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宽带非选择性激发钚同位素用于共振电离质谱同位素比测量:理论研究。

Broadband non-selective excitation of plutonium isotopes for isotope ratio measurements in resonance ionization mass spectrometry: a theoretical study.

机构信息

National Centre for Compositional Characterisation of Materials, Bhabha Atomic Research Centre, Hyderabad 500 062, India.

出版信息

Rapid Commun Mass Spectrom. 2012 Oct 15;26(19):2231-40. doi: 10.1002/rcm.6342.

Abstract

RATIONALE

Making isotope ratio measurements with minimum isotope bias has always been a challenging task to mass spectrometrists, especially for the specific case of plutonium, owing to the strategic importance of the element. In order to use resonance ionization mass spectrometry (RIMS) as a tool for isotope ratio measurements, optimization of the various laser parameters and other atomic and system parameters is critical to minimize isotopic biases.

METHODS

Broadband simultaneous non-selective excitation of the isotopes of plutonium in the triple resonance excitation scheme with λ(1) = 420.77 nm, λ(2) = 847.28 nm, and λ(3) = 767.53 nm based on density matrix formalism has been theoretically computed for the determination of isotope ratios. The effects of the various laser parameters and other factors such as the atomization temperature and the dimensions of the atomic beam on the estimation of isotope ratios were studied. The effects of Doppler broadening, and time-dependent excitation parameters such as Rabi frequencies, ionization rate and the effect of non-Lorenztian lineshape have all been incorporated.

RESULTS

The average laser powers and bandwidths for the three-excitation steps were evaluated for non-selective excitation. The laser intensity required to saturate the three-excitation steps were studied. The two-dimensional lineshape contour and its features were investigated, while the reversal of peak asymmetry of two-step and two-photon excitation peaks under these conditions is discussed. Optimized powers for the non-selective ionization of the three transitions were calculated as 545 mW, 150 mW and 545 mW and the laser bandwidth for all the three steps was ~20 GHz.

CONCLUSIONS

The isotopic bias between the resonant and off-resonant isotope under the optimized conditions was no more than 9%, which is better than an earlier reported value. These optimized laser power and bandwidth conditions are better than in the earlier experimental work since these comprehensive calculations yield simultaneous and much more accurate isotope ratios than those in the sequential and less accurate determination reported earlier. Application of these theoretical calculations to minimize the isotopic biases under these conditions for the rapid, efficient and accurate isotope ratio measurements using RIMS has been outlined.

摘要

原理

对于质谱仪专家来说,使同位素比测量的同位素偏差最小化一直是一项具有挑战性的任务,特别是对于钚这种具有战略重要性的元素。为了将共振电离质谱(RIMS)用作同位素比测量的工具,优化各种激光参数以及其他原子和系统参数对于最小化同位素偏差至关重要。

方法

基于密度矩阵理论,对三重共振激发方案中钚同位素的宽带同时非选择性激发进行了理论计算,激发波长为 λ(1) = 420.77nm、λ(2) = 847.28nm 和 λ(3) = 767.53nm,用于确定同位素比。研究了各种激光参数和其他因素(例如原子化温度和原子束的尺寸)对同位素比估计的影响。考虑了多普勒展宽以及时间相关的激发参数(例如拉比频率、电离率和非洛伦兹线型的影响)的影响。

结果

评估了用于非选择性激发的三步激发的平均激光功率和带宽。研究了饱和三步激发所需的激光强度。研究了二维线型轮廓及其特征,同时讨论了在这些条件下两步和双光子激发峰的峰不对称性反转。计算了三条跃迁非选择性电离的优化功率为 545mW、150mW 和 545mW,所有三个步骤的激光带宽约为 20GHz。

结论

在优化条件下,共振和非共振同位素之间的同位素偏差不超过 9%,优于先前报道的值。这些优化的激光功率和带宽条件优于早期的实验工作,因为这些综合计算比早期报道的顺序和不太准确的测定结果提供了更准确的同时同位素比值。概述了应用这些理论计算在这些条件下最小化同位素偏差,以便使用 RIMS 进行快速、高效和准确的同位素比测量。

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