首页> 外文期刊>Spectrochimica Acta, Part B. Atomic Spectroscopy >Matrix and energy effects during in-situ determination of Cu isotope ratios by ultraviolet-femtosecond laser ablation multicollector inductively coupled plasma mass spectrometry
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Matrix and energy effects during in-situ determination of Cu isotope ratios by ultraviolet-femtosecond laser ablation multicollector inductively coupled plasma mass spectrometry

机译:飞秒激光烧蚀多收集器电感耦合等离子体质谱法原位测定Cu同位素比时的基体和能量效应

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Copper isotope compositions in Cu-bearing metals and minerals have been measured by deep (194 nm) ultraviolet femtosecond laser ablation multi-collector inductively coupled plasma mass spectrometry (UV-fsLA-MC-ICP-MS). Pure Cu-metal, brass, and several Cu-rich minerals (chalcopyrite, enargite, covellite, malachite and cuprite) have been investigated. A long-term reproducibility of better than 0.08 parts per thousand at the 95% confidence limit on the NIST SRM 976 (National Institute of Standards and Technology) Cu-metal standard has been achieved with this technique. The delta Cu-65 values for all samples have been calculated by standard-sample-standard bracketing with HIST SRM 976. All analyses have been carried out using Ni as a mass discrimination monitor added by nebulization prior to entering the plasma torch. For further verification samples have been analysed by conventional solution nebulization MC-ICP-MS and the results obtained have been compared with those from UV-fsLA-MC-ICP-MS. Several potential matrix-induced molecular interferences on the mineral copper isotope ratio, such as ((SS)-S-32-S-33)(+) and (S-32-(OO)-O-16-O-17)(+) do not affect the Cu isotope measurements on sulfides, while hydrides, such as Zn-H or doubly-charged Sn2+ that interfere Ni isotopes can be either neglected or stripped by calculation. Matrix independent Cu-isotope measurements are sensitive to the energy density (fluence) applied onto the sample and can produce artificial shifts in the obtained delta Cu-65 values which are on the order of 3 parts per thousand for Cu-metal, 0.5 parts per thousand for brass and 0.3 parts per thousand for malachite when using energy density of up to 2 J/cm(2) for ablation. A positive correlation between applied energy density and the magnitude of the isotope ratio shift has been found in the energy density range from 0.2 to 1.3 J/cm(2) which is below the ablation threshold for ns-laser ablation. The results demonstrate that by using appropriate low fluence it is possible to measure Cu isotopic ratios in native copper and Cu-bearing sulfides, carbonates and oxides in situ with a precision of better than 0.1 parts per thousand (2SD) without using a matrix-matched standard during laser ablation analyses. Thus, this is a suitable tool to resolve Cu isotopic zoning larger than 0.1 parts per thousand in Cu-sulfides, carbonates and oxides. (C) 2015 Elsevier B.V. All rights reserved.
机译:含铜金属和矿物中的铜同位素组成已通过深(194 nm)紫外飞秒激光烧蚀多收集器电感耦合等离子体质谱仪(UV-fsLA-MC-ICP-MS)进行了测量。已研究了纯铜金属,黄铜和几种富含铜的矿物(黄铜矿,钠辉石,陨石,孔雀石和铜矿)。通过此技术,在NIST SRM 976(美国国家标准技术研究院)的铜金属标准品的95%置信度极限下,其长期再现性优于千分之0.08。所有样品的Cu-65δ值均已通过HIST SRM 976的标准样品-标准括号计算得出。所有分析都是在进入等离子炬之前使用雾化添加的Ni作为质量鉴别监测仪进行的。为了进一步验证,已通过常规溶液雾化MC-ICP-MS分析了样品,并将获得的结果与UV-fsLA-MC-ICP-MS的结果进行了比较。几种潜在的基质诱导的分子干扰对矿物铜同位素比率的影响,例如((SS)-S-32-S-33)(+)和(S-32-(OO)-O-16-O-17) (+)不会影响硫化物中的Cu同位素测量,而可以通过计算忽略或去除干扰Ni同位素的氢化物(例如Zn-H或双电荷Sn2 +)。独立于基质的Cu同位素测量值对施加到样品上的能量密度(注量)敏感,并且可以在获得的Cu-65δ值中产生人为偏移,对于Cu-金属而言,其变化约为千分之三,每千分之0.5当使用高达2 J / cm(2)的能量密度进行消融时,黄铜为1000,孔雀石为0.3千分之几。在能量密度范围为0.2至1.3 J / cm(2)(低于​​ns激光烧蚀的烧蚀阈值)的范围内,发现了施加的能量密度与同位素比率偏移幅度之间的正相关关系。结果表明,通过使用适当的低注量,可以在不使用基质匹配的情况下,以高于0.1的千分之几(2SD)的精度就地测量天然铜和含铜硫化物,碳酸盐和氧化物中的铜同位素比。激光烧蚀分析中的标准。因此,这是解决铜硫化物,碳酸盐和氧化物中大于0.1千分之一的Cu同位素分区的合适工具。 (C)2015 Elsevier B.V.保留所有权利。

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