中国及境外天山铅锌成矿作用与找矿方向

中国及境外天山铅锌矿床多有发现,如哈萨克斯坦Tekeli、Shalkiya和Achisai,乌兹别克斯坦Kurgashinkan和Uchkulach,塔吉克斯坦Altyntopkan,中国新疆乌拉根、彩霞山、阿齐山、阿尔恰勒等大型—超大型铅锌矿床,构成了天山巨型铅锌成矿带。这些铅锌矿床形成于怎样的地球动力学背景?铅锌成矿的基本地质特征是什么?有哪些重要成矿类型?受何要素控制?未来找矿突破方向在哪里?这些都是颇受关注的地质找矿问题。在广泛矿产地质调查和综合分析前人研究成果的基础上,将中国及境外天山作为整体,综述了天山造山带构造演化和重要铅锌成矿环境、典型矿床特征与成矿系统/成矿类型,总结了天山地区铅锌成矿演化过程,并分析了区域铅锌成矿特点与找矿突破方向。结果表明:天山造山带经历了前寒武纪古陆形成、洋-陆俯冲增生、陆-陆碰撞造山和陆内成盆4个地球动力学过程,先后出现了元古宙古陆边缘裂陷盆地、古生代洋-陆俯冲增生岛弧、晚古生代陆-陆碰撞造山与中—新生代山前/山间盆地4类重要铅锌成矿环境。在元古宙古陆边缘裂陷盆地环境,主要受同生断层、还原性细碎屑岩-碳酸盐岩建造等控制,形成了古陆边缘裂陷盆地铅锌成矿系统与SEDEX型铅锌矿床; 在古生代洋-陆俯冲增生岛弧环境,主要受弧岩浆活动、断裂构造、地层等控制,形成了增生岛弧铅锌成矿系统与矽卡岩型、斑岩型、岩浆热液脉型、VMS型铅锌矿床; 在晚古生代陆-陆碰撞造山环境,主要受被动陆缘海相碳酸盐岩、张性开放空间、逆冲推覆构造等控制,形成了碰撞造山铅锌成矿系统与MVT型铅锌矿床; 在中—新生代山前/山间盆地环境,主要受盆地三元结构、油气运移与红层“漂白”、硫酸盐岩等控制,形成了山前/山间盆地铅锌成矿系统与砂岩型铅锌矿床。由此可见,天山地区存在多种铅锌成矿环境和不同铅锌成矿系统与成矿类型,其铅锌成矿表现出长时间、多期次、多类型叠合成矿和一定继承性的演化特点。尽管沉积岩容矿铅锌矿床(包括SEDEX型、MVT型和砂岩型)在全球铅锌矿产资源中占据主导地位,而在天山地区增生岛弧铅锌成矿系统则占有更为重要的地位,特别是北天山岛弧带,哈萨克斯坦—伊犁板块南、北缘和中天山地块应该给予高度重视。与此同时,哈萨克斯坦—伊犁板块北缘与东天山中天山地块元古界SEDEX型铅锌找矿、境外中天山地块北缘与南天山造山带古生代被动陆缘碳酸盐岩地层MVT型铅锌找矿、新疆西南天山山前/山间盆地砂岩型铅锌找矿前景良好,也仍值得持续关注。

Phase transition and properties of Mg_3P_2 crystal structure under high pressure

Based on the first principles and CALYPSO crystal structure prediction method, the structure, phase transition behavior and physical properties of Mg₃P₂ crystal were studied in the pressure range of 0～100 GPA.The results show that under normal pressure, the space group of Mg₃P₂ crystal is Ia-3 cubic structure, with the lowest energy and the most stable structure, which is consistent with the experimental structure; At the pressure of 2.5 GPa, the crystal structure of Mg₃P₂ changes into monoclinic structure with space group P -3m1. When the pressure is 19.9 GPa, the phase of the crystal structure changes to monoclinic structure with C2/m space group. At 48.2 GPa, the phase of the crystal structure changes to Cmc 2₁ phase. The phonon dispersion relation of crystal structures is analyzed and shown that the four phases have no imaginary frequency in their Brillouin zone. The four phases have dynamic stability. The electronic properties of crystal structures are calculated, and the results show that the conduction band and valence band in the predicted Ia -3 phase, P -3m1 phase, C2/m phase and Cmc 2₁ phase do not overlap near the Fermi surface, indicating that the structure is non -metallic. The electron localization function of crystal structures revealed that there is a polar covalent bond between Mg and P atoms in the Ia -3, P -3m1, C2/m and Cmc 2₁ phases. Bader charge transfer calculations show that the P atom is the acceptor, the Mg atom is the donor, and the charge is transferred from the Mg atom to the P atom.