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Method for isotope ratio drift correction by internal amplifier signal synchronization in MC-ICPMS transient signals

机译:MC-ICPMS瞬态信号中通过内部放大器信号同步进行同位素比漂移校正的方法

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摘要

The measurement of isotope ratios by Multi Collection Inductively Coupled Plasma Mass Spectrometry (MC-ICPMS) in transient signals often shows a drift of the isotope signal ratio during signal acquisition. This "isotopic drift" is generally related to the small and distinct time lags between the responses of the amplifiers involved in the Faraday detector configuration. In this work, a method of synchronization of transient isotope signals for a duration of a few tens of seconds is proposed in order to: quantify the time lags between the amplifiers using the ratios of the raw isotope signals and correct the isotope ratio drifts. The method was successfully tested on lead isotope ratio measurements obtained from two different multi-collector mass spectrometers and setups (flow injection with direct injection and gas chromatography). This approach offered a precise determination of the time lag between the different amplifier systems and an effective correction of the isotope ratio drift. The performances of the methods traditionally used for isotope ratio calculation of transient signals were also compared before and after isotope ratio drift correction.
机译:通过多集合电感耦合等离子体质谱法(MC-ICPMS)对瞬态信号中的同位素比率进行测量,通常会在信号采集期间显示出同位素信号比率的漂移。这种“同位素漂移”通常与法拉第探测器配置所涉及的放大器的响应之间的微小且明显的时滞有关。在这项工作中,提出了一种在几十秒的持续时间内使瞬态同位素信号同步的方法,以便:使用原始同位素信号的比率来量化放大器之间的时滞,并校正同位素比率的漂移。该方法已成功通过两种不同的多收集器质谱仪和装置(采用直接进样的流动注射和气相色谱法)获得的铅同位素比测量结果进行了测试。这种方法可精确确定不同放大器系统之间的时间间隔,并有效校正同位素比漂移。在同位素比漂移校正之前和之后,还比较了传统上用于瞬态信号同位素比计算的方法的性能。

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  • 来源
    《Journal of Analytical Atomic Spectrometry》 |2014年第9期|1607-1617|共11页
  • 作者单位

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Universite de Pau et des Pays de l'Adour, Laboratoire de Chimie Analytique Bio-Inorganique et Environnement/ IPREM UMR 5254, Helioparc Pau Pyrenees 2 Avenue du President Angot, 64053 Pau, Cedex 9, France;

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Commissariat a l'Energie Atomique (CEA), DEN/DPC/SEARS/LANIE, 91191 Gif-sur-Yvette Cedex, France;

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Commissariat a l'Energie Atomique (CEA), DEN/DPC/SEARS/LANIE, 91191 Gif-sur-Yvette Cedex, France;

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Institut de Physique du Globe de Paris, Sorbonne Paris Cite, Universite Paris-Diderot, UMR CNRS 7154, 1 rue Jussieu, 75238 Paris Cedex, France;

    Universite de Pau et des Pays de l'Adour, Laboratoire de Chimie Analytique Bio-Inorganique et Environnement/ IPREM UMR 5254, Helioparc Pau Pyrenees 2 Avenue du President Angot, 64053 Pau, Cedex 9, France;

    Commissariat a l'Energie Atomique (CEA), DEN/DPC, 91191 Gif-sur-Yvette Cedex, France;

    Universite de Pau et des Pays de l'Adour, Laboratoire de Chimie Analytique Bio-Inorganique et Environnement/ IPREM UMR 5254, Helioparc Pau Pyrenees 2 Avenue du President Angot, 64053 Pau, Cedex 9, France;

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