首页> 外文期刊>Journal of Analytical Atomic Spectrometry >Precise isotope analysis of sub-nanogram lead by total evaporation thermal ionization mass spectrometry (TE-TIMS) coupled with a ~(204)Pb-~(207)Pb double spike method
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Precise isotope analysis of sub-nanogram lead by total evaporation thermal ionization mass spectrometry (TE-TIMS) coupled with a ~(204)Pb-~(207)Pb double spike method

机译:全蒸发热电离质谱(TE-TIMS)结合〜(204)Pb-〜(207)Pb双峰方法对亚纳米铅进行精确同位素分析

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摘要

We present a new analytical technique for precise isotope measurement of sub-nanograms of Pb by total evaporation thermal ionization mass spectrometry (TE-TIMS) coupled with a ~(204)Pb-~(207)Pb double spike. The precise determination of Pb isotopic composition with a small (sub-nanograms) quantity of Pb is hampered due to the low signal intensity of ~(204)Pb+, which has the lowest isotope abundance in natural samples (1.4%). The advantage of TE-TIMS is that the measured signal intensities are larger and the measurement time is shorter than those by the measurement with constant filament current. In this study, we investigated optimization of the analytical protocol for Pb isotope measurement by TE-TIMS coupled with a ~(204)Pb-~(207)Pb double spike, including the sample loading technique, filament temperature control, and the reduction method of isotope data acquired. The Pb isotope analysis was performed with the heating rate of 18, 90, and 450 mA min~(-1), with a short measurement time of 60, 30, and 20 minutes. The resulting reproducibilities of Pb isotope ratios were comparable to those of previous techniques including the ~(202)Pb-~(205)Pb double spike method and the ~(204)Pb-~(207)Pb double spike method using an amplifier with a state-of-the-art 10~(13) C2 resistor for collecting the ~(204)Pb signal. The absolute Pb isotope ratios for NIST 981 measured by our method were biased due to anomalous ~(207)Pb behavior occurring at the filament temperature of >1250 °C as well as the deterioration of Faraday cups. However, we confirmed that the accurate absolute Pb isotope ratios for an unknown sample can be obtained by normalizing the observed Pb isotope ratios to those of NIST 981 that are determined in the same analytical period and then multiplying the reference Pb isotope ratios of NIST 981. We measured the Pb isotope ratios of a standard rock material JB-3, of which the results were consistent with those reported by previous studies. We conclude that our method is suitable especially for the isotope analysis of sub-nanograms of Pb, and using a ~(204)Pb-~(207)Pb double spike instead of a ~(202)Pb-~(205)Pb double spike is beneficial for a number of laboratories due to the availability of the spikes. Furthermore, reduced measurement time compared to previous studies is helpful for measuring a large quantity of samples.
机译:我们提出了一种新的分析技术,该技术可以通过全蒸发热电离质谱(TE-TIMS)结合〜(204)Pb-〜(207)Pb双尖峰精确地测量亚纳米级的Pb同位素。由于〜(204)Pb +的信号强度低,因此同位素的丰度在自然样品中最低(1.4%),因此以少量(亚纳克级)的Pb精确测定Pb同位素组成受到阻碍。 TE-TIMS的优势在于,与通过恒定灯丝电流进行测量相比,所测量的信号强度更大,测量时间更短。在这项研究中,我们研究了TE-TIMS结合〜(204)Pb-〜(207)Pb双尖峰对铅同位素分析方法的优化,包括样品加载技术,灯丝温度控制和还原方法采集的同位素数据。在18、90和450 mA min〜(-1)的加热速率下进行Pb同位素分析,测量时间较短,分别为60、30和20分钟。铅同位素比的重现性与包括〜(202)Pb-〜(205)Pb双尖峰法和〜(204)Pb-〜(207)Pb双尖峰法在内的使用放大器的现有技术相当。最新的10〜(13)C2电阻器,用于收集〜(204)Pb信号。通过我们的方法测量的NIST 981的绝对Pb同位素比率由于在> 1250°C的灯丝温度下发生的异常〜(207)Pb行为以及法拉第杯的变质而产生偏差。但是,我们确认可以通过将观察到的Pb同位素比值标准化为在相同分析期内确定的NIST 981值,然后再乘以NIST 981的参考Pb同位素比值,来获得未知样品的准确绝对Pb同位素比值。我们测量了标准岩石材料JB-3的Pb同位素比,其结果与先前研究报道的结果一致。我们得出的结论是,我们的方法特别适合于亚铅纳米级同位素的同位素分析,并且使用〜(204)Pb-〜(207)Pb双峰代替〜(202)Pb-〜(205)Pb双峰由于尖峰的可用性,尖峰对于许多实验室都是有益的。此外,与以前的研究相比,减少测量时间有助于测量大量样品。

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  • 来源
    《Journal of Analytical Atomic Spectrometry》 |2017年第4期|848-857|共10页
  • 作者单位

    Japan Agency for Marine-Earth Science and Technology, 2-15 Natsushima-cho, Yokosuka, 237-0061, Japan;

    Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama, Tokyo 152-8851, Japan;

    Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama, Tokyo 152-8851, Japan;

    Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama, Tokyo 152-8851, Japan, Earth-Life Science Institute, Tokyo Institute of Technology, Ookayama, Tokyo 152-8850, Japan;

    Department of Earth and Planetary Sciences, Tokyo Institute of Technology, Ookayama, Tokyo 152-8851, Japan;

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