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1.
云南澜沧老厂花岗斑岩中锆石标型特征及地质意义   总被引:2,自引:2,他引:0  
运用Pupin的锆石标型研究方法,通过对锆石晶形的鉴定和统计来探讨云南省澜沧老厂花岗斑岩的成因信息。研究表明,本区花岗斑岩中的锆石有20种亚型,主要由{110}、{100}柱面和{101}、{211}锥面构成,其中柱面以{110}最为发育,锥面{101}和{211}都发育,但{101}较{211}更为发育;T.E.T曲线比较短,且主要分布在演化趋势图的右上角,表明锆石主要在低温过碱环境中形成,结晶速度较快,结晶温度范围750~600℃。锆石的结晶标型显示,本区隐伏花岗斑岩是以壳源为主的壳幔源混合成因的花岗斑岩。  相似文献   

2.
赣南淘锡坑锡矿床中锡石晶体形态学和地球化学研究   总被引:1,自引:0,他引:1  
黄品赟  汪相  陈洁  任名华  赖光兵 《地质论评》2012,58(5):987-1000
本文对淘锡坑锡矿床的含矿石英脉中的锡石晶体开展了晶体形态学和地球化学的系统研究。按晶面组合特征,淘锡坑锡矿床中的锡石可分为三种类型:由{111}锥面+{110}柱面共2个单形构成的A型锡石、由{111}锥面+{110}柱面+{100}柱面共3个单形构成的B型锡石和由{111}锥面+{101}锥面+{110}柱面+{100}柱面共4个单形构成的C型锡石。综合各种锡石晶型与结晶条件的资料分析,本文推测A型、B型锡石的结晶温度高于C型锡石的。本文首次利用电子探针分析仪对锡石进行阴极发光(CL)成像观测,发现淘锡坑锡矿床中的锡石经历了两期结晶作用:早期锡石以CL荧光亮度较小(黑色——暗灰色)为特征,边缘有明显的溶蚀痕迹,常见典型的韵律振荡构造和砂钟构造,其晶面组合特征显示了早期锡石属于A型或B型锡石;晚期锡石以CL荧光亮度较大(白色——浅灰色)为特征,往往沿着早期锡石的溶蚀边界面充填生长,一般不显示韵律振荡构造和砂钟构造,其晶面组合特征显示了晚期锡石属于C型锡石。电子探针分析显示,淘锡坑锡矿床中锡石的FeO、Ta2O5含量较高,指示其形成于高温热液环境;HfO2含量较高,Zr/Hf比值较低,说明成矿热液来源于高度分异的花岗质岩浆。两期锡石的FeO含量和In2O3含量的对比结果显示,早期锡石相对富FeO而贫In2O3,反映了早期锡石的结晶温度和压力均高于晚期锡石的,故两期锡石的结晶作用分别与淘锡坑矿床的两期岩浆热液成矿作用相关。  相似文献   

3.
为探讨后峪地区锆石的生长条件及其与该地区岩浆岩的成因和演化的关系,对本区不同岩体中的锆石形态标型进行了系统的研究。结果表明:不同岩体中锆石的长宽比大多集中在1.5∶1~3∶1之间,按Pupin锆石晶体类型分类,岩体中的锆石可划分为R2、P1-5、S2-5、S7-10、S12-15和S20等类型,说明锆石是在碱质岩浆中结晶,且结晶温度较低;岩体的液相线的温度为850~750℃,锆石大规模结晶温度为700~650℃。锆石的结晶作用从岩浆早期开始一直持续到岩浆后期,温度跨度大,持续时间长,说明岩浆为富水岩浆,有利于斑岩型矿床Cu-Mo-Au的矿化。本区岩浆岩的化学成分分析及不同岩体中锆石群类型的演化趋势图表明:本区岩浆除了壳源成因之外还有幔源成分加入其中,岩浆岩属于钙碱性系列(偏碱性)岩石。  相似文献   

4.
安徽茅坦A型花岗岩研究   总被引:22,自引:1,他引:21  
吴才来  黄许陈 《地质学报》1998,72(3):237-248
安徽茅坦花岗岩体是由4次侵入的细粒花岗岩、花岗斑岩、中粒花岗岩和粗粒花岗岩组成的复式岩体。各期次岩石具有高硅,富碱,富LREE、Y,Nb,Zr等大离子高电价元素及低Al、Mg,Ca、Ni、Cr,Ti,V的特点,与国内外A型花岗岩相似。岩石中副矿物种类聚多,以含碳硅石,磷钛矿等深源矿物为特征。锆石晶形以正锥面(111)和四方柱面(110)最为发育,与一般I型花岗岩有明显的差异。研究表明,该复式岩体为  相似文献   

5.
摘要福建建宁地区中元古代韩家、严塘二个岩体来自上地幔,其副矿物有28种。副矿物有三个结晶阶段,以富含自然铁、铬铁矿和富铪锆石为特征。锆石具高柱面指数和高锥面指数。变石英闪长岩和变英云闪长岩的锆石类型有二个主型和七个亚型。根据其副矿物标型组合及标型矿物特征,认为其物质来自幔源为主成因的岩浆。  相似文献   

6.
对个旧锡矿床的块状硫化物型、电气石细脉带型、含锡白云岩型、层间氧化矿型矿床中的锡石晶体运用扫描电镜、阴极发光成像技术、X-射线粉晶衍射、电子探针等试验开展了矿物学的系统研究。结果表明从块状硫化物型→电气石细脉带型→含锡白云岩型→层间氧化矿型矿床中的锡石有如下特征或变化规律:1颗粒体积依次变小。2深色的锡石到浅色锡石晶胞参数变大,c∶a值变小。3锡石晶体单型组合共有7种,单型从{111}锥面发育逐渐向{110}柱面发育。4锡石内部环带从均匀发育到不发育。以上特征均指示了4种矿床类型中锡石的形成温度依次降低。根据CL阴极发光下锡石亮度的差异,判断块状硫化物型、电气石细脉带型、含锡白云岩型矿床中锡石存在2个形成期次,认为此3类矿床在早阶段高温热液流体活动与早期锡石结晶作用有关,晚阶段低温热液流体活动与晚期锡石结晶作用有关。而层间氧化矿型矿床中的锡石具备悬浮在流体中生成的特征,可能为被流体搬运沉积形成,认为此矿床为重泥质沉积成因。  相似文献   

7.
锆石形态标型特征及标型生长机制探讨   总被引:4,自引:0,他引:4       下载免费PDF全文
本文在系统总结归纳不同研究者对锆石形态标型特征的研究成果基础上,重点从晶体生长、晶体化学和地球化学理论为重点探讨了锆石形态标型特征的生长机制。研究表明:锆石晶体结构中不同的面网方向,其平面内的原子组成、比例、化学键联结和键力以及面网间距和密度都是有差别的,由此决定了锆石晶体在不同的结晶介质条件下,不同面网的生长速度发生改变,生成相应的晶形。例如,尽管碱性元素并不进入锆石晶格,但它们可以影响Zr、Si、O离子的扩散速度,但是富钾和富钠的介质对锆石晶形发育的影响是有差别的,表现为:在富钾的介质中,将导致柱面的法向生长速度较锥面快得多,而锥面中,{111}的法向生长又较{311}快,由此决定了形成以{311}锥为主的双锥状晶体;在富钠的介质中,柱面和锥面都有一定程度的发育,但前者弱于后者,而柱面中,{100}的法向生长较{110}慢,由此决定了形成以{100}柱和{111}锥为主的短柱锥状晶体。根据类似方法,论证了其它形态标型特征的客观性,从而揭示了标型之间的内在联系和本质,展示了花岗岩研究中锆石形态标型特征应用推广的前景,也可为单颗粒锆石定年研究提供更多的分析应用价值  相似文献   

8.
海南岛千家复式岩体位于海南岛南部,发育有一系列的钼、银、铅锌矿床,目前对其开展的年代学工作缺少对整个复式岩体系统的年代学研究。对千家复式岩体各单元进行了系统的精确定年,LA-ICP-MS锆石U-Pb分析结果显示,各单元的侵位结晶年龄集中在100 Ma左右,表明各单元岩浆活动是同时侵位结晶的,可能是由同一岩浆房经过结晶分异演化形成的,原认为是早白垩世晚期的光头岭单元,现拟定为三叠纪岩浆活动产物。复式岩体成岩时代与华南白垩纪大规模成岩成矿时代相吻合,与受太平洋俯冲作用影响的华南岩石圈伸展作用相近(100~90 Ma)。  相似文献   

9.
漳州复式岩体锆石的标型特征及地球化学意义   总被引:1,自引:0,他引:1  
漳州复式岩体共分七次侵入(Ⅰ—Ⅶ),对区内Ⅱ至Ⅶ次岩体20个人工重砂的锆石作了大量测试研究和综合分析,确定了五种锆石类型:前身锆石、富锆锆石、富铪锆石、变生锆石及贫铪锆石。本文重点论述各类锆石的晶出产状,结晶形态,矿物物理、矿物化学特征及标型意义,并探讨标型特征的控制因素和地球化学条件。据锆石的标型和成因特征,提出本区Ⅱ—Ⅴ、Ⅶ次及Ⅵ次岩体分别与J.P.Pupin(1980)的地壳+地幔和地幔或以地幔为主成因的花岗岩相当。  相似文献   

10.
锆石柱面中Hf、Y的配位差异性及其对晶型的控制效应   总被引:1,自引:0,他引:1  
天然锆石的形态并不简单地依照PBC理论发育,它同时受到生长温度 、熔体扩散系数等物理参数的影响,以及置换Zr的杂质离子的种类和浓度等化学因素的制约 ,即杂质离子选择性地置换Zr而降低晶面的生长速度。通过对{100}和{110}柱面的半定量分 析发现,Hf4+、Y3+离子同O2-离子的成键数目在{100}与{110}生长层 上是不同的,且Hf-O的键强比Zr-O的大,而Y-O的键强比Zr-O的小。如果假定晶体与岩浆熔体并未达到真正的平衡,而是各晶面与岩浆熔体分别达到平衡,按热力学中浓度与能量变化的指数律去处理Hf和Y在{100}与{110}晶面上的配分可以得到,{100}晶面上趋于富Hf贫 Y,{110}晶面上趋于富Y贫Hf,从而导致富Hf的锆石上{100}优先发育,富Y的锆石上{110}优 先发育。  相似文献   

11.
黑龙江省饶河县石场一带分布的跃进山杂岩为一套富含晚三叠世化石的海陆交互相沉积地层.砾岩样品中的LA-ICP-MS锆石U-Pb测年结果显示,样品中的碎屑锆石年龄谱具有4组年龄,分别为800 Ma以上、500 Ma、251~284 Ma和219~222 Ma.前三者与佳木斯地块中的热事件年龄完全一致,表明其沉积物源主要来自佳木斯地块;后者为砾岩最小年龄组,大致可将这组最小年龄视为这套砾岩的沉积时代下限,与西侧松辽地块东缘的张广才岭地区广泛分布的210~228 Ma的晚三叠世早期花岗岩基本一致,说明具有最小年龄组的碎屑锆石可能来自松辽地块东部.碎屑锆石年龄及其源区特征表明,在晚三叠世之前,跃进山增生杂岩已经就位在佳木斯地块东缘,并成为佳木斯地块东部大陆边缘的一部分.  相似文献   

12.
黑龙江省饶河县石场一带分布的跃进山杂岩为一套富含晚三叠世化石的海陆交互相沉积地层.砾岩样品中的LA-ICP-MS锆石U-Pb测年结果显示,样品中的碎屑锆石年龄谱具有4组年龄,分别为800 Ma以上、500 Ma、251~284 Ma和219~222 Ma.前三者与佳木斯地块中的热事件年龄完全一致,表明其沉积物源主要来自佳木斯地块;后者为砾岩最小年龄组,大致可将这组最小年龄视为这套砾岩的沉积时代下限,与西侧松辽地块东缘的张广才岭地区广泛分布的210~228 Ma的晚三叠世早期花岗岩基本一致,说明具有最小年龄组的碎屑锆石可能来自松辽地块东部.碎屑锆石年龄及其源区特征表明,在晚三叠世之前,跃进山增生杂岩已经就位在佳木斯地块东缘,并成为佳木斯地块东部大陆边缘的一部分.  相似文献   

13.
M.-A. Kaczmarek  S.M. Reddy  N.E. Timms 《Lithos》2011,127(3-4):414-426
Magmatic zircons within two sheared gabbroic dykes from the peridotitic massif of Lanzo (Western-Alps, Italy) revealed evolution of deformation from crystal plasticity to rigid body rotation during shear zone evolution. This is the first time that multiple zircon grains have been analysed in a kinematic context in a shear zone. Zircon grains recorded crystal plastic deformation activating the commonly inferred <100>{001} and <001>{100} glide-systems to the newly identified <001>{110} glide-system. The exact selection of glide-system could be dependant of deformation conditions such as pressure, temperature, and strain rate. Moreover, the activation of one or several glide-systems within a single grain could be favoured by the primary orientation of the grains combined with a high strain rate. In these sheared gabbros, the deformation mechanisms evolve from plastic deformation at low strain rate conditions to increase strain, strain softening and localisation of deformation. The progressive shear zone development and the softening of the matrix relative to the zircon has lead to a switch from crystal-plasticity to rigid body rotation of zircon. The zircon grains rigid body rotation involved that their long axes became parallel to the lineation of the shear zone, causing reorientation and dispersion of the misorientation axes away from kinematic Y.  相似文献   

14.
The deformation-related microstructure of an Indian Ocean zircon hosted in a gabbro deformed at amphibolite grade has been quantified by electron backscatter diffraction. Orientation mapping reveals progressive variations in intragrain crystallographic orientations that accommodate 20° of misorientation in the zircon crystal. These variations are manifested by discrete low-angle (<4°) boundaries that separate domains recording no resolvable orientation variation. The progressive nature of orientation change is documented by crystallographic pole figures which show systematic small circle distributions, and disorientation axes associated with 0.5–4° disorientation angles, which lie parallel to rational low index crystallographic axes. In the most distorted part of the grain (area A), this is the [100] crystal direction. A quaternion analysis of orientation correlations confirms the [100] rotation axis inferred by stereographic inspection, and reveals subtle orientation variations related to the local boundary structure. Microstructural characteristics and orientation data are consistent with the low-angle boundaries having a tilt boundary geometry with dislocation line [100]. This tilt boundary is most likely to have formed by accumulation of edge dislocations associated with a 〈001〉{100} slip system. Analysis of the energy associated with these dislocations suggest they are energetically more favorable than TEM verified 〈010〉{100} slip. Analysis of minor boundaries in area A indicates deformation by either (001) edge, or [100](100) and [001](100) screw dislocations. In other parts of the grain, cross slip on (111), and (112) planes seems likely. These data provide the first detailed microstructural analysis of naturally deformed zircon and indicate ductile crystal-plastic deformation of zircon by the formation and migration of dislocations into low-angle boundaries. Minimum estimates of dislocation density in the low-angle boundaries are of the order of ∼3.1010 cm−2. This value is sufficiently high to have a marked effect on the geochemical behavior of zircon, via enhanced bulk diffusion and increased dissolution rates. Therefore, crystal plasticity in zircon may have significant implications for the interpretation of radiometric ages, isotopic discordance and trace element mobility during high-grade metamorphism and melting of the crust.  相似文献   

15.
Based on microprobe work, we present arguments that the size relations of the two common prisms {100} and {110} of accessory granite zircons are strongly influenced by chemical factors. Magmatic growth zoning patterns, which we have studied by means of backscattered electron imaging in special zircon sections orientated perpendicular to the c-axis, do not support previous models which assumed temperature or the degree of ZrSiO4 supersaturation to be the primary prism-form-directing factors. The element U, which usually occupies the Zr-sites of granite zircoms to some degree, is strongly suspected of producing an (adsorptive) growth-blocking effect for {110}-type faces thus creating crystals with {110}-dominated prism morphology. A second independent mechanism that is likely to form zircons with large {110} prisms is the common substitution Zr4++Si4+ versus Y(REE) and P contents (relative to Zr) are, according to our model, predestinated to produce zircons with large {100} prisms and vice versa.Dedicated to Prof. Günther Frasl on the occasion of his seventieth birthday  相似文献   

16.
黄铁矿成因形态学   总被引:25,自引:5,他引:20  
在1981—1986年野外工作的基础上,作者对胶东三县四个金矿床黄铁矿晶体形态进行了系统研究,对其中2495粒晶体进行了统计,对300粒晶体进行了测角,对60粒晶体进行了微形貌观察。根据以上实际工作及国内外有关资料提出了黄铁矿晶休常见单形出现频率的定量资料与晶体微形貌的特点,特别是{210}面上负条纹的特征与成因探讨。并讨论了黄铁矿晶体形态与分带性,与形成温度,与主、微量成分,与共生组合及与矿化等的关系。查明黄铁矿形态及其晶面微形貌的发育与硫逸度、温度、冷却速度等密切相关。在以上基础上提出了胶东四个金矿床中蚀变岩型金矿及石英脉型金矿两种成因类型黄铁矿形态特征上的五点差异。最后对黄铁矿研究方法要点进行了总结。  相似文献   

17.
Li diffusion in zircon   总被引:2,自引:2,他引:0  
Diffusion of Li under anhydrous conditions at 1 atm and under fluid-present elevated pressure (1.0–1.2 GPa) conditions has been measured in natural zircon. The source of diffusant for 1-atm experiments was ground natural spodumene, which was sealed under vacuum in silica glass capsules with polished slabs of zircon. An experiment using a Dy-bearing source was also conducted to evaluate possible rate-limiting effects on Li diffusion of slow-diffusing REE+3 that might provide charge balance. Diffusion experiments performed in the presence of H2O–CO2 fluid were run in a piston–cylinder apparatus, using a source consisting of a powdered mixture of spodumene, quartz and zircon with oxalic acid added to produce H2O–CO2 fluid. Nuclear reaction analysis (NRA) with the resonant nuclear reaction 7Li(p,γ)8Be was used to measure diffusion profiles for the experiments. The following Arrhenius parameters were obtained for Li diffusion normal to the c-axis over the temperature range 703–1.151°C at 1 atm for experiments run with the spodumene source:
D\textLi = 7.17 ×10 - 7 exp( - 275 ±11 \textkJmol - 1 /\textRT)\textm2 \texts - 1. D_{\text{Li}} = 7.17 \times 10^{ - 7} { \exp }( - 275 \pm 11\,{\text{kJmol}}^{ - 1} /{\text{RT}}){\text{m}}^{2} {\text{s}}^{ - 1}.  相似文献   

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