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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research >Carbon background and ionization yield of an AMS system during ~(14)C measurements of microgram-size graphite samples
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Carbon background and ionization yield of an AMS system during ~(14)C measurements of microgram-size graphite samples

机译:微克大小的石墨样品〜(14)C测量期间AMS系统的碳背景和电离产率

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For ~(14)C AMS measurements of samples at the microgram level, ion source related effects start to play a role, while generally the lower sample size limit is set by the carbon background introduced during chemical preparation procedures. Measurements of about 800 graphite targets in the mass range of 1-100 μg were performed within 25 AMS beam-times during the last three years at VERA, revealing a dependency of measured ~(14)C~(3+)/~(12)C~(3+) ratios on ~(12)C~(3+) currents. This dependency can be accounted for by assuming a background current, which was determined for each AMS measurement by least square fitting. ~(12)C ion currents extracted from microgram graphite samples were typically (1.0 ± 0.5) μA / μg C. On average a ~(12)C~(3+) background current of (0.14 ± 0.14) μA with F~(14)C = 0.22 ± 0.46 (skewness γ_1 = 3.0) was deduced with significant variations between single measurements. The determination of this background current for each AMS measurement of microgram graphite samples allowed to apply a quantitative correction and thereby to improve the AMS measurement precision. Furthermore, the yield of graphitization and ionization in a Cs sputter ion source of graphitized microgram CO_2 samples was investigated. No dependency on the cathode target geometry was observed for 9 differently shaped cathode types.
机译:对于微克级样品的〜(14)C AMS测量,离子源相关效应开始起作用,而通常,样品下限的下限由化学制备过程中引入的碳背景设定。在过去三年中,在VERA的25个AMS射线时间内,对质量范围为1-100μg的约800个石墨靶进行了测量,揭示了〜(14)C〜(3 +)/〜(12)的依赖性。 〜(12)C〜(3+)电流上的)C〜(3+)比率。这种依赖性可以通过假设背景电流来解决,该背景电流是通过最小二乘拟合为每个AMS测量确定的。从微克石墨样品中提取的〜(12)C离子电流通常为(1.0±0.5)μA/μgC.平均,在F〜(...下,〜(12)C〜(3+)背景电流为(0.14±0.14)μA。 14)C = 0.22±0.46(偏斜度γ_1= 3.0)被推导,单次测量之间存在显着差异。对于微克石墨样品的每次AMS测量,该背景电流的确定允许进行定量校正,从而提高AMS测量精度。此外,还研究了石墨化微克CO_2样品的Cs溅射离子源中的石墨化和电离产率。对于9种不同形状的阴极类型,未观察到对阴极靶几何形状的依赖性。

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    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

    University of Vienna, Faculty of Physics - Isotope Research, VERA Laboratory, Waehringer Str. 17,A-1090 Vienna, Austria;

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