山东山城金矿Ⅰ号脉矿物找矿标型

I号矿脉是山城金矿区中主要的工业矿体之一.黄铁矿和石英是主要的载金矿物,其标型特征是在矿脉空间上有规律的分布.矿体上部的黄铁矿以聚形晶为主,主要是八面体和立方体聚形晶以及立方体、八面体和五角十二面体聚形晶.黄铁矿的电物理性质,vnp＞|-17|,α＞|-120|.石英相对吸光度D1、D2、D2/D3、D3/D1、D2+3/D1相对较大.矿体下部的黄铁矿晶体形态主要是立方体单晶和立方体与八面体聚形晶,vnp＜|-17|,α＜|-120|,D1、D2、D2/Da、Da/D1、D2+3/D1相对较小.依据矿物标型展布规律,结合矿脉金含量的分布、载金矿物黄铁矿的晶体形态和热电性,以及石英相对吸光度的空间展布特征,建立了矿物学找矿模型,对深部矿脉进行了预测.     

山东山城金矿I号脉矿物找矿标型

Ⅰ号矿脉是山城金矿区中主要的工业矿体之一。黄铁矿和石英是主要的载金矿物 ,其标型特征是在矿脉空间上有规律的分布。矿体上部的黄铁矿以聚形晶为主 ,主要是八面体和立方体聚形晶以及立方体、八面体和五角十二面体聚形晶。黄铁矿的电物理性质 ,vnp>|- 17|,α >|- 12 0 |。石英相对吸光度D1、D2 、D2 /D3 、D3 /D1、D2 + 3 /D1相对较大。矿体下部的黄铁矿晶体形态主要是立方体单晶和立方体与八面体聚形晶 ,vnp<|- 17|,α <|- 12 0 |,D1、D2 、D2 /D3 、D3 /D1、D2 + 3 /D1相对较小。依据矿物标型展布规律 ,结合矿脉金含量的分布、载金矿物黄铁矿的晶体形态和热电性 ,以及石英相对吸光度的空间展布特征 ,建立了矿物学找矿模型 ,对深部矿脉进行了预测     

团结沟斑岩金矿床自然金的成因矿物学研究

团结沟斑岩金矿床的地质特征,已有文章论述,本文仅就该区自然金成因矿物学的研究成果介绍如下。一、自然金的矿物标型根据自然金的颗粒大小及在矿物中的赋存状态,将该区自然金大致分为三类。第一类金为矿石及脉石矿物中的次显微金,据透射电镜研究,次显微金一般是0.2—0.05微米,呈圆球状、链状赋存在硫化矿物之中,其分布方式与寄主矿物的结晶形态有很大关系,在结核状或同心圆状的白铁矿之中,次显微金沿其边缘呈同心环状分布,少部分在晶体间隙内。部分次显微金呈立方体{100}及八面体{111}的聚形晶产出。     

沁水盆地晚古生代煤中硫的地球化学特征及其对有害微量元素富集的影响

煤中硫是多种有害微量元素的重要载体。基于形态硫分析、电感耦合等离子质谱及X射线衍射等方法分析沁水盆地晚古生代煤中硫和有害微量元素的分布规律,探讨了煤中硫对有害微量元素富集的影响,运用带能谱的扫描电镜和光学显微镜划分煤中硫化物的微观赋存特征。结果表明,沁水盆地煤中硫整体上以有机硫为主,平均占全硫的78%,只有在太原组个别高硫煤中以黄铁矿硫为占优势。显微镜和扫描电镜下可识别出煤中黄铁矿的微观赋存状态包括莓球状、薄膜状、晶粒状、结核状、团窝状黄铁矿和细粒黄铁矿集合体,白铁矿的微观赋存特征包括聚片状、板状和矛头状白铁矿,部分白铁矿与黄铁矿共生。沁水盆地煤中有害微量元素含量整体较低,黄铁矿是有害微量元素As、Se和Hg的重要载体,而有机硫决定了煤中U的富集。研究认为,成煤时期海水对泥炭沼泽的影响导致太原组煤中全硫和黄铁矿硫较高,太原组煤中硫的来源具有多样性,煤中黄铁矿具有多阶段演化的特点。     

鄂西宜昌地区下寒武统水井沱组草莓状黄铁矿SEM图像特征及古环境指示意义：以鄂阳页1井为例

草莓状黄铁矿在页岩中广泛分布,其形态特征及粒径大小等可作为指示氧化还原状态的环境指标。本文以鄂西宜昌地区鄂阳页1井水井沱组富有机质层段及岩家河组样品为研究对象,利用氩离子抛光-场发射扫描电镜技术,结合图像处理软件ImageJ,快速获取SEM图像中草莓状黄铁矿相关参数,并探讨其环境指示意义。结果表明,鄂阳页1井下寒武统剖面样品中黄铁矿赋存形式多样,包括草莓状黄铁矿集合体、团块状黄铁矿、黄铁矿自形晶及有机质中星点状分散的黄铁矿等。其中,草莓状黄铁矿作为最主要的赋存形式,其粒径(D)、微晶粒径(d)、D/d值以及微晶晶型等相关参数在垂向上呈现明显变化。岩家河组草莓状黄铁矿微晶晶型以八面体为主,水井沱组富有机质层段底部以五角十二面体及近球形为主,中部以八面体、立方体为主,上部以立方体、四面体为主,自下而上微晶圆度呈逐渐减小趋势,反映了还原性减弱的过程。水井沱组富有机质页岩中草莓状黄铁矿平均粒径为4.43μm,中下部偏大,上部粒径偏小。草莓状黄铁矿微晶平均粒径为0.338μm,剖面上自下而上呈现由大到小的变化趋势。D/d值在岩家河组样品中偏小,在水井沱组富有机质层段下部最大,上部逐渐减小。综合相...     

黄铁矿加热相变特征的XRD初步研究

<正>黄铁矿,化学成分FeS2,其晶体属等轴晶系的硫化物矿物。常见晶形是立方体、五角十二面体、八面体及它们的聚形。立方体晶面上有与晶棱平行的条纹,各晶面上的条纹相互垂直。     

利用电子探针研究甘肃陇南赵家庄金矿载金矿物特征

应用偏光显微镜与电子探针相结合的手段是研究载金矿物的主要方法。本文采用镜下鉴定和电子探针分析技术,对赵家庄金矿中载金矿物含量、形态特征及其与其他矿物的空间关系开展研究,并对载金矿物进行定性和定量分析,探寻具有找矿意义的载金矿物和总结标志矿物特征。结果表明:研究区金矿石中主要载金矿物为黄铁矿,少量为黄铜矿、闪锌矿,这些载金矿物中Au含量依次为:细晶黄铁矿粗晶黄铁矿草莓状黄铁矿黄铜矿。不同时期的黄铁矿(粗晶黄铁矿、细晶黄铁矿、草莓状黄铁矿)中Au的分布均匀,但存在差异性,主要表现为细晶黄铁矿和草莓状黄铁矿中的Au含量较高(平均含量0. 14%～0. 18%),这种现象表明此类矿物为构造热液期形成,金易富集。Au以两种形式存在,一种是"可见金"包裹于脉石矿物中,或以裂隙金的形式嵌布在矿物晶隙及裂隙中;另一种是"不可见金"以纳米级颗粒金的形式存在于载金矿物中,也是Au的主要存在形式。本研究为后期矿床的成因、成矿过程和成矿机理研究提供了佐证,同时易于根据含金矿物的特征选择合适的选冶方法。     

铜陵包村金(铜)矿床中胶状黄铁矿矿物学及成因解析

黄铁矿是安徽铜陵包村金(铜)矿床中主要硫化物,对热液成因的显晶质黄铁矿已有大量研究,而胶状黄铁矿研究较少且成因存在争议.本文以粉晶X射线衍射、扫描电镜(SEM)、透射电镜(TEM)以及拉曼光谱(RS)为主要研究方法和手段,对包村金(铜)矿床中胶状黄铁矿的矿物组成和微结构进行研究.包村胶状黄铁矿主要由黄铁矿组成,含有白铁矿、菱铁矿、石英、含铁白云石、高岭石和有机质.黄铁矿主要以纳米-亚微米粒径的自形、半自形的立方体为主,少量微米级他形颗粒,显著不同于胶体或非晶态的无定型黄铁矿.由黄铁矿、白铁矿和有机质组成的胶状结构中,白铁矿和有机质富集在暗色环带,黄铁矿相对富集在浅色环带,浅色和暗色交替变化主要由三者含量变化所致,与矿物粒径无关.结合铜陵地区胶状黄铁矿研究成果,我们认为铜陵地区乃至长江中下游成矿带内铜-金-铁多金属硫化物矿床相关研究文献中记载的胶状黄铁矿为铁硫化物、碳酸盐矿物、黏土矿物、石英和有机质组成的矿物集合体,是在陆源物质输入受限的半封闭海盆环境下经生物化学作用直接沉淀的纳米-亚微米黄铁矿为主的矿物集合体.虽然胶状黄铁矿经历沉积成岩作用和中生代岩浆热液叠加改造作用,但是沉积微结构、矿物成因信息仍然被有效保存.     

白铁矿转变和黄铁矿前身物的岩相学鉴定

利用综合的关于由白铁矿合成的黄铁矿，以及由白铁矿和磁黄铁矿形成的黄铁矿的天然样品的特征，就能识别薄片中由白铁矿转变和由磁黄铁矿氧化淋滤而形成的黄铁矿。由白铁矿转变而形成的黄铁矿的特征有：其孔隙空间约为实际矿物的２％，孔隙内无副产物充填，光学各向异性（暗绿至暗红色）和呈相对于白铁矿母晶具两个取向的他形子体黄铁矿晶畴。由磁黄铁矿氧化溶解（与淋滤作用相反）形成的黄铁矿或白铁矿的特征有：孔隙空间达实际矿物     

草莓状黄铁矿形成机制及其研究意义

黄铁矿是沉积物中较为常见的矿物之一,而草莓状黄铁矿是由等粒度的亚微米级黄铁矿晶体或微晶体紧密堆积而成。基于已有的草莓状黄铁矿相关研究成果,本文综述了草莓状黄铁矿的形成机制,阐述了其对古环境恢复的意义。目前普遍认为草莓状黄铁矿的成因主要有两种,即有机成因和无机成因,前者认为有机质或细菌参与草莓状黄铁矿形成;而后者主要认为过饱和的黄铁矿浓度是微球粒草莓状黄铁矿形成的必备条件。草莓状黄铁矿粒径的大小是其古沉积环境的直接反映,被作为比较可靠的古氧化还原条件判别指标,已被广泛应用于古代及现代海洋沉积物的古环境恢复。目前,虽然草莓状黄铁矿粒径判别古环境的大小及分布范围还不统一,但普遍认为封闭的水体环境（硫化环境）草莓状黄铁矿粒径较小且变化不大,且随着含氧程度增加,草莓状黄铁矿的粒径大小增大且分布范围趋于加宽。     

The differential enrichment mechanism of thallium in the Huodehong MVT deposit,NE Yunnan Province,China: Evidence from EBSD,LA-ICPMS and TEMSCIEI北大核心CSCD

铊(Tl)是一种战略性关键金属,在高科技领域具有重要用途。作为“稀散元素”之一,Tl主要富集于低温贱金属硫化物矿床中,黄铁矿和白铁矿是其主要载体矿物。滇东北火德红MVT铅锌矿床中黄铁矿和白铁矿显示Tl的富集,其中白铁矿中Tl含量显著高于黄铁矿,为探究Tl在不同矿物之间的差异性富集机制提供了理想对象。本文对火德红矿床共生黄铁矿-白铁矿开展系统的结晶学、矿物学和地球化学研究。电子背散射衍射(EBSD)结果表明,热液黄铁矿、白铁矿晶粒组构具有一定继承性,与闪锌矿紧密共生,暗示为同一成矿事件的产物。激光剥蚀耦合等离子体质谱(LA-ICPMS)原位微量元素含量分析结果显示,黄铁矿和白铁矿中的Tl含量分别为127×10^(-6)~516×10^(-6)和356×10^(-6)~1046×10^(-6),不同含量测点Tl的激光剥蚀时间分辨元素信号曲线均较为平滑,暗示Tl主要以类质同象形式进入黄铁矿和白铁矿晶格。透射电镜(TEM)进一步证实Tl类质同象直接替换Fe为主,即2Tl^(+)←→□(空位)+Fe^(2+)。结合黄铁矿和白铁矿中Tl与Zn含量的正相关关系,本文认为白铁矿中Tl的超常富集可能与偏酸性条件下富Tl、Zn和Fe等金属成矿流体有关。综合研究表明,火德红矿床黄铁矿与白铁矿中Tl的差异性富集与晶体结构、Tl赋存状态无关,而是流体成分、物化条件共同制约的结果,受到矿物和矿床等不同尺度苛刻成矿条件的影响。与闪锌矿共生的白铁矿是未来寻找铊资源的重要方向。     

An occurrence of secondary sulfides from Leg 37 basalts

Two types of secondary sulfides occur on the walls of a vesicle in slightly altered basalt recovered from site 332A of DSDP Leg 37. The first consists of euhedral crystals of pure pyrite, with occasional small partial overgrowths of fibrous chalcopyrite, embedded within smectite (altered glass) which lines the vesicle. The second type occurs as small composite sulfide spherules lightly attached to the surface of the smectite. The spherules are composed of pyrite crystallites arranged in approximate pyritohedral symmetry, with marcasite crystallites decorating the pyritohedron edges. Precession camera photographs and optical studies suggest the marcasite and pyrite grew simultaneously from a pyrite nucleus, with marcasite adopting the pyrite growth habit. These spherules differ sharply from the magmatic sulfide spherules previously described.     

黄铁矿与沥青铀矿的共生条件及在沥青铀矿形成过程中所起作用的实验研究

高价铁与高价铀混合溶液在还原场中形成了共生的黄铁矿与沥青铀矿,该过程必须在弱酸性-中性-碱性介质中进行,其中在弱酸性至中性介质中易形成大的黄铁矿单晶。高价铀溶液流经黄铁矿矿区时,若在高温高压条件下,有新生的黄铁矿或白铁矿与沥青铀矿共生。黄铁矿还原六价铀形成沥青铀矿时,起还原作用的是二价硫。赤铁矿常与沥青铀矿共生,但它们是热液演化过程中不同阶段的产物,赤铁矿形成于体系氧逸度高的氧化环境,沥青铀矿形成于体系氧逸度低的还原环境,赤铁矿形成于沥青铀矿之前。     

Atomistic simulation of the structure and elastic properties of pyrite (FeS2) as a function of pressure

Interatomic potential parameters have been derived at simulated temperatures of 0 K and 300 K to model pyrite FeS₂. The predicted pyrite structures are within 1% of those determined experimentally, while the calculated bulk modulus is within 7%. The model is also able to simulate the properties of marcasite, even though no data for this phase were included in the fitting procedure. There is almost no difference in results obtained for pyrite using the two potential sets; however, when used to model FeS₂ marcasite, the potential fitted at 0 K performs better. The potentials have also been used to study the high-pressure behaviour of pyrite up to 44 GPa. The calculated equation of state gives good agreement with experiment and shows that the Fe–S bonds shorten more rapidly that the S–S dimer bonds. The behaviour of marcasite at high pressure is found to be similar to that of pyrite.     

Morphology and formation mechanism of pyrite induced by the anaerobic oxidation of methane from the continental slope of the NE South China Sea

In order to understand the response of authigenic pyrite to gas hydrate geo-systems, pyrite tubes or rods at the sulfate–methane transition (SMT) zone of core GC10 from the northern continental slope of the South China Sea (SCS) were investigated. In situ X-ray diffraction (XRD) results show that the pyrite tube consists of pyrite micro-crystals with trace amount of graphite in the inner tube. Scanning electron microscope (SEM) observations of pyrite tubes indicate various aggregations in the form of framboidal, euhedral, and colloidal pyrite microcrystals. Typical framboidal pyrite is considered as packing of octahedral microcrystals. Interestingly, many framboids in the tubes consist of round or irregular microcrystals and have an outer crust that consists of secondary pyrite. The size of the framboids in the inner wall of the tube is larger than that in the middle wall or foraminifer-filled pyrite. High-resolution transmission electron microscopic (HRTEM) images show marcasite lamellae defects in the spherulitic pyrite crystals, which reveal different solution conditions during the pyrite precipitation. Nano-foil-like graphitic carbon was observed to be closely associated with the pyrite spherules. The occurrence of both marcasite layers and nano-foil-like graphitic carbon suggest that the migration of methane from deep sediment. It is suggested that the formation of pyrite serves as a catalyst during the reaction from methane to elemental carbon under the anaerobic oxidation of methane. Meanwhile, this reaction results in local acidification of the solution inside the pyrite tubes, which favors marcasite lamellae growth on the host pyrite substrate.     

美国内华达卡林金矿之含金FeS2微晶中不可见金的TEM研究和地球化学模型

透射电子显微术的研究表明,美国内华达州卡林金矿中环绕黄铁矿大 晶体的Fe的硫 化物微晶乃是白铁矿。该白铁矿含Au和As,并在其中有纳米尺度的似带状区。相对于邻区 而言,似带状区相对富As。因而提出：似带状区还相对富晶格金。根据所得出的方解石中三 价阳离子的分配系数方程认为,Au3＋阳离子是在白铁矿的非平衡(快速)结晶 作用期间,从白铁矿－溶液界面上被结合到细粒白铁矿中去的。Au3＋在白铁矿中的 配分是由非平衡分布系数(Kd')所控制的。然而,由于Au 3＋的平衡分 配系数(Kd)小,故通过平衡(缓慢)结晶作用形成的黄铁矿并不将Au 3 ＋结合到晶体中去。早期形成的细粒晶体的再结晶作用则将把REE和Au从晶体中迁移走。 相对于正常的白铁矿结构而言,较大的Au3＋和Au＋阳离子结合进入到白铁矿晶格 中,可引起局部的结构畸变,从而表现为似带状的特征。     

The Existence of the Negative Charge of Gold in Sulphide Minerals and Its Formation Mechanism1;

Abstract: Through a study, particularly an X-ray photoelectron spectroscopy (XPS or ESCA) analysis, of gold-bearing arsenopyrite and pyrite in Carlin-type gold deposits of Guangxi, China, and hydrothermally synthesized gold-bearing pyrite and marcasite, the authors have found that these minerals contain “invisible gold” whose binding energy is lower than that of native gold (Au°). Therefore they suggest that gold occurs in a negative charge state in these sulphide minerals as it replaces some sulphur and is combined with sulphur with the covalent bond. This paper also preliminarily discusses the possibility of its formation from the chemistry and geochemistry of gold, crystal chemistry of arsenopyrite, pyrite and marcasite and geochemical environment.     

The 57Fe Mössbauer parameters of pyrite and marcasite with different provenances

Eighteen pyrite and twelve marcasite samples which have different provenances have been investigated to determine the systematics of the influence of mineralogical and geological factors on the ⁵⁷Fe Mössbauer spectra at 298 K. The following results have been obtained: there is no ambiguity in distinguishing single phase pyrite from single phase marcasite by means of ⁵⁷Fe Mössbauer spectroscopy at 298 K. At 298 K the average electric quadrupole splitting, 〈ΔE_Q〉, and average isomer shift, 〈δ〉, with respect to Fe metal, are 0.6110 ± 0.0030 mm s^?1 and 0.313 ± 0.008 mm s^?1, respectively, for the 18 pyrites; 〈ΔE_Q〉 = 0.5030 ± 0.0070 mm s^?1 and 〈δ〉 = 0.2770 ± 0.0020 mm s^?1 for the 12 marcasites. At 77 K, ΔE_Q is 0.624 mm s^?1 for pyrite and 0.508 mm s^?1 for marcasite. In distinguishing pyrites from marcasites, spectra obtained at 77 K are not warranted.The Mössbauer parameters of pyrite and marcasite exhibit appreciable variations, which bear no simple relationship to the geological environment in which they occur but appear to be selectively influenced by impurities, especially arsenic, in the pyrite lattice. Quantitative and qualitative determinations of pyrite/marcasite mechanical mixtures are straightforward at 298 K and 77 K but do require least-squares computer fittings and are limited to accuracies ranging from ±5 to ±15 per cent by uncertainties in the parameter values of the pure phases. The methodology and results of this investigation are directly applicable to coals for which the presence and relative amounts of pyrite and marcasite could be of considerable genetic significance.