0 0km深度 ,显示了低速高热物质组成的垂向低速异常带特征及大型超岩石圈或地幔剪切带的产出 ;发现康西瓦、东昆仑—金沙江、班公湖—怒江和雅鲁藏布缝合带下部存在不连续的高速异常带 ,可以解释为青藏高原地体拼合及碰撞过程中可能保留的加里东、古特提斯和中特提斯大洋岩石圈“化石”残片 ,是“拆沉”的地球物理证据。印度大陆岩石圈的巨厚俯冲板片以 15～ 2 0°倾角向北插入唐古拉山下 30 0km深处 ,并被高热物质组成的地幔剪切带分开。结合新的横穿喜马拉雅及青藏高原的地幔层析资料 ,提出青藏高原碰撞动力学新模式 :青藏高原南部印度岩石圈板片的翻卷式陆内超深俯冲 ,北缘克拉通向南的陆内俯冲 ,腹地深部的地幔羽上涌 ,以及地幔范围内的高原“右旋隆升”及物质向东及北东方向运动及挤出。     

East-West Antarctic boundary in McMurdo sound

Common-depth-point seismic reflection profiling indicates that the crust beneath western McMurdo Sound is capped by a thin veneer of layered reflectors. The absence of deep, layered reflectors suggests the crust beneath the coast is made up primarily of intrusions which we associate with plutons generated during the Ross Orogeny. The layered reflectors dip and thicken to the east, away from the coast, where they are found at two-way reflection times of 7 s, corresponding to depths of 14–16 km. Reflection data support earlier refraction, gravity, and magnetic interpretations that indicate fundamental differences in the crust beneath McMurdo Sound and the Transantarctic Mountains. Differences may be due to early Paleozoic subduction of the Ross Embayment crust beneath the Transantarctic Mountains during the Ross Orogeny. Orogeny has produced an over-thickened crust beneath the Ross orogenic belt which was followed by several periods of reactivation including the Jurassic thermal event and the uplift of the present-day Transantarctic Mountains in early Tertiary time. The presence of the McMurdo Volcanics and preliminary interpretations of reflection data suggest that the Sound is now being thinned by processes of extension.     

Cenozoic Volcanism and Intraplate Subduction at the Northern Margin of the Tibetan Plateau

Developed in the Mt.Kunlun orogenic belt at the northern margin of the Tibetan Plateau is an active Cenozoic volcanic zone which is more than 1000km in length and some ten to hundred kilometers in width.It extends east-westwards and is roughly parallet to the strike of Mt.Kunlun.The Cenozoic volcanic rocks are divided into the northern(N-)and southern(S-)subzones.Eruptions of volcanic lavas in the S-subzone are related to an initial rift zone within the north Qiangtang terrane,but the volcanic rocks in the N-subzone are relatively close to the contact zone between the Mt.Kunlun and the Tarim terrane.The space-time distribution,petrological and geochemical features can be explained by a model of southward intraplate subduction of the Tarim terrane.     

塔里木盆地及邻区岩石圈拆离解耦与盆山格局关系的天然地震分析

与洋陆俯冲关系不同,在板内汇聚过程中,大陆岩石圈固有的多圈层、多界面结构的特点,使得地块的俯冲变形伴有多圈层顺层拆离解耦的行为,使变形结构复杂化。虽然多圈层界面拆离解耦所引发的地震点群空间分布不像洋陆俯冲关系那么规则完美,但是依据地震群与破裂位置、破裂与岩石圈分层力学特性的依次控制关系,运用深度/频次、平面密度等统计方法,再以各种地球物理实测手段得到的岩石圈结构构造数据作为界面标定依据,还是能够得出诸如拆离解耦的界面深度、界面归属和区域层间变形范围等重要的几何学信息,这些变形几何学、运动学数据是构建大陆岩石圈板内汇聚造山特别是盆山耦合模式时的关键性的依据。文中通过对塔里木盆地及周缘造山带的相关研究,在岩石圈层拆离解耦状态及其与盆山构造格局之间的关系方面得出以下几点认识:(1)塔里木盆地及周缘造山带岩石圈的主拆离解耦层均发育于中地壳,但随各区中地壳的具体深度位置不同而有所差别;(2)塔西南/西昆仑盆山构造耦合关系是构建于岩石圈尺度上的,塔北/南天山盆山耦合关系是构建于地壳尺度上的;(3)地震活动的密集程度及密集带的展布与天山的变形强度、隆升状态和地貌阶段类型的变化规律有着近乎完美的精确匹配关系;(4)塔北/南天山和塔西南/西昆仑对应于岩石圈的强拆离解耦区,塔东北/东天山和塔东南/阿尔金山之间无耦合关系,其边缘带对应于岩石圈弱拆离解耦和无拆离解耦区;(5)塔里木盆地总体上的弱变形状态与其岩石圈弱或未拆离解耦类型占据总面积90%的情形相适应;(6)塔里木地块以驱动、阻挡约束、平移滚筒约束和克拉通过渡等多重“身份”存在于相邻单元“包围”的力学环境中。