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1.
The estimation of the peak metamorphic temperature by Raman spectroscopy of carbonaceous material (RSCM) is influenced by several bias sources grouped in measuring conditions, spectral processing and sample heterogeneity. The measuring conditions (selected excitation wavelength) and the operator bias during spectral processing have a pronounced impact on the temperature estimate and thus on the comparability and portability of thermometric data obtained by RSCM. Several calibration lines of RSCM geothermometers are published already, but no standardised approach exists. Samples of carbonaceous material bearing metasediments with well‐established metamorphic conditions of the central and western Alps compile a reference series. By applying an automated, iterative and randomised curve‐fitting approach, a consistent and user input‐independent RSCM geothermometer is presented, which covers peak metamorphic temperatures from ca. 160 to 600 °C. The method is hardware independent because the measuring conditions bias is excluded by the use of the reference series and the automated curve‐fitting approach reduces the spectral processing bias effectively, increasing the method's comparability and portability. By distributing the reference series and the automated curve‐fitting software, a laboratory will be able to derive a laboratory specific calibration line for the RSCM geothermometer.  相似文献   

2.
This contribution attempts to summarize the principles, sample preparation, analytical procedures, influencing factors, and geological applications of Raman Spectroscopy of Carbonaceous Material (RSCM) thermometry. Irreversible graphitization of carbonaceous material in sedimentary rocks occurs during the process of reaching peak metamorphic temperature and can be effectively quantified by Raman spectroscopy. However, in addition to temperature, other factors, such as structural and compositional heterogeneity of carbonaceous materials, structural damage caused by polishing, wavelength and energy of laser used for analyses, hematite content,etc., also have significant influence on the Raman signals of carbonaceous materials. Therefore, fresh samples should be collected for analyses to eliminate the influence of hematite. Further, standard experimental procedure should be practiced to avoid the effects of polishing and laser parameter setups. Additionally, multiple (usually more than 25) analyses per sample should be carried out for deriving statistical average and uncertainty values so as to minimize the influence of sample heterogeneity. RSCM thermometry is applicable to a temperature range between 100~700 ℃, and has been widely used in many fields of geological studies, including metamorphism and deformation of orogens, sediment burial history, fault gouge characteristics and evolution, and maturation grade of carbonaceous materials,etc.  相似文献   

3.
In this study, we detail procedures to synthesise inclusions of fluids of known composition under diagenetic conditions – low temperatures (50–180 °C) and pressures (2–25 MPa) – hosted by quartz. Pre‐existing microcavities in polished quartz chips were used, decrepitated and rinsed before being healed in an autoclave. Each synthesis required around 4 weeks. A range of biphase liquid–vapour inclusions in the H2O–CH4–NaCl system, similar to natural ones, were synthesised in quartz, varying the content of all three components. The quartz chips were checked before and after synthesis by optical microscopy, microthermometry and Raman spectroscopy. The method was used to build a series of calibration curves relating methane‐to‐water count ratios to the methane content of aqueous fluid inclusions. Good correlation was obtained between Raman band area ratios and the expected CH4 solubilities from equations of state. The chosen procedure's main advantages, compared with other published methods, are as follows: quicker healing of the microfractures at lower temperatures, larger inclusions, simple quartz sample preparation, control of fluid inclusion composition and the use of commercial reactors. Such reference material inclusions allow the calibration of Raman microspectrometers with the objective of PTX reconstruction of palaeofluid migration in petroleum reservoirs.  相似文献   

4.
This study combines microstructural observations with Raman spectroscopy on carbonaceous material (RSCM), phase equilibria modelling and U–Pb dating of titanite to delineate the metamorphic history of a well‐exposed section through the South Tibetan Detachment System (STDS) in the Dzakaa Chu valley of Southern Tibet. In the hanging wall of the STDS, undeformed Tibetan Sedimentary Series rocks consistently record peak metamorphic temperatures of ～340 °C. Temperatures increase down‐section, reaching ～650 °C at the base of the shear zone, defining an apparent metamorphic field gradient of ～310 °C km?1 across the entire structure. U–Th–Pb geochronological data indicate that metamorphism and deformation at high temperatures occurred over a protracted period from at least 20 to 13 Ma. Deformation within this 1‐km‐thick zone of distributed top‐down‐to‐the‐northeast ductile shear included a strong component of vertical shortening and was responsible for significant condensing of palaeo‐isotherms along the upper margin of the Greater Himalayan Series (GHS). We interpret the preservation of such a high metamorphic gradient to be the result of a progressive up‐section migration in the locus of deformation within the zone. This segment of the STDS provides a detailed thermal and kinematic record of the exhumation of footwall GHS rocks from beneath the southern margin of the Tibetan plateau.  相似文献   

5.
The degree of graphitization of carbonaceous material (CM) has been widely used as an indicator of metamorphic grade. Previous work has demonstrated that peak metamorphic temperature (T) of regional metamorphic rocks can be estimated by an area ratio (R2) of peaks recognized in Raman spectra of CM. The applicability of this method to low‐pressure (<3 kbar) contact metamorphism was tested using Raman spectroscopic analyses of samples from two contact‐metamorphic aureoles in Japan (Daimonji and Kasuga areas). A suitable measurement procedure allows the dependence of the geothermometer on sample type (thin section, chip) and incident angle of laser beam relative to the c‐axes of CM to be tested. Two important general results are: (i) in addition to standard thin sections, chips are also suitable for spectral analysis; and (ii) the incident angle of the laser beam does not significantly affect the temperature estimation, i.e. spectral measurements for the geothermometer can be carried out irrespective of the crystallographic orientation. A laser wavelength of 532 nm was used in this study compared with 514.5 nm in an independent previous study. A comparison shows that the use of a 532‐nm laser results in a slightly, but systematically larger R2 ratio than that of a 514.5‐nm laser. Taking this effect into account, our results show that there is a slight but distinct difference between the R2–T correlations shown by contact and regional metamorphic rocks: the former are slightly better‐crystallized (have slightly lower R2 values) than the latter at the same temperature. This difference is interpreted as due to the degree of associated deformation. Despite the slight difference, the results of this study coincide within the estimated errors of ±50 °C with those of the previously proposed Raman CM geothermometer, thus demonstrating the applicability of this method to contact metamorphism. To facilitate more precise temperature estimates in regions of contact metamorphism, a new calibration for analyses using a 532‐nm laser is derived. Another important observation is that the R2 ratio of metamorphosed CM in pelitic and psammitic rocks is highly heterogeneous with respect to a single sample. To obtain a reliable temperature estimate, the average R2 value must be determined by using a substantial number of measurements (usually N > 50) that adequately reflects the range of sample heterogeneity. Using this procedure (with 532‐nm laser) and adapting our new calibration, the errors of the Raman CM geothermometer for contact metamorphic rocks decrease to ～±30 °C.  相似文献   

6.
变质沉积岩普遍含有碳质物,其源自沉积母岩中有机质。在变质过程中这些有机质逐渐转变为碳质物或石墨,且碳质物结晶程度可以作为变质等级的可靠指示标志。拉曼光谱是表征碳质物结晶度的有效工具,Beyssac et al.(2002a)基于碳质物拉曼光谱参数(R1=D1/G,D1和G为碳质物拉曼光谱峰强;R2=D1/(G+D1+D2),G、D1和D2为碳质物拉曼光谱峰面积)与寄主岩变质温度之间的线性关系构建了碳质物拉曼光谱温度计:T(℃)=-445(R2)+641,其简单且实用,并被应用到阿尔卑斯和喜马拉雅造山带热结构与折返机制研究中;随后,Rahl et al.(2005)对该变质温度计进行修订,修订后温度估算表达式为:T(℃)=737.3+320.9R1-1067R2-80.638R12,并将变质温度估算范围扩展为100~700℃。本文对碳质物拉曼光谱变质温度计的基本原理、方法、应用条件及其在造山带热结构重建与演化方面的研究进展进行了综述,并对碳质物拉曼光谱温度计与传统温度计估算的变质温度进行了系统的对比分析,结果表明碳质物拉曼光谱温度计代表峰期变质温度,不会受后期退变质影响,当传统温度计结果代表峰期变质温度时,二者计算结果一致。碳质物拉曼光谱温度计已被用于造山带热结构重建、折返过程的热演化,以及高应变带、流体相关热异常等研究。尽管变质过程的压力、变质持续时间、碳质物前体类型等因素对于碳质物拉曼光谱温度计的影响尚待研究,但与传统矿物组合温压计相结合,该方法可以有效评价峰期变质条件和造山多期热演化。  相似文献   

7.
岳季  吕增  崔莹 《地球科学》2020,45(12):4617-4629
西南天山造山带是塔里木板块和伊犁-中天山板块聚合碰撞的产物,经历了长期复杂的演化.伊犁-中天山陆块南缘的变质作用研究对于揭示西南天山的地质演化历史具有重要意义.这一地区变质岩分布广泛,但目前的变质作用研究主要集中于木扎尔特的高级变质岩,位于同一构造带上其他变质岩的演化和分布特点缺少详细的研究,尚不清楚它们是作为高温变质带的一部分还是来自造山带的其他构造单元.针对该问题,在详细的岩相学分析基础上,利用碳质拉曼光谱（Raman spectroscopy of carbonaceous material,RSCM）温度计对木扎尔特东侧的阿克牙孜河下游地区多个剖面开展了变质温度研究.根据结构构造特征将这些岩石分为具有变余沉积结构构造且发生不同程度糜棱岩化的浅变质碎屑岩-碳酸盐岩系列和具有变质结晶结构的片岩-变粒岩系列.RSCM温度计显示前者经历的峰期温度为465~597℃,原岩很可能为卷入造山带的石炭纪地层,抬升过程中局部发生糜棱岩化.后者峰期温度为552~617℃,绿片岩相叠加期间发生C-O-H流体活动,可能属于伊犁-中天山的变质基底那拉提岩群.研究表明,伊犁-中天山南缘的阿克牙孜下游一带的变质岩具有不同的变质演化历史,它们来自不同的构造单元,并不是木扎尔特高温变质带的延续.   相似文献   

8.
The degree of recrystallization of carbonaceous material (CM), as monitored by Raman microspectroscopy, was examined as a function of metamorphic grade in two well‐studied contact aureoles containing carbonaceous pelites: the Nelson aureole, British Columbia and the Ballachulish aureole, Scotland. Here, we use (a) the R2 ratio extracted from the Raman spectrum of CM as a proxy for the degree of graphitization (0.0 in perfect graphite then increasing with structural defects) and (b) the second‐order S1 band (~2,700 cm?1) as a marker for the tridimensional ordering of CM. The Nelson aureole (garnet–staurolite–andalusite–sillimanite–K‐feldspar sequence, ~550–650°C, 3.5–4.0 kbar) was developed in rocks that were unmetamorphosed prior to contact metamorphism, whereas the Ballachulish aureole (cordierite–andalusite–K‐feldspar–sillimanite sequence, ~550–700°C, ~3.0 kbar) was developed in rocks that had been metamorphosed to garnet grade conditions (~7 kbar, ~500°C) c. 45 Ma before contact metamorphism. Thirty‐one samples were examined from Nelson and 29 samples from Ballachulish. At Nelson, the R2 ratio steadily decreases from ~0.25 to 0.0 as the igneous contact is approached, whereas at Ballachulish, the R2 ratio remains largely unchanged from regional values (~0.20–0.25) until less than 100 m from the igneous contact. The second‐order S1 band reveals that carbonaceous material (CM) was transformed to highly “ordered” locally tridimensional graphitic carbon at Ballachulish by regional metamorphism prior to contact metamorphism, whereas CM was still a disordered turbostratic (bidimensional) material before contact metamorphism in the case of Nelson. Pretexturation of CM likely induced sluggish recrystallization of CM and delayed graphitization in the Ballachulish aureole. Temperatures of recrystallization of the CM in the two aureoles were estimated using different published calibrations of the thermometry based on Raman Spectroscopy of Carbonaceous Material (RSCM), with differences among the calibrations being minor. In the Nelson aureole, temperatures are in reasonable agreement with those indicated by the metapelitic phase equilibria (all within 50°C, most within 25°C). In the Ballachulish aureole, the retarded crystallization noted above results in increasing underestimates of temperatures compared to the metapelitic phase equilibria (up to ~75°C too low within 200 m of the igneous contact). Our study calls for careful attention when using RSCM thermometry in complexly polymetamorphosed rocks to assess properly the meaning of the calculated temperature.  相似文献   

9.
Raman spectra of carbonaceous material in metasediments: a new geothermometer   总被引：13，自引：0，他引：13  
Metasedimentary rocks generally contain carbonaceous material (CM) deriving from the evolution of organic matter originally present in the host sedimentary rock. During metamorphic processes, this organic matter is progressively transformed into graphite s.s. and the degree of organisation of CM is known as a reliable indicator of metamorphic grade. In this study, the degree of organisation of CM was systematically characterised by Raman microspectroscopy across several Mesozoic and Cenozoic reference metamorphic belts. This degree of organisation, including within‐sample heterogeneity, was quantified by the relative area of the defect band (R2 ratio). The results from the Schistes Lustrés (Western Alps) and Sanbagawa (Japan) cross‐sections show that (1) even through simple visual inspection, changes in the CM Raman spectrum appear sensitive to variations of metamorphic grade, (2) there is an excellent agreement between the R2 values calculated for the two sections when considering samples with an equivalent metamorphic grade, and (3) the evolution of the R2 ratio with metamorphic grade is controlled by temperature (T). Along the Tinos cross‐section (Greece), which is characterised by a strong gradient of greenschist facies overprint on eclogite facies rocks, the R2 ratio is nearly constant. Consequently, the degree of organisation of CM is not affected by the retrogression and records peak metamorphic conditions. More generally, analysis of 54 samples representative of high‐temperature, low‐pressure to high‐pressure, low‐temperature metamorphic gradients shows that there is a linear correlation between the R2 ratio and the peak temperature [T(°C) = ?445 R2 + 641], whatever the metamorphic gradient and, probably, the organic precursor. The Raman spectrum of CM can therefore be used as a geothermometer of the maximum temperature conditions reached during regional metamorphism. Temperature can be estimated to ± 50 °C in the range 330–650 °C. A few technical indications are given for optimal application.  相似文献   

10.
This study provides a measurement of success rate of Raman spectroscopy for mineral identification, and a direct comparison of powder X‐ray diffraction (PXRD) is provided by applying the same procedure for measuring its success rate against the identical set of samples. Consistent, standardised analytical procedures were applied to a set of fifty‐five minerals, and a success score was assigned to the results of each analytical method for each sample. For each analytical method, an average success rate (on a scale of 0–100) was calculated from these success scores. The success rate measured for powder XRD is 89, while the success rate for Raman spectroscopy came to 77. As the most common analytical challenge in Raman spectroscopy is specimen photoluminescence (PL), an estimate of the impact of technological advances that would eliminate this interference is provided by recalculating the success rate after removing the samples that produced PL interference from consideration. The resulting no‐PL success rate of 90 indicates that the success rate of Raman spectroscopy would be quite comparable to powder XRD if PL interference could be removed from Raman spectra.  相似文献   

11.
Raman microspectroscopy on carbonaceous material (RSCM) from the eastern Tauern Window indicates contrasting peak‐temperature patterns in three different fabric domains, each of which underwent a poly‐metamorphic orogenic evolution: Domain 1 in the northeastern Tauern Window preserves oceanic units (Glockner Nappe System, Matrei Zone) that attained peak temperatures (Tp) of 350–480 °C following Late Cretaceous to Palaeogene nappe stacking in an accretionary wedge. Domain 2 in the central Tauern Window experienced Tp of 500–535 °C that was attained either within an exhumed Palaeogene subduction channel or during Oligocene Barrovian‐type thermal overprinting within the Alpine collisional orogen. Domain 3 in the Eastern Tauern Subdome has a peak‐temperature pattern that resulted from Eo‐Oligocene nappe stacking of continental units derived from the distal European margin. This pattern acquired its presently concentric pattern in Miocene time due to post‐nappe doming and extensional shearing along the Katschberg Shear Zone System (KSZS). Tp values in the largest (Hochalm) dome range from 612 °C in its core to 440 °C at its rim. The maximum peak‐temperature gradient (≤70 °C km?1) occurs along the eastern margin of this dome where mylonitic shearing of the Katschberg Normal Fault (KNF) significantly thinned the Subpenninic‐ and Penninic nappe pile, including the pre‐existing peak‐temperature gradient.  相似文献   

12.
The aim of this study was to improve the quality of laser ablation inductively coupled plasma‐mass spectrometry (LA‐ICP‐MS) determination of phosphorus in crystalline quartz. Over the last decade, the Geological Survey of Norway has routinely performed trace element determinations on quartz from both operating and potential quartz deposits by LA‐ICP‐MS. The determined phosphorus concentrations were, with but few exceptions, consistently within the range of 10 to 30 μg g?1, results that seemed to be both too high and too consistent. The multi‐material calibration curve obtained from a suite of reference materials (NIST SRM 610, 612, 614, 1830, BAM No. 1 amorphous SiO2 glass) did not define a precise regression line. Published phosphorus concentrations for the reference materials are poorly constrained and the observed dispersions along the multi‐material calibration curve suggest that some of the reference values may be inaccurate. Furthermore, the calibration curve did not pass through the origin of the [(cps 31P/cps 30Si) · cone. Si] vs. P concentration diagram; thus, in addition to the uncertainties of the literature values of phosphorus, it is difficult to define the calibration curve. Three reference materials (NIST SRM 614, 1830, synthetic quartz KORTH) were sent for phosphorus accelerator implantation, providing an independent and accurate (± 3%) approach for determining phosphorus concentrations in crystalline quartz. The intrinsic phosphorus concentrations of the three implanted samples plus those for NIST SRM 610 and 612 were determined by secondary ion mass spectrometry (SIMS), yielding new phosphorus values for NIST SRM 610, 612, 614 and 1830. Using these new values resulted in a better defined LA‐ICP‐MS calibration curve. However, the source of the ICP‐MS related background could not be defined, such that it must still be empirically corrected for.  相似文献   

13.
We report on an improved method for determining trace element abundances in seawater and other natural waters. The analytical procedure involves co‐precipitation on iron hydroxides after addition of a Tm spike, and measurement by inductively coupled plasma‐sector field mass spectrometry (ICP‐SFMS). The validity of the method was assessed through a series of co‐precipitation experiments, using ultra‐diluted solutions of a certified rock reference material (BIR‐1). Results obtained for four natural water reference materials (NASS‐5, CASS‐4, SLEW‐3, SLRS‐4) are in agreement with published working values for rare earth elements, yttrium, vanadium and, when available, for hafnium, zirconium, thorium and scandium. A set of proposed values with uncertainties typically better than 8% RSD is proposed for Hf, Zr and Th.  相似文献   

14.
东西走向的北喜马拉雅片麻岩穹隆带位于喜马拉雅造山带核心,记录了造山演化和青藏高原隆升的变质与变形信息。对穹隆构造热结构及其变形历史的重建有助于揭示喜马拉雅造山过程。本次研究选取然巴片麻岩穹隆的各类构造岩开展微观构造解析、碳物质拉曼光谱温度估算(RSCM)和石英组构学(CPO)分析,对比该穹隆各构造层变质和变形温度及其变化。研究结果揭示然巴穹隆被上、下两条环形拆离断层分为三个构造层:下拆离断层以下为下构造层,其由核部淡色花岗岩和片麻岩组成;下拆离断层和上拆离断层之间为中构造层,由强烈韧性变形的低-中级变质的片岩和少量片麻岩组成;上拆离断层以上为上构造层,由板岩、千枚岩和少量片岩组成。碳物质拉曼光谱变质温度计估算结果显示下构造层和中构造层峰期变质温度为550~600℃,上构造层峰期变质温度400~550℃。各构造层韧性变形岩石内石英组构(CPOs)特征揭示:下构造层石英以柱面滑移为主,韧性剪切变形温度超过600℃;而从中构造层底部向上构造层,石英滑移系由柱面滑移逐渐转变为底面滑移为主,响应的变形温度由550℃逐渐降低为300~350℃。综合分析解释认为然巴穹隆新生代以来经历了四期构造变形,分别对应喜马拉雅造山演化四个阶段:始新世(约45Ma)地壳增厚,发生区域变质作用,变质峰期温度达600℃(如下构造层记录),由下构造层向幔部递减(500℃到300℃);在造山伸展阶段,伴随藏南拆离系北向韧性剪切作用以及晚期南北向裂谷的启动提供的东西向伸展环境导致晚中新世淡色花岗岩底辟就位(约8~7Ma),穹隆幔部岩石遭受接触变质作用改造,接触变质峰期温度为570℃。  相似文献   

15.
使用Renishaw System-1000型激光拉曼光谱仪, 研究了大兴安岭北部上古生界泥质岩石碳质物的拉曼光谱特征及其对形成温度的表征, 探讨了拉曼光谱参数与镜质体反射率(Ro)的关系。研究表明:研究区上古生界泥质岩石碳质物不具有石墨的拉曼光谱谱带吸收峰, 揭示了地层的变质程度未达到低绿片岩相。利用此次经过完善建立的拉曼光谱地质温度计, 对大兴安岭北部上古生界泥质岩石变质温度的估算结果主要为270~320℃, 表明研究区上古生界遭受了极低级变质作用, 变质程度属近变质带。依据碳质物拉曼光谱参数与镜质体反射率的相互关系, 估算研究区有机质成熟度的Ro值主要分布为3.03%~4.23%, 与实测Ro值吻合, 表明有机质演化处于过成熟阶段, 泥质岩石具有生烃的能力, 部分层位可能具有形成油气资源的潜力。  相似文献   

16.
The commonly used, but no longer available, reference materials NIST SRM 976 (Cu) and ‘JMC Lyon’ (Zn) were calibrated against the new reference materials ERM®‐AE633, ERM®‐AE647 (Cu) and IRMM‐3702 (Zn), certified for isotope amount ratios. This cross‐calibration of new with old reference materials provides a continuous and reliable comparability of already published with future Cu and Zn isotope data. The Cu isotope amount ratio of NIST SRM 976 yielded δ65/63Cu values of ?0.01 ± 0.05‰ and ?0.21 ± 0.05‰ relative to ERM®‐AE633 and ERM®‐AE647, respectively, and a δ66/64ZnIRMM‐3702 value of ?0.29 ± 0.05‰ was determined for ‘JMC Lyon’. Furthermore, we separated Cu and Zn from five geological reference materials (BCR‐2, BHVO‐2, BIR‐1, AGV‐1 and G‐2) using a two‐step ion‐exchange chromatographic procedure. Possible isotope fractionation of Cu during chromatographic purification and introduction of resin‐ and/or matrix‐induced interferences were assessed by enriched 65Cu isotope addition. Instrumental mass bias correction for the isotope ratio determinations by MC‐ICP‐MS was performed using calibrator‐sample bracketing with internal Ni doping for Cu and a double spike approach for Zn. Our results for the five geological reference materials were in very good agreement with literature data, confirming the accuracy and applicability of our analytical protocol.  相似文献   

17.
Determination of the peak thermal condition is vital in order to understand tectono-thermal evolution of the Himalayan belt. The Lesser Himalayan Sequence (LHS) in the Western Arunachal Pradesh, being rich in carbonaceous material (CM), facilitates the determination of peak metamorphic temperature based on Raman spectroscopy of carbonaceous material (RSCM). In this study, we have used RSCM method of Beyssac et al. (J Metamorph Geol 20:859–871, 2002a) and Rahl et al. (Earth Planet Sci Lett 240:339–354, 2005) to estimate the thermal history of LHS and Siwalik foreland from the western Arunachal Pradesh. The study indicates that the temperature of 700–800 °C in the Greater Himalayan Sequence (GHS) decreases to 650–700 °C in the main central thrust zone (MCTZ) and decreases further to <200 °C in the Mio-Pliocene sequence of Siwaliks. The work demonstrates greater reliability of Rahl et al.’s (Earth Planet Sci Lett 240:339–354, 2005) RSCM method for temperatures >600 and <340 °C. We show that the higher and lower zones of Bomdila Gneiss (BG) experienced temperature of ~600 °C and exhumed at different stages along the Bomdila Thrust (BT) and Upper Main Boundary Thrust (U.MBT). Pyrolysis analysis of the CM together with the Fission Track ages from upper Siwaliks corroborates the RSCM thermometry estimate of ~240 °C. The results indicate that the Permian sequence north of Lower MBT was deposited at greater depths (>12 km) than the upper Siwalik sediments to its south at depths <8 km before they were exhumed. The 40Ar/39Ar ages suggest that the upper zones of Se La evolved ~13–15 Ma. The middle zone exhumed at ~11 Ma and lower zone close to ~8 Ma indicating erosional unroofing of the MCT sheet. The footwall of MCTZ cooled between 6 and 8 Ma. Analyses of P–T path imply that LHS between MCT and U.MBT zone falls within the kyanite stability field with near isobaric condition. At higher structural level, the temperatures increase gradually with P–T conditions in the sillimanite stability field. The near isothermal (700–800 °C) condition in the GHS, isobaric condition in the MCTZ together with T–t path evidence of GHS that experienced relatively longer duration of near peak temperatures and rapid cooling towards MCTZ, compares the evolution of GHS and inverted metamorphic gradient closely to channel flow predictions.  相似文献   

18.
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19.
Raman spectral analyses of carbonaceous material (CM) extracted from pelitic samples along two sections traversing the metamorphic belt of Taiwan were carried out in the present study. The results show similar spectral variations of CM with metamorphic grade as those documented in the literature. However, continuous sampling from zeolite facies through prehnite–pumpellyite facies to greenschist facies metamorphic rocks in the present study does reveal some interesting features on the Raman spectra of CM that were not noted before. Both the Raman D (disordered-)/O (ordered-) peak area (i.e. integrated intensity) ratio and the D/O peak width (i.e. full width at half maximum, FWHM) ratio of the CM decrease with progressive metamorphism, but the most prominent change in the D/O peak area ratio occurs in samples of lower greenschist facies metamorphic grade, while the most significant decrease in the D/O peak width ratio occurs in samples near the boundary of prehnite–pumpellyite facies and greenschist facies. This phenomenon is interpreted as a result of the decoupling of the changing rates of in-plane crystallite size and degree of defects of CM with progressive metamorphism. It is postulated that the Raman spectrum of CM can serve as a metamorphic grade indicator to distinguish samples of prehnite–pumpellyite facies metamorphic grade from those of greenschist facies metamorphic grade.  相似文献   

20.
硅钼蓝分光光度法测定钛铁矿中二氧化硅不确定度评定   总被引：2，自引：0，他引：2  
蔡玉曼 《岩矿测试》2008,27(2):123-126
对硅钼蓝分光光度法测定钛铁矿中SiO2含量的不确定度进行评估,建立了数学模型,认为测量过程中不确定度主要来源于标准物质、样品制备、曲线拟合,以及重复实验产生的不确定度。当SiO2平均含量为0.67%时,评定其扩展不确定度为0.05%(k=2)。  相似文献   

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