北秦岭官坡地区高压—超高压榴辉岩岩相学及变质作用研究

北秦岭官坡地区的榴辉岩及含柯石英榴辉岩产在帮岭岩群的北侧，主要由绿辉石和石榴石组成，部分石榴石和绿辉石中含柯石英包体。此外还含有退变质的多硅白云母、角闪石、黝帘石和纳长石等矿物，根据变质矿物之间的替代关系及共生组合规律，榴辉岩退变质作用可划分为四个阶段，各阶段代表性矿物组合依次为：柯石英＋绿辉石＋石榴石；石英＋绿辉石＋石榴石；多硅白云母＋绿辉石＋石榴石＋石英；角闪石＋斜长石＋白云母＋黑云母。这四个     

鲁东造山带榴辉岩变质作用特征及其动力学机制

岩相学研究表明,广泛发育鲁东造山逞中的榴辉岩可以划分为四种类型：第一类为含柯石英及其假象榴辉岩;么二类为含蓝晶石 、黝帘石及多硅白云母等榴辉岩;第三类为石榴石－绿辉石－石英组合榴辉岩;第四类为（角闪石）石榴石－辉及有关岩石（非典型“榴辉岩”）。这四类榴辉岩峰期前进变质矿物共生组合及Ｐ－Ｔ条件估算结果均显示它们应属于高温与超高压变质作用产物,其变质作用ＰＴｔ轨迹表现为顺时针演化趋势,反映出板块俯冲碰     

新疆西南天山哈布腾苏一带榴辉岩的岩石学特征及变质作用P-T轨迹

西南天山哈布腾苏河沿岸的含石墨的石榴石多硅白云母石英片岩中出露一套若干大小不等的布丁状变基性岩块,产状与区域面理一致。本文对其中保存完好的榴辉岩体进行了较为细致的岩石学研究和温压演化条件计算。根据主要矿物的含量,将该套榴辉岩大致分为两类—角闪榴辉岩和钠云母榴辉岩,二者的主要矿物均为 Grt Omp Na-Ca-Amp Pg Dol/Cal Rt±Qtz。石榴石变斑晶两阶段生长明显,从核部到边部 X_(Mn)和X_(Fe)降低,X_(Mg)和 X_(Ca)升高,指示了升温降压的变质过程。根据石榴石核部和边部的包体组合特征,确立了两期榴辉岩相变质作用:前一阶段经历了高压但较低温的硬柱石-硬绿泥石(仅见假象)榴辉岩相,变质温度为400～500℃,压力不低于1.8～1.9GPa,表明早期经历了快速俯冲过程;后一阶段的变质温度为570±30℃,压力为2.0～2.5GPa。在退变质绿帘角闪岩相阶段,形成低压脉体(矿物组合为 Ab Di Na-Ca-Amp Ep/Czo Cal)和一系列退变质反应结构,如 Dol 的 Cal 增生边,Omp 的 Di Ab 后成合晶结构。利用 Dol-Cal 分溶温度计和 Di的 Jd 分子含量得到该阶段的温度约500～530℃,压力小于0.9～1.1GPa,表明其退变质经历的是降温降压过程。这与利用Thermocalc 3.1在 NCFMASH 体系下计算的 PT 视剖面图是一致的。     

青藏高原拉萨地块松多榴辉岩的岩相学特征和变质演化过程

松多榴辉岩出露于拉萨地块的石英片岩中,主要由较为基性的金红石榴辉岩和较为酸性的石英榴辉岩组成。榴辉岩相矿物组合为石榴子石 绿辉石 绿帘石±多硅白云母±石英±金红石。岩石发生了较强烈的退变质作用,退变质矿物有角闪石、绿帘石、石英、钠长石及绿泥石。石榴子石变斑晶具有生长环带结构,变斑晶和基质石榴子石主要落入C类榴辉岩区,少数石榴子石变斑晶边部和基质石榴子石落入B类榴辉岩区;单斜辉石主要为绿辉石,少数Ⅰ世代和Ⅲ世代为普通辉石;角闪石均为钙质角闪石。根据石榴子石-绿辉石-多硅白云母矿物温压计计算,获得的温压范围为630～777℃和2.58～2.70GPa,峰期变质条件接近于石英-柯石英转变线。榴辉岩的原岩经历了从高绿片岩相、角闪岩相、榴辉岩相、角闪岩相到高绿片岩相的变质过程,这反映了与古特提斯洋闭合有关的俯冲进变质作用和随后的折返退变质作用。     

Experimental Investigation of Eclogite Rheology and Its Fabrics at High Temperature and Pressure

Eclogite plays an important role in mantle convection and geodynamics in subduction zones. An improved understanding of processes in the deeper levels of subduction zones and collision belts requires information on eclogite rheology. However, the deformation processes and associated fabrics in eclogite are not well understood. Incompatible views of deformation mechanism have been proposed for both garnet and omphacite. We present here deformation behaviour of eclogite at temperatures of 1027–1427 °C, confining pressures of 2.5–3.5 GPa, and strain rates of 1 × 10^?5 s^?1 to 5 × 10^?4 s^?1. We obtained a power‐law creep for the high temperature and pressure deformation of a ‘dry’ eclogite (50 vol.% garnet, 40% omphacite and 10% quartz) with A = 10^{3.3 ± 1.0}, n = 3.5 ± 0.4, ΔE =403 ± 30 KJ mol^?1 and ΔV = 27.2 cm³ mol^?1. The two principal minerals of eclogite have greatly different strengths. Progressive increase of garnet results in a smooth increase in strength. Analysis by electron back‐scattered diffraction shows that: (1) garnet displays pole figures with near random distributions of misorientation angle under both dry and wet conditions; (2) omphacite shows pronounced lattice preferred orientations (LPOs), suggesting a dominant dislocation creep mechanism. Further investigation into the water effects on eclogite show: (3) water content does not influence the style of omphacite fabric but increases slightly the fabric strength; (4) grain boundary processes dominate the deformation of garnet under high water fugacity or high shear‐strain conditions, yielding a random LPO similar to that of non‐deforming garnet, despite the strong shape preferred orientation (SPO) observed. {110} [001] slip may dominate the deformation of rutile. Quartz displays complicated and inconsistent LPOs in eclogite. These results are remarkably similar to observations from deformed eclogites in nature.     

Late Miocene–Pliocene eclogite facies metamorphism, D'Entrecasteaux Islands, SE Papua New Guinea

The D'Entrecasteaux Islands of south‐eastern Papua New Guinea are active metamorphic core complexes that formed within a region where the plate tectonic regime has transitioned from subduction to rifting. While rapid, post 4 Myr exhumation and cooling of amphibolite and greenschist facies rocks that constitute the footwall of the crustal scale detachment fault system have been previously documented on Fergusson and Goodenough Islands of the D'Entrecasteaux chain, the timing of eclogite facies metamorphism in rocks of the footwall was unknown. Recent work revealed that at least one of the eclogite bodies formed during the Pliocene. We present combined in situ ion microprobe U–Pb age analyses of zircon from five variably retrogressed eclogite samples from Fergusson and Goodenough Islands that document Late Miocene–Pliocene (8–2 Ma) eclogite formation on these islands. Textural relationships and zircon–garnet rare earth element partition coefficients indicate that U–Pb ages constrain zircon crystallization under eclogite facies conditions in all samples. Results suggest westward younging of eclogite facies metamorphism from Fergusson to Goodenough Island. Present‐day exposure of Late Miocene–Pliocene eclogites requires exhumation rates > 2.5 cm yr^?1.     

对山东高压-超高压变质带的几点看法——程裕淇院士野外考察记

通过对山东高压超高压变质带的考察,初步认为：榴辉岩的最后隆升时代为燕山期;含硬玉石英岩＋榴辉岩＋（透辉石）大理岩组合说明表壳岩经历了高压超高压变质作用;该带晋宁期长英质片麻岩花岗岩广泛出露;在其北部麻粒岩和榴辉岩密切伴生。     

榴辉岩中绿辉石的测定方法研究

通过对某地榴辉岩中伴生的有用矿物的纯矿物物质组成的研究,发现Ｎａ可作为其中绿辉石的特征性成分,且Ｎａ２Ｏ含量与其纯度呈正相关。因此,推荐用测定Ｎａ２Ｏ量并以求得的换算系数计算榴辉岩中绿辉石含量的化学物相分析方法。经合成样品验证,方法的相对误差＜１．７％,用于生产样品分析,所得结果的重现性好,平均偏差＜０．５％。     

Thermal calculation for high-pressure contact metamorphism: application to eclogite formation in the Sebadani area, the Sambagawa belt, SW Japan

Eclogite, a high-pressure–temperature metamorphic rock characterized by garnet + omphacite, is usually considered to be a product of regional metamorphism under a low geothermal gradient. However, in the Sebadani area of the Sambagawa metamorphic belt most petrologists agree that the eclogite formed by localized contact metamorphism due to intrusion of a body in the solid-state (the Sebadani mass). This process is termed ‘high-pressure contact metamorphism'. However, geological considerations suggest that the effect of such a process would be limited, firstly because the speed of emplacement for solid-state material will generally be much lower than that for magma and secondly because in the solid-state there is no heat of fusion in the body available for thermal effects. Thermal modelling of a solid-state intrusion, based on the heat conduction equation, allows the relationship between size of intrusion, velocity of emplacement and thermal effects to be calculated. Two cases have been considered: (1) a hot model, where none of the heat conducted into the surroundings is lost during the rise of the body; and (2) a cold model where all the heat conducted into the surroundings is lost. These models bracket possible thermal histories of the body. Calculations suggest that in the Sebadani region, production of the observed metamorphic features requires unrealistically high velocity and a much larger intruded body than is observed. These conclusions suggest that it is unlikely that eclogite in the Sebadani area was formed by high-pressure contact metamorphism, but rather that it represents the highest-grade part of the regional Sambagawa metamorphism.