Experimental investigation of the origin of majoritic garnet inclusions in diamonds

 Multianvil experiments were carried out at 10–15 GPa and 1600–1700 °C to match the compositions of majoritic garnet inclusions from diamonds, and to determine the compositions of other phases potentially coexisting with these inclusions in the source. Most experiments produced coexisting majoritic garnet, diopsidic clinopyroxene, one or more (Mg,Fe)₂SiO₄ polymorphs, and quenched carbonatic melt. The experimental garnets had relatively high Ca and Fe contents similar to the observed Ca and Fe contents of the inclusions. The resulting Si contents confirmed that the depth of origin of the inclusion with the highest Si content did not exceed 410 km, thus none of the majoritic garnet inclusions found so far originated in the transition zone (410–660 km). The evidence from inclusions and experiments is consistent with the presence of an eclogite layer occurring globally between 200 and 410 km. Compositional variations observed among more than 100 majoritic garnet inclusions with their Si content, which is a measure of pressure and depth, are consistent with the origin of the eclogite layer by crystal fractionation in a magma ocean. The compositions of olivine coexisting with majoritic garnet in the experimental products had the average Fe/(Fe + Mg) ratios between 0.16 and 0.28. Inclusions with such high Fe contents have not been found; the Fe/(Fe + Mg) ratio of the olivine inclusions in diamonds usually varies between 0.05 and 0.09. Hence, the mantle between 200 and 410 km may not contain olivine. In the absence of olivine, the discontinuity at 410 km is most likely a chemical boundary between the 200-km-thick eclogite layer and a more mafic transition zone. Received: 15 March 2001 / Accepted: 14 September 2001     

TPD软件绘制水盐体系三元相图

介绍了三种三角相图绘图软件 ,着重说明用Delphi5开发设计绘图软件 (TPD)解决了几个难点 ,达到具有多功能特点的水盐体系专用计算机绘图软件。实现了快速绘制三元平衡相图。并应用本程序绘制了不同类型相图。表明该程序方便、快速和可靠 ,所绘图形满意     

西部含锂、钾、镁、硼盐卤资源水盐体系相化学研究

从资源特点出发 ,分别回顾了含锂、钾、镁氯化物多元水盐体系 ,镁水泥体系 ,盐卤锂、钾卤化物水盐体系的相化学研究 ,概括了主要研究成果并指出实际应用上的关键问题 ,以及研究的主要内容。     

相空间中划分大尺度异常雨型的进一步研究

使用1962~2001年的逐日台站降水资料,考察中国夏季大尺度低频降水的时空特征。对于20d以上的低频尺度降水异常,在前8个主要EOF模态支撑的相空间中,采用聚类分析方法划分了6种大尺度异常雨型:东北型、黄河型、秦岭淮河型、长江江南型、华南型和少雨型。分析表明,这些雨型的物理意义明确,具有较好的持续性,优于使用2维概率密度函数的划分结果,从而说明相空间中的聚类分型是整体性和区域性兼顾的划分方式,同时也证实了多维相空间的不均匀性。统计结果显示,新雨型在季节内交替出现,能够反映出大尺度异常降水的低频演变特征,并且具有不同于季风雨带变化的特点。通过分析新雨型在历史上的分布情况,并与以往分型相比较,进一步反映出新雨型划分的客观性和合理性。     

非均匀电磁波在导电媒质界面反射的横向偏移

由电磁场边值关系给出了非均匀电磁波在导电媒质界面反射时反射系数所产生的附加相角. 利用这一附加相角导出了非均匀电磁波在导电介质界面的横向偏移,并进行了横向偏移的相关计算,绘出了横向偏移随入射角的变化曲线. 结果表明：在导电媒质界面反射电磁波的横向偏移随入射角的增大而增大,当入射角接近90°时,电磁波在界面要传播较长时间后才返回第一种媒质. 在同一入射角电场偏振化方向在入射面的电磁波要比电场偏振化方向垂直于入射面的电磁波的横向偏移大,随着电磁波频率的增加横向偏移变小.     

山西大同遥测台网低倍率系统的建设及作用

为拓宽台网的动态范围,根据山西大同遥测台网低倍率系统的建设及使用情况,简述了大同遥测台网提高定位精度、建立低倍率系统的方法及取得的实际效益,认为低倍系统可以解决大震记录限幅带来的震相识别困难问题,可提高定位精度。     

利用EMD和子波振幅谱与相位谱关系的时变子波提取方法

本文首先分析了地震波在黏弹介质的传播规律,基于黏弹介质地震波动方程总结了时变子波振幅谱和相位谱的关系,从而得出结论,准确估计子波相位谱初值和不同时刻的子波振幅谱是实现时变子波准确提取的必要条件.在此基础上,针对传统方法限制子波振幅谱形态且受限于分段平稳假设的问题,提出了一种利用EMD(Empirical Mode Decomposition)和子波振幅谱与相位谱关系的时变子波提取方法,根据子波对数振幅谱光滑连续而反射系数对数振幅谱振荡剧烈的特点,采用EMD方法将不同时刻地震记录的对数振幅谱分解为一组具有不同振荡尺度的模态分量,通过滤除振荡剧烈分量、重构光滑连续分量提取时变子波振幅谱;再应用子波振幅谱和相位谱的关系提取时变子波相位谱,将分别提取的振幅谱和相位谱逐点进行合成,最终实现时变子波的准确提取.本文方法不需要求取Q值,适用于变Q值的情况,具有良好的抗噪性能.数值仿真和叠后实际资料处理结果表明,相比传统的分段提取方法,利用本文方法提取的时变子波准确度更高,研究成果对提高地震资料分辨率具有重要意义.     

多极子阵列声波测井数据的纵横波慢度联合反演方法

多极子阵列声波测井仪器采集的单极和偶极数据受到地层、井孔、仪器测量系统的影响.在处理实际声波测井数据时,必须考虑多极子模式波的频散效应,以及测井仪器在其中的影响.根据仪器等效理论和相位匹配方法,本文提出了一种从多极子阵列声波测井数据中同时获得纵、横波慢度的联合反演方法.这种方法的关键在于利用相同仪器-地层模型计算多极子模式波频散曲线,以此来匹配频域内纵波与横波数据的相位.相对于将泄漏纵波和弯曲波频散效应分开处理的其他方法,该方法不仅可以减少纵横波速度反演的不确定性,而且还避免了从声波数据中提取频散数据的繁琐过程.通过理论分析和现场数据处理证明了本文联合反演方法的准确性和有效性.     

Metamorphism,fluid behavior and magmatism in oceanic subduction zones

Based on the updated results of experimental petrology and phase equilibria modelling and combined with the available thermal structure models of subduction zones, this paper presents an overview on the dehydration and melting of basic,sedimentary and ultrabasic rocks that occur in the different stages during oceanic subduction processes and their influences on magmatism above subduction zones. During the subduction at the forearc depth of <90–100 km, the basic and ultrabasic rocks from most oceanic slabs can release very small amounts of water, and significant dehydration may occur in the slab superficial sediments. Strong dehydration occurs in both basic and ultrabasic rocks during subduction at the subarc depth of 90–200 km. For example, more than 90% water in basic rocks is released by the successive dehydration of chlorite, glaucophane, talc and lawsonite in the subarc depths. This is diversely in contrast to the previous results from synthetic experiments. Ultrabasic rocks may undergo strong dehydration through antigorite, chlorite and phase 10 ? at the subarc depth of 120–220 km. However,sediments can contribute minor fluids at the subarc depth, one main hydrous mineral in which is phengite(muscovite). It can stabilize to ~300 km depth and transform into K-hollandite. After phengite breaks down, there will be no significant fluid release from oceanic slab until it is subducted to the mantle transition zone. In a few hot subduction zones, partial melting(especially flux melting) can occur in both sediments and basic rocks, generating hydrous granitic melts or supercritical fluids, and in carbonates-bearing sediments potassic carbonatite melts can be generated. In a few cold subduction zones, phase A occurs in ultrabasic rocks, which can bring water deep into the transition zone. The subducted rocks, especially the sediments, contain large quantities of incompatible minor and trace elements carried through fluids to greatly influence the geochemical compositions of the magma in subduction zones. As the geothermal gradients of subduction zones cannot cross the solidi of carbonated eclogite and peridotite during the subarc subduction stage, the carbonate minerals in them can be carried into the deep mantle.Carbonated eclogite can melt to generate alkali-rich carbonatite melts at >400 km depth, while carbonated peridotite will not melt in the mantle transition zone below a subduction zone.     

相位空间内的解缠绕相位反演

全波形反演方法是一种数据域高精度反演方法,该方法通过匹配观测数据与模拟数据的地震波形,利用梯度法准确反演地下介质参数的分布情况.由于观测数据普遍缺少低频信息,该方法易受周期跳跃现象影响.特别是当地下存在大尺度强反射界面的构造时,地下介质的反演转化为强非线性问题求解.该情形下,即使观测数据包含充足的低频信息,全波形反演也难以给出准确的反演结果.一般可以通过减弱反演对初始模型参数的依赖性来克服上述问题,具体表现为使用新变量(例如瞬时相位、包络等)代替目标函数中的采样后波场,以增强新目标函数的凸性.但是,对该新目标函数进行反演时,伴随状态方程中存在关于新变量和波场的一个链式微分项,该项保留了反演问题的非线性,导致新的反演方法难以处理包含大尺度构造的强非线性反演问题.此外,基于新变量的反演问题依然在波场空间中计算模型梯度,难以充分利用新变量与模型参数之间的弱非线性关系.因此,本文提出用频率域波动方程的相位形式代替传统的波动方程来消除伴随状态方程中的链式微分项,用解缠绕的相位代替目标函数中采样前波场并在相位空间进行反演.该方法可以最大程度地利用地下介质参数和解缠绕相位之间的弱非线性关系,从而削弱反演的非线性性.由于基于频率域波场计算得到相位有严重的缠绕问题,本文采用基于振幅排序的多聚类算法来对相位进行解缠绕.虽然将介质参数到波场的映射替换为介质参数与解缠绕相位的映射,会导致反演结果的分辨率有所下降,但该方法可以在相位空间恢复介质参数的大尺度低波数分量.Marmousi模型测试证明了该方法的有效性和准确性,针对部分BP模型的测试也证明了该方法处理强非线性问题的能力.