多硅白云母中Fe2+的高压有序效应

21个多硅白云母来自4个低温高压变质带。用电子探针、X射线粉末衍射及穆斯堡尔谱测定其化学成分、b0值及Fe²⁺占位。建立Fe²⁺(M1)/Fe²⁺(M2)对b0值相关图,发现Fe²⁺在八面体晶位有序化并解释其有序机理。     

大别山高压-超高压片麻岩锆石的拉曼光谱学研究

对大别山高压-超高压片麻岩的锆石进行了激光拉曼探针、阴极发光(CL)、U-Pb年龄和U、Th等微量元素的测定分析.研究结果表明:锆石拉曼光谱1008cm-1峰的半高宽普遍小于20cm-1,指示锆石结晶程度较好到中等程度的蜕晶化;早期继承锆石在三叠纪高压-超高压变质作用中经历了退火和重结晶作用,所受的放射性通量是从200Ma的早侏罗纪开始积累的,表明高压-超高压岩石在这一时间已出露地表;北大别白垩纪岩浆热事件对高压-超高压岩石的影响很小;大多数锆石数据都落在天然锆石的放射性破坏趋势(RDT)中,表明锆石在高压、超高压过程中基本发生了完全的重结晶.     

大别山榴辉岩退变质多硅白云母及地

大别山榴辉岩中的多硅白云母可以分成三个世代形成于榴辉岩相进变质阶段的原生Phe1、榴辉岩相退变质晚阶段的Phe2和角闪岩相至绿片岩相退变质阶段的Phe3.电子探针测得,超高压下形成的Phe1,其Si和Fe2++Mg值出乎意料地低于低压下形成的Phe3,这与多硅白云母地压计的基本原理,即多硅白云母的Si和Fe2++Mg含量与其形成压力成正比这一原理产生了矛盾.产生这种矛盾的可能原因是,多硅白云母的成分除了取决于压力因素以外,还取决于主岩的铝-硅比值、Fe2++Mg含量、氧逸度的变化、流体的存在等因素.因此,利用多硅白云母的硅含量来探讨退变质过程压力时必须加倍小心.     

多硅白云母地质压力计的研究进展

白云母是变质岩中分布最广泛的矿物之一,在大多数矿物组合中白云母的Si含量随着变质作用压力的增加而增加,可作为地质压力计。对KMASH体系3个有限组合中多硅白云母的Si含量与温压条件关系的实验研究结果表明,多硅白云母Si含量地质压力计明显与矿物组合有关。因此,不能把这些实验结果简单地外延到矿物组合不同的天然岩石中。在KMASH体系的温压视剖面图上模拟白云母的Si含量等值线与质量较好的实验结果非常接近,由此可以把这种方法推广到KFMASH或更复杂的体系中。在利用多硅白云母Si的含量确定天然矿物组合的变质作用压力时,最好利用视剖面图的方法。     

略阳地区泥盆纪地层中3T型多硅白云母的成因机理及找矿意义

3T型多硅白云母是白云母的一个变种。它不但是变质相带中的标型矿物,也是特球构造和板块消亡带的特征矿物。略阳地区泥盆系中3T型多硅白云母的发现在我省属于首次。该矿物发现于略阳县的西部,产于泥盆纪地层中金矿体内。金矿赋存于蚀变细碧岩中,共生矿物有石英、白云石、绿泥石、铁方解石、黄铁矿等。矿体含金品位增高时,3T型多硅白云母含量同步增长,而且地层扭动也随之强烈。本文对3T型多硅白云母产生的地质环境、矿物学特征,形成机理以及与构造运动、板块活动的关系等方面进行了初步探讨。     

大别山榴辉岩退变质多硅白云母及地压计可用性讨论

大别山榴辉岩中的多硅白云母可以分成三个世代；形成于榴辉岩相进变质阶段的原生Phel、榴辉岩相退变制裁晚阶段的Phe2和角闪岩相至绿片岩相退变质阶段的Phe3。电子探针测得，超高压下形成的Phel，其Si和Fe^2 Mg值出乎意料地低于低压下形成的Phe3，这与多硅白云母地压计的基本原理，即多硅白云i和Fe^2 Mg含量与其形成压力成正比这一原理产生了矛盾，产生这种矛盾的可能原因是，多硅白云母的成分除了取决于压力因素以外，还取决于主岩的铝-硅比值、Fe^2 Mg含量、氧逸度的变化、流体的存在等因素，因此，利用多硅白云母的硅含量来探讨退变质过程压力时必须加倍小心。     

新疆阿克苏前寒武纪蓝片岩中多硅白云母的研究

新疆阿克苏蓝片岩是目前世界范围内保存最好的前寒武纪蓝片岩之一.一般认为蓝闪石片岩是在低温高压条件下形成的,且与板块俯冲有密切联系.本文对阿克苏蓝片岩地体的泥质片岩和砂质片岩中的白云母进行了电子探针分析,通过对得到的Si含量数据进行统计,探讨了蓝片岩地体不同区域所受压力的变化,进而用矿物组合、矿物形变、多硅白云母压力计等分析方法讨论了变质温压区间和温压关系.研究结果表明阿克苏蓝片岩带南侧岩石承受的变质压力明显大于北侧,这可能指示了古洋壳板块从北向南的俯冲方向.     

多硅白云母b0值对澜沧群中压和高压变质的反映

多硅白云母b₀值作为相对地质压力计的理论和方法,已受到各国地质学家的普遍重视。本文以澜沧群多硅白云母作为研究对象,提出运用多硅白云母b₀值区分不同压力变质的方法。研究结果表明澜沧群经历了中压和高压变质作用,两期变质的多硅白云母b₀值分别为9.027Å和9.047Å。     

滇西南澜沧群多硅白云母的多型和化学成分特征及其意义

从理论、实验及实际观察的结果都表明,随着压力的增加白云母中绿鳞石的含量显著地增加,可以认为在多期变质作用过程中,尤其是在变质压力不同的多期变质作用下,形成的多硅白云母,其化学成分就会打上不同的烙印。７７个多硅白云母化学成分的统计结果表明,澜沧群低级变质岩中的多硅白云母有两种成因。在Ｎａ－Ｍｇ相关图上,反映了高压和中压变质特征,高压变质的多硅白云母约占７０％。这与用多硅白云母ｂ０值鉴别的高压和中压变质是相吻合的。多硅白云母的多型为３Ｔ和２Ｍ１型,以２Ｍ１型为主     

高温高压下石膏脱水相变的原位拉曼光谱研究

本文运用激光拉曼光谱仪,利用水热金刚石压腔装置对高温高压条件下石膏-水体系中的石膏脱水相变进行拉曼光谱研究.在压力0.1 MPa～837.9 MPa和温度16～200 ℃条件下通过系列实验对相变的过程进行了原位光谱分析.与人们已知的无水条件下石膏分两步脱水的过程不同,高压下石膏在饱和水环境下倾向于一次性的脱去所有结晶水而形成无水石膏,实验中没有观察到半水石膏的出现.通过实验数据得到石膏和无水石膏的转折温度和平衡压力间的关系式为P(MPa)=19.56·T(℃)-2926.5.     

High-pressure Raman spectroscopic study of chondrodite

Variation of Raman spectra of both natural (F-bearing) and synthetic (F-free) chondrodite samples were studied up to 400 kbar at room temperature. Ambient Raman frequencies for the synthetic sample are in general lower than those for the natural one. This is correlated with a slight expansion of the volume of the synthetic sample due to substitution of OH for F. The frequencies of all Raman bands for both samples increase monotonically with increasing pressure. The positive pressure dependences in the O−H stretch frequencies for both F-free and F-bearing samples are contrary to those for other dense hydrous magnesium silicates. A mechanism involving both the hydrogen-hydrogen repulsion and hydrogen bondings is proposed to explain the abnormal behavior. The effects of substitution of F for OH on both the ambient and high-pressure Raman spectra of chondrodite are also discussed. Received: 19 February 1998 / Revised accepted: 26 June 1998     

Raman spectroscopic study of K-lingunite at various pressures and temperatures

K-lingunite is a high-pressure modification of K-feldspar that possesses the tetragonal hollandite structure. Variations of the Raman spectra of K-lingunite were studied up to ~31.5 GPa at room temperature, and in the range 79–823 K at atmospheric pressure. The Raman frequencies of all bands were observed to increase with increasing pressure, and decrease with increasing temperature for K-lingunite. This behavior is in line with those observed for most of other materials. New sharp Raman bands appear at pressures greater than 13–15 GPa, suggesting a phase transition in K-lingunite with increasing pressure. The transition is reversible when pressure was released. The appearance of these new Raman bands may correspond to the phase transition revealed earlier at around 20 GPa by X-ray diffraction studies. Instead of transforming back to its stable minerals, such as orthoclase, microcline or sanidine, K-lingunite became amorphous in the temperature range 803–823 K at atmospheric pressure.     

High-pressure behaviour of serpentine minerals: a Raman spectroscopic study

Four main serpentine varieties can be distinguished on the basis of their microstructures, i.e. lizardite, antigorite, chrysotile and polygonal serpentine. Among these, antigorite is the variety stable under high pressure. In order to understand the structural response of these varieties to pressure, we studied well-characterized serpentine samples by in situ Raman spectroscopy up to 10 GPa, in a diamond-anvil cell. All serpentine varieties can be metastably compressed up to 10 GPa at room temperature without the occurrence of phase transition or amorphization. All spectroscopic pressure-induced changes are fully reversible upon decompression. The vibrational frequencies of antigorite have a slightly larger pressure dependence than those of the other varieties. The O–H-stretching modes of the four varieties have a positive pressure dependence, which indicates that there is no enhancement of hydrogen bonding in serpentine minerals at high pressure. Serpentine minerals display two types of hydroxyl groups in the structure: inner OH groups lie at the centre of each six-fold ring while outer OH groups are considered to link the octahedral sheet of a given 1:1 layer to the tetrahedral sheet of the adjacent 1:1 layer. On the basis of the contrasting behaviour of the Raman bands as a function of pressure, we propose a new assignment of the OH-stretching bands. The strongly pressure-dependent modes are assigned to the vibrations of the outer hydroxyl groups, the less pressure-sensitive peaks to the inner ones.     

High-pressure Raman spectroscopic study of Co- and Ni-olivines

 The Raman spectra of synthetic α-Co₂SiO₄ and α-Ni₂SiO₄ olivines have been studied at room temperature and various pressures. All the Raman frequencies of the two olivines increase with increasing pressure, and most of the frequency–pressure plots obtained under both quasi- and nonhydrostatic conditions are nonlinear. It has been found that the average pressure derivative of Raman frequencies of the lattice modes in both Co- and Ni-olivines is smaller than that of the internal modes of SiO₄, indicating that the distortion of SiO₄ tetrahedra under static compression may be more severe than that of MO₆ octahedra. In addition, four new Raman bands were observed in Ni-olivine under nonhydrostatic compression and above 30 GPa. This result suggests that a new phase of Ni-olivine should be formed at 30 GPa or amorphization may occur at still higher pressure. Received: 11 July 2000 / Accepted: 19 December 2000     

Raman spectroscopic study of hydroxyl-clinohumite at various pressures and temperatures

 Variations of Raman spectra of hydroxyl-clinohumite were studied up to ∼370 kbar at room temperature, and in the range 81–873 K at atmospheric pressure. With the exception of the symmetric OH-stretch bands, the Raman frequencies of all bands were observed to increase monotonically with increasing pressure, and decrease with increasing temperature. This behavior is in line with those observed for other humite members (norbergite and chondrodite) so far studied. The symmetric OH-stretching band shows a mode softening with increasing pressure, and splits into two bands at either high pressure or low temperature. In the quasihydrostatic experiment, the compression and decompression paths of one of the asymmetric OH-stretch bands form a hysteresis loop, but the same behavior was not observed in the nonhydrostatic experiment. These results indicate that the two kinds of OH groups in hydroxyl-clinohumite have nonequivalent movement paths on compression, and with one OH group experiencing a release of spatial hindrance during compression. This behavior appears to be modified by shear stress. The same complication of the OH groups was not observed in the temperature variation study. The pressure and temperature variations of the Raman frequencies for the various vibrations involving the SiO₄ tetrahedra and MgO₆ octahedra below ∼1000 cm⁻¹ for clinohumite behave similarly to other hydrous magnesium silicates. On the basis of the relationship between isothermal bulk modulus and Raman data, it is suggested that the linear pressure dependences of vibrational frequencies of various Raman bands reported in the literature are inadequate. Received: 20 March 1999 / Revised, accepted: 24 August 1999     

低温原位拉曼光谱技术在流体包裹体研究中的应用

国外学者自80年代起利用原位低温拉曼测定技术在国际上首先开展地质领域感兴趣的几种盐水化合物研究以来,原位低温拉曼测定技术已经成功地用于对人工合成和自然界盐水体系流体包裹体的研究,在流体相中盐类的鉴定、低温相平衡及盐度研究等方面取得了显著成果。该方法是对传统的流体包裹体显微测温方法的重要补充,正在成为国际上流体包裹体研究的一个新的热点,在地质流体研究方面具有非常广阔的应用前景。     

石英高压相变研究进展

文中总结了前人有关石英高温高压相变的实验结果。根据以前的实验,在静水压条件下,石英-柯石英-斯石英-CaCl2结构超斯石英相-α-PbO2结构超斯石英相之间的相变方程分别是:p(GPa)=(2.11±0.03)+(9.8×10-4±1.2×10-4)×T(℃),p(GPa)=(8.0±0.2)+(1.1×10-3±3×10-4)×T(℃),p(GPa)=(51±2)+(0.012±0.005)×T(K),p(GPa)=98+(0.0095±0.0016)×T(K)。文中还初步探讨了非静水压状态对石英相变的影响。实验结果表明,差应力的出现降低了石英相变所需要的围压,即相变边界向低压方向偏移,在周永胜等人实验数据的基础上,笔者尝试将二维的相图扩展到三维相图以考虑差应力的影响。最后讨论了石英相变在地学研究中的作用,对比不同的观点分析了前人对超高压变质作用过程的解释,希望可以为以后解释地质资料提供较为广泛的可能性,促进我们对地球内部动力学过程的了解。     

A Raman spectroscopic study of shock-wave densification of vitreous silica

The densification processes in SiO₂ glass induced by shock-wave compression up to 43.4 GPa are investigated by Raman spectroscopy. At first, densification increases with increasing shock pressure. A maximum densification of 11% is obtained for a shock pressure of 26.3 GPa. This densification is attributed to the reduction of the average Si−O−Si angle, which occurs first by the collapse of the largest ring cavities, then by further reduction of the average ring size. For higher shock pressures, a different structural modification is observed, resulting in decreasing densification with increasing shock pressure. Indeed, the recovered densification becomes very small, with values of 1.8 and 0.5% at 32 and 43.4 GPa, respectively. This is attributed to partial annealing of the samples due to high after shock residual temperatures. The study of the annealing process of the most densified glass by in situ high temperature Raman spectroscopy confirms that relaxation of the Si−O−Si angle starts at a lower temperature (about 800 K) than that of the siloxane rings (about 1000 K), thus explaining the high intensity of the siloxane defect bands in the samples schocked at compressions of 32 and 43.4 GPa. The large intensity of the siloxane bands in the nearly undensified samples shocked by compressions above 30 GPa may be explained by the relaxation during decompression of five- and six-fold coordinated silicon species formed at high pressure and high temperature during the shock event. Received: March 30, 1998 / Revised, accepted: August 21, 1998