岩浆－热液过渡阶段体系中不相容元素地球化学行为及其机制－以新疆阿尔泰3号伟晶岩脉研究为例

伟晶岩形成和演化中岩浆-热液过渡阶段物理化学性质、过铝质富挥发分岩浆体系岩浆液相不混溶、流体相出溶事件的相对时间尺度以及在岩浆-热液过渡阶段体系中稀土和其它微量元素地球化学行为(稀土“四重效应”机制和微量元素分异及控制因素等)是目前过铝质岩浆体系研究的焦点问题。对上述问题的研究和探讨，将有助于了解伟晶岩形成和演化的全过程，有助于了解挥发分(H_20、F、B、P)对过铝质岩浆体系物理性质以及对REE和其它微量元素地球化学行为影响，这对于理解过铝质岩浆体系成岩、成矿作用过程具有重大的理论和实际意义。本论文选择著名的新疆阿尔泰3号伟晶岩脉为研究对象，由于它具有完美的分带特征，使我们有可能通过各结构带矿物学、地球化学的研究揭示伟晶岩成因和演化过程以及讨论岩浆-热液过渡阶段体系中的稀土和微量元素地球化学行为。由于LCT型伟晶岩具有明显的分带性、矿物颗粒大小不均匀性等特点，因此利用全岩样品研究伟晶岩往往因取样没有代表性而被大多数岩石学家和地球化学家所否定。考虑到这点，本文系统采集阿尔泰3号伟晶岩脉各结构带磷灰石、电气石、碱性长石、石英矿物，部分结构带的石榴石、绿柱石、锂辉石矿物以及伟晶岩冷凝边和蚀变围岩的全岩样品，通过各结构带磷灰石矿物化学组成和~(87)Sr／~(86)Sr比值测定，电气石矿物的化学组成和硼同位素组成分析，碱性长石中磷含量的电子探针分析和碱性长石-石英矿物对的氧同位素体系研究以及蚀变围岩和冷凝边的化学组成分析，本文较为详尽系统地探讨以上所有的问题。通过本次多年的研究，我们获得了以下几点新的认识：f1) 富挥发分过铝质岩浆体系的样品存在稀土“四重效应”和Y-Ho、Zr-Hf、Nb-Ta、Sr-Eu元素对的显著分异，表明在过铝质岩浆演化过程中含氟流体相起着重要的作用；目前，稀土“四重效应”机制被认为是含水流体相与过铝质岩浆熔体相互作用的结果(Irber 1999；Bau 1997)，而不是独居石、磷钇矿、石榴石矿物等矿物的早期结晶引起的残余熔体稀土含量的异常变化。由于阿尔泰3号伟晶岩脉各带磷灰石以及与其共生的石榴石、绿柱石、碱性长石、锂辉石矿物均存存明显的稀土“四重效应”以及相同电价、相似离子半径的不相容元素间存在显著的分异，并结合最近赵振华等(1999)和Sba and Chappell(1999)报道S型花岗岩全岩和单矿物(磷灰石、独居石、长石、黄玉等)均存在稀土“四重效应”这一现象，本文研究提出，稀土“四重效应”是富挥发分过铝质岩浆体系的一个基本特征，其机制既不可能由含稀土的副矿物早期结晶引起残余熔体相中REE含量变化的结果，也不能定性地归因于流体相与熔体相相互作用过程中稀土元素在流体／熔体之间分异的结果，而很可能与伟晶岩岩浆形成之前某些过程密切相关，S型花岗岩岩浆在液相线以上存在硅酸盐熔体与高盐熔体(或卤水相)的不混溶液相分离有可能是过铝质岩浆体系产生稀土“四重效应”的主要原因。(2) 由于Sr~(2+)与Eu~(2+)具有相同的电价、相似的离子半径，根据经典的地球化学原理，它们具有相似的地球化学行为，在各种地质过程中其它们具有紧密的一致性。阿尔泰3号伟晶岩磷灰石中Sr／Eu比值具有二歧变化现象，其中I、Il、III和IV带磷灰石具有低的Sr／Eu比值(16:0～111.2)，而V、VI、VII带、核部带和IV带中的一个磷灰石则显示较大的Sr／Eu比值(主要在246．6～514:9范围，其中IV带的一个磷灰石该比值在10000以上)。对世界范围内的过铝质花岗岩统计表明，过铝质岩浆岩的全岩样品中的Sr／Eu也呈现二歧变化，由此本文提出Sr／Eu比值是指示过铝质岩浆体系中岩浆流体相出溶的有效地球化学参数，大于300的Sr／Eu比值是Eu~(2+)强烈分配进入流体相的地球化学标志。(3) 阿尔泰3号伟晶岩I、II、III带电气石矿物的硼同位素组成(δ~(11)B)分布在-41.11‰～-30.90‰之间，V、VI、VII带电气石矿物硼同位素组成(δ~(11)B)在-15.23‰～-9.20‰范围，IV带电气石硼同位素分布于-39.19～13.10‰范围，如此大的硼同位素分馏无法根据实验研究获得的熔体／流体相间的分馏系数进行合理解释。我们的研究表明岩浆成因电气石的B同位素组成与电气石化学组成具相关性，随电气石Y位上AI、Li阳离子数的增大，δ~(11)B值显示明显增大的趋势。阿尔泰3号伟晶岩最初形成的结构带中电气石的B同位素组成是目前所发现的最低值之一(-41.1l～39.01‰)，指示形成伟晶岩脉的初始岩浆可能由含非海相蒸发岩的泥质岩经变质深熔作用形成，或是伟晶岩岩浆在上侵定位过程中同化了含非海相蒸发岩地层的结果。本次研究利用电气石-白云母和电气石-四硼酸盐矿物间的同位索分馏以及熔体相-流体相间的同位索分馏，合理解释了阿尔泰3号伟晶岩脉电气石B同位素分馏过程，并首次获得伟晶岩形成、演化过程中B同位素组成演化的全程图谱。(4)伟晶岩岩浆形成和演化过程是否存在由过磷引起的液相不混溶现象未见确凿的岩石学和实验地球化学证据。阿尔泰3号伟晶岩脉糖粒状钠长石带(II带)明显由两种不同组构的岩性组成，而且该带是3号脉主要的Be矿化带，也是P、REE最重要的沉淀场所。阿尔泰3号伟晶岩脉梳状结构带和I带的碱性长石具较高P含量(平均值分别为0.42 wt％和0.22 wt％)，随着岩浆的演化进行，从III带到核部带，碱性长石中P含量逐渐增大(平均值由0.21 wt％增至0.50 wt％)，而II带碱性长石中异常低的P含量(平均值为0.08、wt％)是该带大量磷灰石矿物饱和结晶，导致残余熔体相中P极度亏损所造成的，而不是晚期出溶的岩浆热液交代形成的。根据Watson (1978)、Ryerson and Hess(1980)在液相线以上温度下实验研究获得的微量元素在不混溶的基性和酸性液相中分配特征，以及Webster et a1．(1997）对德国Ehrenfriedersdorf矿区伟晶岩石英中熔体包裹体的研究成果，我们推断在富磷岩浆体系中，在其演化的早期将出现由磷引起的液相不混溶作用，它对伟晶岩成岩和Be的成矿具有重大的影响。

氟、氯对热液钨、铜成矿的制约-以江西德兴铜矿、大吉山钨矿为例

矿化剂在热液矿床成矿过程中的重要作用一直为人们所关注，矿化剂地球化学行为直接影响成矿元素的富集成矿，不同的矿化剂元素可能对金属成矿具有一定的专属性。本文以著名的江西德兴铜厂超大型斑岩铜矿床和大吉山钨矿床作为研究对象，研究F、Cl与W、Cu成矿的关系。主要的认识如下：（1）F在花岗质岩浆中，可以降低岩浆的粘度、密度、固液相线温度、改变熔体结构，而Cl对熔体结构没有多大的影响。F在流体一花岗质熔体相间，绝大多数配分系数小于1.0，趋向于熔体相中配分，DF随体系中F浓度的升高而增加。Cl在流体一花岗质熔体相间的配分系数均大于1.0，且Dc1 随体系中Cl浓度的升高而增大·Cl强烈地趋向富集于流体相中。（2）Cu在流体一花岗质熔体作用过程中，铜总趋向于流体相中分布（DCu都大于1）。特别是在富Cl流体中Cu浓度较高，说明在富含Cl的热液流体能够从共存的熔体中活化迁移出大量的 Cu，S的加入DCu有降低的趋势。钨趋向于熔体相中富集，其配分系数大多小于1.0。（3）德兴铜厂花岗闪长斑岩属钙碱性系列岩石属I型花岗岩类，具有埃达克岩的特征。岩浆来源于深部，在结晶演化过程中发生了围岩物质的混染，这种高铜含量围岩的混染使成矿物质在岩浆中得到富集，有利于铜的活化、迁移。在铜厂岩体不同的蚀变带中，SiO2、K2O、Cu、Mo等从新鲜斑岩甚至弱蚀变带中带出，而在强蚀变带强烈富集，Cl同样有在强蚀变岩石中富集的趋势；而Na2O、Fe从斑岩体中带出，进入流体相中，流体中大量Fe的存在，有利于铜的沉淀、富集成矿。（4）德兴铜厂斑岩体微量元素和稀土元素地球化学特征表明，该岩体发生了流体一熔体作用，分异出来的流体是一种相对富氯的流体，同时成矿流体的流向是从岩体中心向接触带方向流动。（5）大吉山花岗岩具有高SiO2、A/CNK值，显示过铝质特点。黑云母花岗岩是壳源花岗岩但又受到慢源岩浆或慢源流体的影响。随着花岗岩的演化（从I→II→III）SiO2、K2O＋Na2O逐渐增加，ΣFe、Al2O3、CaO、F含量降低，为成矿提供了大量的矿化剂（F）和沉淀剂（Fe、Ca）。Eu负异常从I至III阶段花岗岩逐渐加强，表明该岩浆经历了高度的分异演化。（6）大吉山花岗岩类稀土元素具有“四重效应”配分的特点以及微量元素对玲Rb、Y/Ho、Zr/Hf以及Nb／Ta发生明显分异，暗示在花岗岩岩浆的演化过程中，经历了充分的流体一熔体作用，同时分异出大量富含F、W等矿化剂元素和成矿元素的热液流体，致使钨矿的形成。大吉山石英脉型钨矿的成矿年龄大约在155 Ma。（7）通过对成矿流体和花岗质岩石黑云母、白云母中卤素相对逸度的研究（log(H2O/fHCl）fluid、log（fHF/fHCl）fluid）发现，铜厂斑岩型铜矿床的成矿体系是相对富氯体系，而大吉山石英脉型钨矿床成矿体系相对富氟，同时氟可能主要迁移W、Sn、Nb、Ta等金属元素。（8）结合斑岩型铜矿床成矿流体特征，铜主要以C1的络合物形式存在和迁移，迁移形式主要是CuCl0、CuCl2等。石英脉型钨矿床中，钨主要以钨酸、钨酸盐及其离解形式存在和迁移，如WO42-、HWO4-、NaHWO4、Naw伍．等；在高度富氟的成矿流体中，钨的氟氧络合物（如WO3F-，WO2F42-等）对钨迁移也具有重要的作用。因此，不同矿化剂类型具有一定的成矿专属性，热液铜矿床主要与Cl、S有 关，而热液钨矿床大多与F有关。

地表水体中微量金属元素分布的水/胶体作用控制机理的实验研究

水体中轻重稀土元素之间的分异，特别是一些具有相同电价而又具有近似相同离子半径的元素对（如Y3＋/Ho3＋、Zr4+/Hf4+、Nb5+/Ta5+）之间的分异，Ce异常和REE四重效应存在及产生原因和不同因素的控制机理构成了水体稀土元素及其它微量金属元素地球化学研究的核心科学问题，是我们合理解释地表水体中REE及其它微量金属元素组成变化的重要理论基础。目前研究水I微粒界面作用的工作不少，但至今进行的胶体或其它微粒对REE和高价阳离子（如Zr、Hf、Nb和Ta）的吸附实验研究不多，已有的实验也未能对不同控制因素（如pH、溶液介质类型、无机和有机配位体等）的控制机理进行系统研究。本文通过系列批次实验，定量研究了水合氧化铁（日FO）在不同溶液介质条件下对二价（Cu2+）、三价（Ln3＋）、四价（Zr4+、Hf4+）以及五价（Nb5+、Ta5+）阳离子的吸附／去除作用，重点讨论了溶解配位体和pH影响下水l胶体作用对轻重稀土以及Y-Ho、Zr-Hf和Nb-Ta元素对之间分异行为的影响，并模拟了稀土元素在溶液中的形态分布。研究结果表明：微量金属元素在HFO上吸附的动力学特征受控于HFO生成的动力学，溶液介质条件（包括pH、电解质、溶解配位体、吸附剂及吸附质的浓度以及吸附质的形态分布等）是影响微量金属元素水l胶体作用的主要因素；稀土元素的分配系数在水胶体作用过程中受不同因素的影响而呈现不同的分布模式，但都存在丫的负异常和较低pH下Ce的正异常现象，在CO32-、腐殖酸和SO42-、PO43-的影响下，稀土元素的分配系数分别呈现轻稀土富集和重稀土富集的分布模式，REE在HFO上的作用机制是离子交换和特性吸附综合作用的结果；在天然水体p日范围内，Zr、Hf和Nb、Ta在吸附／共沉淀过程中发生了分异，但均显示相对惰性的行为并表现出较好的一致性，指示了其地球化学孪生对的行为。上述研究结果为合理解释地表水体中稀土和其它微量金属元素分布变化的多样性提供了实验依据。

花岗岩-LiF-NaF-H_2O体系液相不混溶的实验研究

Liquid segregation phenomena have been found and explained in the F(Li)-rich granites in south China by Wang Linakui et al. (1979; 1983). A number of experimental investigations into the liquid immiscibilities in the granites systems have been carried out (Anfilogov et al., 1983; Glyuk et al., 1971; Glyuk et al., 1973a; 1973b; kovalenko, 1978; Wang Liangkui et al., 1987). Nevertheless, the detailed scenarios of the liquid immiscibilities in the granitic magmas are much less understood. This experimental study is amide to get access to this problem. Starting materials are biotite granite +LiF(3-10%)+NaF(3-10%)+H_2O(30%). The experimental results have shown that the liquid immiscibilities of melts of different compositions occur at 1 kbar and 840 ℃ when 5wt% (LiF + NaF) are added to the granite samples. three kinds of glasses indicating of three types of coexisting immiscible melts have been observed: light blue matrix glass, melanocratic glass balls and leucocratic glass balls. It is interesting that we have observed various kinds of textures as follows: spherulitic texture, droplets, flow bands, swirls. All these textures can be comparable to those in the natural granitic bodies. Electron microprobe data suggest that these different kinds of glasses are of different chemical compositions respectively; matrix glasses are F-poor silicate melts; melanocratic balls correspond to F-rich silicate melts; and leucocratic balls are the melts consisting mainly of fluorides. Raman spectrometric data have indicated that different glasses have different melt structures. TFM Diagrams at 1000 * 10~5 Pa have been plotted, in which two miscible gaps are found. One of the two gaps corresponds to the immiscibility between F - poor silicate melt and F-rich silicate melt, another to that between the silicate melt and fluoride melt. The experiments at different pressures have suggested that the decreases in pressures are favorable to the liquid immiscibility. Several reversal experiments have indicated that the equilibria in different runs have been achieved. We have applied the experimental results to explain the field evidence of immiscibilities in some of granites associated with W-Sn-Nb-Ta mineralization. These field phenomena include flow structure, globular structures,mineralized globular patche and glass inclusions in topaz. We believe that the liquid immiscibility (liquid segregation) is a possible way of generation of F(Li)-rich granites. During the evolution of the granitic magmas, the contents of Li, F, H_2O and ore-forming elements in the magmas become higher and higher. The granites formed in the extensional tectonic settings commonly bear higher abundences of the above-mentioned elements. the pressures of the granitic magmas are relatively lower during the processes of their emplacements and cooling. The late-staged magmas will produce liquid immiscibilities, leading to the production of several coexisting immiscible melts with different chemical compositions. The flow of immiscible consisting magmas will produce F(Li)-rich granites. It is also considered that liquid immiscibilities are of great significance in the production of rare metal granites. The ore-forming processes and magmatic crystallization and metasomatic processes can be occur at the same time. The mineralisations of rare metals are related to both magmatic and hydrothermal processes.

Effect of Nb Content on the Microstructure and Mechanical Properties of Zr-Cu-Ni-Al-Nb Glass Forming Alloys

(Zr65Al10Ni10Cu15)(100-x) Nb-x glass forming alloys with Nb contents ranging from 0 to 15 at.% were prepared by water-cooled copper mould cast. The alloys with different Nb contents exhibited different microstructures and mechanical properties. Unlike the monolithic Zr65Al10Ni10Cu15 bulk metallic glass, only a few primary bee beta-Ti phase dendrites were found to distribute in the glassy matrix of the alloys with x = 5. For alloys with x = 10, more beta-phase dendrites forms, together with quasicrystalline particles densely distributed in the matrix of the alloys. For alloys with x = 15, the microstructure of the alloy is dominated by a high density of fully developed P-phase dendrites and the volume fraction of quasicrystalline particles significantly decreases. Room temperature compression tests showed that the alloys with x = 5 failed at 1793 MPa and exhibited an obvious plastic strain of 3.05%, while the other samples all failed in a brittle manner. The ultimate fracture strengths are 1793, 1975 and 1572 MPa for the alloys with x = 0, 10 and 15 at.% Nb, respectively.

Undercooling and Rapid Solidification of Nb-Si Eutectic Alloys Studied by Long Drop Tube

Niobium-silicide alloys have great potential for high temperature turbine applications. The two-phase Nb/Nb5Si3 in situ composites exhibit a good balance in mechanical properties. Using the 52 in drop tube, the effect of undercooling and rapid solidification on the solidification process and micro-structural characterization of Nb-Si eutectic alloy was studied. The microstructures of the Nb-Si composites were investigated by optics microscope (OM), X-ray diffraction (XRD) and scanning electron microscope (SEM) equipped with X-ray energy dispersive spectrometry (EDS). Up to 480 K, deep undercooling of the Nb-Si eutectic samples was successfully obtained, which corresponds to 25% of the liquidus temperature. Contrasting to the conventional microstructure usually found in the Nb-Si eutectic alloy, the microstructure of the undercooled sample is divided into the fine and coarse regions. The most commonly observed microstructure is Nb+Nb5Si3, and the Nb3Si phase is not be found. The change of coarseness of microstructure is due to different cooling rates during and after recalescence. The large undercooling is sufficient to completely bypass the high temperature phase field.

Undercooling and Rapid Solidification of Nb-Si Eutectic Alloys Studied by Long Drop Tube

Niobium-silicide alloys have great potential for high temperature turbine applications. The two-phase Nb/Nb5Si3 in situ composites exhibit a good balance in mechanical properties. Using the 52 in drop tube, the effect of undercooling and rapid solidification on the solidification process and micro-structural characterization of Nb-Si eutectic alloy was studied. The microstructures of the Nb-Si composites were investigated by optics microscope (OM), X-ray diffraction (XRD) and scanning electron microscope (SEM) equipped with X-ray energy dispersive spectrometry (EDS). Up to 480 K, deep undercooling of the Nb-Si eutectic samples was successfully obtained, which corresponds to 25% of the liquidus temperature. Contrasting to the conventional microstructure usually found in the Nb-Si eutectic alloy, the microstructure of the undercooled sample is divided into the fine and coarse regions. The most commonly observed microstructure is Nb+Nb5Si3, and the Nb3Si phase is not be found. The change of coarseness of microstructure is due to different cooling rates during and after recalescence. The large undercooling is sufficient to completely bypass the high temperature phase field.

EFFECT OF V, NB, AND TA DOPING ON THE 2223 PHASE-FORMATION AND THE CRYSTAL-STRUCTURE IN THE BISRCACUO SYSTEM

X-ray diffraction and electrical and diamagnetic analyses revealed that the 2223 phase was significantly enhanced by high-valence cation (V5+, Nb5+, Ta5+, etc.) doping in BiSrCaCuO samples. The optimum nominal composition was Bi1.6M0.4Sr2Ca2Cu3 O(y)(M =

Deformation, Phase Transformation and Recrystallization in the Shear Bands Induced by High-Strain Rate Loading in Titanium and its Alloys

alpha-titanium and its alloys with a dual-phase structure (alpha+beta) were deformed dynamically under strain rate of about 10(4) s(-1). The formation and microstructural evolution of the localized shear bands were characterized by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The results reveal that both the strain and strain rate should be considered simultaneously as the mechanical conditions for shear band formation, and twinning is an important mode of deformation. Both experimental and calculation show that the materials within the bands underwent a superhigh strain rate (9 x 10(5) s(-1)) deformation, which is two magnitudes of that of average strain rate required for shear band formation; the dislocations in the bands can be constricted and developed into cell structures; the phase transformation from alpha to alpha(2) within the bands was observed, and the transformation products (alpha(2)) had a certain crystallographic orientation relationship with their parent; the equiaxed grains with an average size of 10 mu m in diameter observed within the bands are proposed to be the results of recrystallization.

Metallographic Analysis of Cu-Zr-Al Bulk Amorphous Alloys with Yttrium Addition

Minor yttrium addition can improve the glass-forming ability of Cu-Zr-Al ternary alloys via suppression of the growth of eutectic clusters. Yttrium addition also makes the room temperature ductility of the alloys decrease, and both the compressive strength and elastic strain limits increase slightly.

Mechanism of nucleation and precipitation in Li containing Al-Zn-Mg-Cu alloys

Investigations on the aging hardening behavior of four Al-Li-Zn-Mg-Cu alloys were carried out using differential scanning calorimetry, transmission electron microscopy and hardness measurement. It is shown that the addition of Li inhibits the formation of Zn-rich G.P. zones in Al-Zn-Mg-Cu alloys. The dominant aging hardening precipitates is delta'(Al3Li) phase. Coarse T ((AlZn)(49)Mg-32) phase, instead of MgZn2, precipitates primarily on grain boundaries, and provides little strengthening. The multi-stop aging involving plastic deformation introduces in the matrix a high concentration of structural defects. These defects play different role on the nucleation of Zn-rich G.P. zones in different alloys. For the Li free alloy, structural defects act as vacancy sinks and tend to suppress the homogeneous precipitation of G.P. zones, while for the Li containing alloys, these defects promote the heterogeneous nucleation of G.P. zones and metastable MgZn2. A significant aging hardening effect is attained in deformed Li containing alloys due to the extra precipitation of fine MgZn2 in the matrix combined with deformation hardening.