欧亚地区均衡残差大地水准面和上地幔强度

首先计算了欧亚地区均衡残差大地水准面．基于地幔热对流的内负荷理论和最新全球层析成像结果，探讨了欧亚地区中波长均衡残差大地水准面的地球动力学意义．研究结果表明，中波长均衡残差大地水准面主要受上地幔粘滞度和岩石层强度的影响，进而得出欧亚地区一些古老地盾和构造稳定地区的上地幔与年轻山脉及构造活动地区的上地幔结构存在着差异．这个差异主要是占老地盾和构造稳定地区，如波罗的海地盾、中西伯利亚地台、东欧等区域，冷却的上地幔已穿透地幔较深，上地幔与岩石层之间耦合较好;而年轻山脉和构造活动区，如帕米尔、天山、贝加尔活动带、青藏高原、日本海周围地区，在上地幔可能存在着热物质即粘滞度很低的软流层，上地幔与岩石层耦合程度较差，甚至有可能解耦．从欧亚地区上地幔属性的差异，可以解释该地区的一些地球动力学问题．     

欧亚地区均衡残差大地水准面和上地幔强度

首先计算了欧亚地区均衡残差大地水准面．基于地幔热对流的内负荷理论和最新全球层析成像结果,探讨了欧亚地区中波长均衡残差大地水准面的地球动力学意义．研究结果表明,中波长均衡残差大地水准面主要受上地幔粘滞度和岩石层强度的影响,进而得出欧亚地区一些古老地盾和构造稳定地区的上地幔与年轻山脉及构造活动地区的上地幔结构存在着差异．这个差异主要是占老地盾和构造稳定地区,如波罗的海地盾、中西伯利亚地台、东欧等区域,冷却的上地幔已穿透地幔较深,上地幔与岩石层之间耦合较好;而年轻山脉和构造活动区,如帕米尔、天山、贝加尔活动带、青藏高原、日本海周围地区,在上地幔可能存在着热物质即粘滞度很低的软流层,上地幔与岩石层耦合程度较差,甚至有可能解耦．从欧亚地区上地幔属性的差异,可以解释该地区的一些地球动力学问题．     

Thickness and thermal history of continental crust and root zones

The survival to the present of the Archean nuclei of Precambrian shields requires special explanation if, as seems likely, the rate of heat flow out of the earth was two or three times greater in the late Archean (2.5 b.y. ago) than at present, since such a high heat flux would have melted the base of the Archean crust. It is proposed that there must have existed beneath stable continental crust a root zone (or lithosphere, or tectosphere) at least 200 km thick which has acted as a thermal buffer between the crust and the convecting mantle; this is virtually the same model as has been proposed to explain the present distribution of heat flow between continents and oceans. The strong temperature dependence of silicate rheology insures that the mantle temperature at the base of the root zone was no more than about 150°C higher in the late Archean than at present; the greater Archean heat flux would have been removed mainly through faster sea-floor spreading. To have survived, the root zone must be mechanically and chemically distinct from the rest of the mantle, and its formation was probably intimately related to the differentiation and stabilization of the continental crust.     

Seismic tomography beneath the orogenic belts and adjacent basins of northwestern China

Three-dimensional velocity images of the crust and upper mantle beneath orogenic belts and adjacent basins of the northwestern continent of China are reconstructed by seismic tomography, based on arrival data of P wave recorded in seismic networks in Xinjiang, Qinghai, Gansu of China and Kyrgyzstan. The velocity images of upper crust demonstrate the tectonic framework on the ground surface. High velocities are observed beneath orogenic belts, and low velocities are observed in the basins and depressions that are obviously related to unconsolidated sediments. The velocity image in mid-crust maintains the above features, and in addition low velocities appear in some earthquake regions and a low velocity boundary separates the western Tianshan Mts. from eastern Tianshan Mts. The orogenic belts and the northern Tibetan plateau have a Moho depth over 50 km, whereas the depths of the Moho in basins and depressions are smaller than 50 km. The velocity images of upper mantle clearly reveal the colliding relationship and location of deep boundaries of the continental blocks in northwestern China, indicating a weakness of the upper mantle structure of orogenic belts. The top depth of upper mantle asthenosphere varies from place to place. It seems shallower under the northern Tibetan plateau, Altay and Qilian Mts., and deeper under the Tarim and Tianshan regions. Hot mantle probably rose to the bottom of some orogenic belts along tectonic boundaries when continental blocks collided to each other. Therefore their dynamic features are closely correlated to the formation and evolution of orogenic belts in northwestern China.     

中国西北大陆碰撞带的深部特征及其动力学意义

以中国大陆西北地区地震层析成像的结果为基础,通过分析大陆块体内部岩石层和软流层的深部形态,提出西部造山带与相邻块体之间几种可能的碰撞类型：天山与塔里木之间存在地块的嵌入拼合、俯冲、岩石层拆离下沉以及层间插入等多种构造样式;青藏高原与北部地质单元之间存在十分清晰的深部边界,反映出上地幔物质向北扩展的痕迹;推测青藏高原的岩石层在向北运动的过程中由于受到塔里木刚性块体的阻滞发生弯曲甚至折断,但是祁连山以北较浅的软流层相当于一个开放边界,使高原的上地幔物质得以进一步向北迁移.大陆碰撞不仅造成中国西部造山带岩石层结构的变动,而且导致软流层中一部分熔融的岩浆体沿着碰撞边界上涌到岩石层底部,它们对青藏高原以及西部造山带的形成演化起到重要的作用.     

中国西北大陆碰撞带的深部特征及其动力学意义

以中国大陆西北地区地震层析成像的结果为基础，通过分析大陆块体内部岩石层和软流层的深部形态，提出西部造山带与相邻块体之间几种可能的碰撞类型：天山与塔里木之间存在地块的嵌入拼合、俯冲、岩石层拆离下沉以及层间插入等多种构造样式；青藏高原与北部地质单元之间存在十分清晰的深部边界，反映出上地幔物质向北扩展的痕迹；推测青藏高原的岩石层在向北运动的过程中由于受到塔里木刚性块体的阻滞发生弯曲甚至折断，但是祁连山以北较浅的软流层相当于一个开放边界，使高原的上地幔物质得以进一步向北迁移.大陆碰撞不仅造成中国西部造山带岩石层结构的变动，而且导致软流层中一部分熔融的岩浆体沿着碰撞边界上涌到岩石层底部，它们对青藏高原以及西部造山带的形成演化起到重要的作用.     

西昆仑造山带下岩石圈地幔速度结构

在已完成的新疆地学断面研究计划实施中曾在西昆仑山前布置了14个宽频带地震台站.利用记录到的远震P波初至和层析成像方法,研究了西昆仑造山带下的岩石圈地幔结构特征.在已有地震学证据基础上,层析成像结果显示,西昆仑造山带下的高速岩石圈地幔可能是印度岩石圈地幔的俯冲前缘.沿东经80°深度剖面图像显示,在西昆仑造山带下的150～300km处,高速异常的岩石圈地幔前锋与低速异常的塔里木块体岩石圈地幔发生了面对面碰撞.     

On the possible density inversion in the upper mantle of the earth

The possible density inversion throughout seismic wave-guides beneath ocean basins and continental structures (without shields) is discussed in accordance with upper-mantle velocity models, thermodynamic properties of deep matter and temperature profiles. The problem is numerically solved. No density inversion in the upper mantle beneath ancient shields is indicated.     

伽师强震群的深部动力学条件

根据天山造山带及其两侧的塔里木盆地和准噶尔盆地的岩石圈二维速度结构、二维密度结构、二维电性结构、壳幔过渡带的详细结构以及大地热流和震源深度的分布,再结合对新疆西北部的蛇绿岩带、高压变质带和岩浆岩分布的综合分析,建立了天山造山带的地球动力学“层间插入消减”模型。该模型认为,塔里木板块的中上地壳在库尔勒断裂附近向天山造山带的中下地壳层间插入;而下地壳连同岩石圈地幔向天山造山带的上地幔俯冲消减。在天山的西段（哈萨克斯坦境内）,费尔干纳地块由北向南插入到南天山之下约180km的深处,在其东段（中国境内）,塔里木盆地由南向北插入南天山之下。这两个具有不同方向的下降板片的接触部位为费尔干纳走滑断裂。我国的伽师、喀什、乌恰地震区均落在这两个具有不同俯冲方向板块的结合部位附近,有着特殊的深部构造背景。南、北两大板块的双向挤压必定产生强大的应力,在地震区附近,这种应力的积累与释放具有4个显著的特点：（1）板片的俯冲消减速度约高达每年22mm左右;（2）应力的积累与释放速率加快;（3）应力释放较容易;（4）应力释放较为集中。这4个特点可能是伽师地区在较短的时间内连续发生数次强震的构造因素。     

大别—苏鲁及邻区上地幔的各向异性

大别—苏鲁是扬子与华北的碰撞造山带,对该地区上地幔各向异性的研究有助于了解该区的地幔动力学机制.本文选用了中国数字化地震台网和区域数字地震台网(山东、安徽、江苏、河南、湖北)三分量宽频带的远震地震波形数据,分别采用最小能量法和旋转相关法,对大别—苏鲁及邻区进行剪切波偏振分析,计算了研究区台站下方介质的各向异性分裂参数:快波偏振方向(Φ)和快慢波延迟时间(δt).本文研究结果发现,研究区内快、慢波延迟时间0.5~1.63 s,推测各向异性层深度为57.5~187.6 km,由软流圈和岩石圈地幔的各向异性共同作用引起.快波偏振方向在4个不同构造区表现出不同的特点:华北板块快波偏振方向为近E-W向,根据地质资料,我们分析认为华北板块的各向异性受地幔软流圈流动的影响明显;大别造山带各向异性平行于大别主构造,反映造山过程中岩石圈物质沿大别造山轴部NW-SE向迁移的特点; 在大别南侧和东侧的扬子板块快波偏振方向分别表现为近垂直于造山带走向和NEE-SWW,苏鲁造山带各向异性结果为NEE-SWW,与地表构造有一定的夹角,同时与板块运动方向相差较大,分析认为扬子板块和苏鲁造山带各向异性是由地幔软流圈流动和印支—燕山期构造运动残留在岩石圈地幔的"化石各向异性"共同作用的结果.     

大别—苏鲁及邻区上地幔的各向异性

大别—苏鲁是扬子与华北的碰撞造山带,对该地区上地幔各向异性的研究有助于了解该区的地幔动力学机制.本文选用了中国数字化地震台网和区域数字地震台网(山东、安徽、江苏、河南、湖北)三分量宽频带的远震地震波形数据,分别采用最小能量法和旋转相关法,对大别—苏鲁及邻区进行剪切波偏振分析,计算了研究区台站下方介质的各向异性分裂参数:快波偏振方向(Φ)和快慢波延迟时间(δt).本文研究结果发现,研究区内快、慢波延迟时间0.5~1.63 s,推测各向异性层深度为57.5~187.6 km,由软流圈和岩石圈地幔的各向异性共同作用引起.快波偏振方向在4个不同构造区表现出不同的特点:华北板块快波偏振方向为近E-W向,根据地质资料,我们分析认为华北板块的各向异性受地幔软流圈流动的影响明显;大别造山带各向异性平行于大别主构造,反映造山过程中岩石圈物质沿大别造山轴部NW-SE向迁移的特点; 在大别南侧和东侧的扬子板块快波偏振方向分别表现为近垂直于造山带走向和NEE-SWW,苏鲁造山带各向异性结果为NEE-SWW,与地表构造有一定的夹角,同时与板块运动方向相差较大,分析认为扬子板块和苏鲁造山带各向异性是由地幔软流圈流动和印支—燕山期构造运动残留在岩石圈地幔的"化石各向异性"共同作用的结果.     

Diversion of heat by Archean cratons: a model for southern Africa

The surface heat flow in the interior of Archean cratons is typically about 40 mW m⁻² while that in Proterozoic and younger terrains surrounding them is generally considerably higher. The eighty-four heat flow observations from southern Africa provide an excellent example of this contrast in surface heat flow, showing a difference of some 25 mW m⁻² between the Archean craton and younger peripheral units. We investigate two possible contributions to this contrast: (1) a shallow mechanism, essentially geochemical, comprising a difference in crustal heat production between the two terrains, and (2) a deeper mechanism, essentially geodynamical, arising from the existence of a lithospheric root beneath the Archean craton which diverts heat away from the craton into the thinner surrounding lithosphere. A finite element numerical model which explores the interplay between these two mechanisms suggests that a range of combinations of differences in crustal heat production and lithospheric thickness can lead to the contrast in surface heat flow observed in southern Africa. Additional constraints derived from seismological observations of cratonic roots, the correlation of surface heat flow and surface heat production, petrological estimates of the mean heat production in continental crust and constraints on upper mantle temperatures help narrow the range of acceptable models. Successful models suggest that a cratonic root beneath southern Africa extends to depths of 200–400 km. A root in this thickness range can divert enough heat to account for 50–100% of the observed contrast in surface heat flow, the remainder being due to a difference in crustal heat production between the craton and the surrounding mobile belts in the range of zero to 0.35 μW m⁻³.     

秦岭─大别造山带及其南北缘地震层析成像

利用秦岭─大别造山带及其毗邻地区３１０个地震台站记录到的区域地震２３６００条Ｐ波到时数据，重建了该区地壳和上地幔三维速度图像。结果表明：１．秦岭─大别造山带及其毗邻地区地壳和上地幔存在显著的横向不均匀性，直至１１０ｋｍ深度处依然明显。２．地壳上部的速度图像与地表地质构造密切相关：造山带隆起区显著高速；盆地及坳陷区明显低速。由速度鲜明对比勾勒出的秦岭─大别造山带南界基本上位于扬子北缘主边断裂带上。３．中地壳的速度图像表明，造山带内部的一些低速区对应于一些大型推覆构造。４．４０＋０ｋｍ深度处的速度图像反映了该区莫霍界面深度的起伏。大致以１０７°Ｅ为界，以东地区地壳厚度小于４０ｋｍ，以西地区大于４０ｋｍ，且呈现出往西地壳逐渐加厚的趋势。５．位于滦川、商县、丹凤的北秦岭构造带，上地幔顶部出现低速异常，异常速度值约为７．３９—７．５５ｋｍ／ｓ。结合地球物理测深的结果，可能是由下地壳、上地幔顶部的热过程所致。     

秦岭─大别造山带及其南北缘地震层析成像

利用秦岭─大别造山带及其毗邻地区３１０个地震台站记录到的区域地震２３６００条Ｐ波到时数据，重建了该区地壳和上地幔三维速度图像。结果表明：１．秦岭─大别造山带及其毗邻地区地壳和上地幔存在显著的横向不均匀性，直至１１０ｋｍ深度处依然明显。２．地壳上部的速度图像与地表地质构造密切相关：造山带隆起区显著高速；盆地及坳陷区明显低速。由速度鲜明对比勾勒出的秦岭─大别造山带南界基本上位于扬子北缘主边断裂带上。３．中地壳的速度图像表明，造山带内部的一些低速区对应于一些大型推覆构造。４．４０＋０ｋｍ深度处的速度图像反映了该区莫霍界面深度的起伏。大致以１０７°Ｅ为界，以东地区地壳厚度小于４０ｋｍ，以西地区大于４０ｋｍ，且呈现出往西地壳逐渐加厚的趋势。５．位于滦川、商县、丹凤的北秦岭构造带，上地幔顶部出现低速异常，异常速度值约为７．３９-７．５５ｋｍ／ｓ。结合地球物理测深的结果，可能是由下地壳、上地幔顶部的热过程所致。     

秦岭─大别造山带及其南北缘地震层析成像

利用秦岭─大别造山带及其毗邻地区３１０个地震台站记录到的区域地震２３６００条Ｐ波到时数据,重建了该区地壳和上地幔三维速度图像。结果表明：１．秦岭─大别造山带及其毗邻地区地壳和上地幔存在显著的横向不均匀性,直至１１０ｋｍ深度处依然明显。２．地壳上部的速度图像与地表地质构造密切相关：造山带隆起区显著高速;盆地及坳陷区明显低速。由速度鲜明对比勾勒出的秦岭─大别造山带南界基本上位于扬子北缘主边断裂带上。３．中地壳的速度图像表明,造山带内部的一些低速区对应于一些大型推覆构造。４．４０＋０ｋｍ深度处的速度图像反映了该区莫霍界面深度的起伏。大致以１０７°Ｅ为界,以东地区地壳厚度小于４０ｋｍ,以西地区大于４０ｋｍ,且呈现出往西地壳逐渐加厚的趋势。５．位于滦川、商县、丹凤的北秦岭构造带,上地幔顶部出现低速异常,异常速度值约为７．３９—７．５５ｋｍ／ｓ。结合地球物理测深的结果,可能是由下地壳、上地幔顶部的热过程所致。     

大洋岩石层拖曳窄条陆壳俯冲的极限尺度分析——以新西兰南岛和大别山超高压变质带为例

超高压变质研究涉及的一个基本力学问题是为什么低密度的大陆地壳岩石能克服浮力俯冲到高密度地幔100多公里的深度.本文的三维有限单元法计算表明:俯冲海洋板块可以拖曳侧面相邻宽度不超过150km的一窄条大陆板块,俯冲到超高压变质深度,形成少见的大规模超高压变质带.十几公里乃至几十公里尺度的陆壳块体,可能被俯冲地幔裹挟至超高压变质深度,在造山带内形成零星出露的超高压变质岩.成熟的陆-陆碰撞带则不可能使陆壳俯冲到超高压变质深度.     

大洋岩石层拖曳窄条陆壳俯冲的极限尺度分析--以新西兰南岛和大别山超高压变质带为例

超高压变质研究涉及的一个基本力学问题是为什么低密度的大陆地壳岩石能克服浮力俯冲到高密度地幔100多公里的深度.本文的三维有限单元法计算表明:俯冲海洋板块可以拖曳侧面相邻宽度不超过150km的一窄条大陆板块,俯冲到超高压变质深度,形成少见的大规模超高压变质带.十几公里乃至几十公里尺度的陆壳块体,可能被俯冲地幔裹挟至超高压变质深度,在造山带内形成零星出露的超高压变质岩.成熟的陆-陆碰撞带则不可能使陆壳俯冲到超高压变质深度.     

Stress field and seismicity in the Indian shield: Effects of the collision between India and Eurasia

Intraplate stresses and intraplate seismicity in the Indian subcontinent are strongly affected by the continued convergence between India and Eurasia. The mean orientation of the maximum horizontal compression in the Indian subcontinent is subparallel to the direction of the ridge push at the plate boundary as well as to the direction of compression expected to arise from the net resistive forces at the Himalayan collision zone, indicating that the intraplate stresses in the subcontinent, including the shield area, are caused by plate tectonic processes. Spatial distribution of historic and instrumentally recorded earthquakes indicate that the seismic activity is mostly confined to linear belts while the remaining large area of the shield is stable. The available conventional heat flow data and other indicators of heat flow suggest hotter geotherms in the linear belts, leading to amplification of stresses in the upper brittle crust. Many of the faults in these linear belts, which happen to be 200–80 m.y. old, are being reactivated either in a strike-slip or thrust-faulting mode. The reactivation mechanisms have been analyzed by taking into consideration the amplification of stresses, pore pressures, geological history of the faults and their orientation with respect to the contemporaneous stress field. The seismicity of the Indian shield is explained in terms of these reactivation mechanisms.     

Age-dependent Large-scale Fabric of the Mantle Lithosphere as Derived from Surface-wave Velocity Anisotropy

—Systematic variations of the seismic radial anisotropy ξ to depths of 200–250 km in North America and Eurasia and their surroundings are related to the age of continental provinces, and typical depth dependences of ξ _R are determined. The relative radial anisotropy ξ _R in the mantle lithosphere of Phanerozoic orogenic belts is characterized by ν _SH > ν _SV , with its maximum depth of about 70 km, on the average, while beneath old shields and platforms, it exhibits a maximum deviation from ACY400 model (Montagner and Anderson, 1989) at depths of about 100 km with ν _SV ≥ν _SH signature. An interpretation of the observed seismic anisotropy by the preferred orientation of olivine crystals results in a model of the mantle lithosphere characterized by anisotropic structures plunging steeply beneath old shields and platforms, compared to less inclined anisotropies beneath Phanerozoic regions. This observation supports the idea derived from petrological and geochemical observations that a mode of continental lithosphere generation may have changed throughout earth's history.     

天山造山带地区瑞利面波相速度与方位各向异性

天山造山带作为世界上陆内最大的造山带之一,现今地震活动频繁,造山运动强烈,是开展陆内造山和内陆地震活动研究的天然试验场.本文利用整个天山造山带地区国内及国际台网的108个地震台站连续三年的背景噪声资料,提取了8~50 s周期的瑞利面波相速度频散曲线,并构建了整个天山造山带地区的二维瑞利面波相速度与方位各向异性分布图像.结果表明：浅部结构与地表的地质构造单元具有较大的相关性.低波速异常主要分布于沉积层厚度较大的盆地地区,而高波速异常主要分布于构造活动比较活跃的山脉地区.东天山地区中下地壳存在比较弱的低波速异常,而塔里木盆地和准噶尔盆地汇聚边缘的上地幔区域则表现为明显的高波速异常,各向异性快波方向呈现近NS向的特征,暗示着塔里木盆地和准噶尔盆地的岩石圈已经俯冲至东天山的下方.中天山地区的中下地壳至上地幔区域均呈现为明显的低波速异常,且各向异性快波方向变化比较复杂,表明中天山地区的整个岩石圈结构已经弱化,热物质上涌可能对介质的方位各向异性有一定的影响.西天山及帕米尔高原的上地幔区域存在低波速异常,各向异性表现为NW-SE方向,可能与欧亚板块的大陆岩石圈南向俯冲有关.塔里木盆地内部存在相对弱的低波速异常,推测塔里木盆地可能已经受到上涌的地幔热物质的侵蚀和破坏.