共查询到18条相似文献,搜索用时 171 毫秒
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采用一组熔融片样品研究了由不同的X光管激发电位和不同的X光管靶材(Cr靶和Rh靶)所导致的入射X射线能量及强度分布变化对3种散射效应增强荧光强度的影响规律。研究的散射增强包括相干散射激发的荧光强度、非相干散射激发的荧光强度以及其他方向的一次荧光被散射进探测方向的强度。研究结果表明,对于采用的熔融片, 相干散射效应和一次荧光被散射进探测器方向增强效应对荧光强度的贡献随X光管激发电位增大而减小,用Cr靶原级谱激发比用Rh靶原级谱激发贡献大;而非相干散射效应对荧光强度的贡献则随X光管激发电位增大而增大,用Rh靶原级谱激发比用Cr靶原级谱激发贡献大;3种散射效应对荧光强度的总贡献随X光管激发电位增大而增大,在Rh靶原级谱激发条件下比用Cr靶原级谱激发贡献大。 相似文献
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原位能量色散X射线荧光现场分析岩样矿物成分时,岩样基体效应会对测量结果产生影响。本文以Cu元素作为待测元素,研究了17种不同岩样基体对原位能量色散X射线荧光分析Cu元素特征X射线强度的影响及其修正方法。采用蒙特卡罗方法模拟获得了Cu元素含量相同的17种不同岩样测量谱线,综合各类岩石元素构成的相似性,并依据模拟谱线Cu元素Kα射线强度与谱线参数之间的相关性,反映了原位能量色散X射线荧光分析岩样Cu元素的基体效应并不完全受岩体元素构成或岩石分类的控制,需要依据岩石样分析谱线参数的相关性进行归类讨论。针对基体影响Cu元素特征射线强度相似的15种岩样进一步研究,并对Cu元素特征X射线与谱线主要参数的主成分进行分析,发现散射本底、X光管靶材料特征X射线及其非相干散射峰强度能够很好的描述Cu元素特征X射线强度受岩样基体影响的变化,据此可以对基体效应影响相似的岩体进行Cu元素测量结果修正。采用本文方法同样也能为不同岩性岩体其他待测元素基体效应的修正提供参考。 相似文献
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X射线荧光光谱检测多层薄膜样品的增强效应研究 总被引:4,自引:4,他引:0
研究了X射线荧光光谱检测多层薄膜样品的增强效应。根据多层膜中的X荧光强度理论计算公式编写了计算机程序,并计算了Zn/Fe和Fe/Zn双层膜样品中不同薄膜厚度时Fe Kα的一次荧光强度、二次荧光强度、二次荧光与一次荧光强度比以及二次荧光在总荧光强度中比例。研究发现,在多层膜样品的X射线荧光分析中,激发条件不变的情况下,元素谱线的一次荧光相对强度、二次荧光相对强度和二次荧光在总荧光强度中所占比例都随薄膜厚度及位置的变化而变化。当Fe和Zn层厚度相同时,随厚度的变化,对于Fe/Zn样品,Fe Kα二次荧光强度占总荧光强度最高为9%,而对于Zn/Fe样品这一比例最高可达35%。 相似文献
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近二、三十年来,X射线荧光分析(简称XRF)已成为物质中元素含量分析的基本手段,已广泛应用于物理、化学、生物、医学、法学、地学、材料科学等学科及工农业生产中.XRF是用X射线激发样品,并检测从样品中发射出的元素之特征X射线强度,分析样品中元素的含量.所谓特征X射线,是指每种元素的原子受激后会发射特定能量的X射线,它们是不连续的,是各自分立的.当原子内壳层中的电子受外来粒子作用而电离后,就会在内壳层留下一个空穴,于是较外层的电子就会跃迁到这个空穴,这就是所谓的退激发过程. 相似文献
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土壤重金属铅元素的X射线荧光光谱测量分析 总被引:3,自引:0,他引:3
在实验室条件下,利用NITON XLt793型便携式X射线荧光光谱重金属分析仪测量并分析土壤中铅元素的X射线荧光光谱特性。分别以铅的Lα(10.55 keV)和Lβ(12.61 keV)特征谱线作为分析线,分析了不同基体元素对分析线的影响;测定在不同铅浓度下的特征谱线强度变化。结果表明铅的质量分数在10×10-6~1 800×10-6范围内,元素的光谱强度与浓度之间呈现较好的线性关系;建立了铅元素的定标曲线,并计算得到铅的检出限为7.89×10-6。 相似文献
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Hydrogen adsorption on Pt(6)H(n) clusters leads to striking changes in the Pt L(2,3) x-ray absorption spectra. These effects are interpreted using a self-consistent real space Green's function approach. Calculations show that they are due largely to changes in the atomic background contribution to x-ray absorption (i.e., atomic x-ray absorption fine structure) and to reduced Pt-Pt scattering at the edge, while Pt-H multiple scattering is relatively weak. The origin of both effects is traced to the change in the local Pt potential due to Pt-H bonding. 相似文献
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Elongated microvoids, internal fibrillar structure, and edge scattering from both surface refraction cause an equatorial streak in small angle X-ray scattering. A model for analyzing the edge scattering of fibers is proposed. Simulation results indicate that the intensity of edge scattering from surface refraction of a cylindrical fiber is strong and makes an important contribution to the equatorial streak. Two factors influence edge scattering intensity. One is the sample-to-detector distance (D); edge scattering intensity increases with increasing D. The equatorial streak becomes weak when D is shortened. The other factor is the refraction index. Edge scattering intensity increases as the real component of the refraction index decreases. In experiment, weak or even no equatorial streaks were found for samples measured in a roughly index-matching fluid. Edge scattering can be eliminated or weakened, and it can be calculated by comparing the intensities of a cylindrical fiber when it is measured in air and in index-matching fluid. The simulation data are basically in agreement with the experimental data. 相似文献
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Sulfur K‐edge XANES (X‐ray absorption near‐edge structure) spectroscopy is an excellent tool for determining the speciation of sulfur compounds in complex matrices. This paper presents a method to quantitatively determine the kinds of sulfur species in natural samples using internally calibrated reference spectra of model compounds. Owing to significant self‐absorption of formed fluorescence radiation in the sample itself the fluorescence signal displays a non‐linear correlation with the sulfur content over a wide concentration range. Self‐absorption is also a problem at low total absorption of the sample when the sulfur compounds are present as particles. The post‐edge intensity patterns of the sulfur K‐edge XANES spectra vary with the type of sulfur compound, with reducing sulfur compounds often having a higher post‐edge intensity than the oxidized forms. In dilute solutions (less than 0.3–0.5%) it is possible to use sulfur K‐edge XANES reference data for quantitative analysis of the contribution from different species. The results show that it is essential to use an internal calibration system when performing quantitative XANES analysis. Preparation of unknown samples must take both the total absorption and possible presence of self‐absorbing particles into consideration. 相似文献
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On the basis of the multiple scattering approach in combination with the spin-polarized self-consistent potential calculation, an interpretation is proposed for the spin-polarized x-ray absorption spectra near the Mn K edge in MnP. The effect of the core vacancy potential on the spectra is analyzed and found to be insignificant. The method used for the calculations allowed the separation of the effect of the dipole transition matrix element on the spectra and the effect of the density of unoccupied electron states. It is shown that the transition matrix element causes an intensity redistribution only near the absorption jump, while the difference in the densities of states is most pronounced in the energy region 35–55 eV away from the main edge and leads to a shift in energy for the spectra corresponding to the two spin directions. The effect of the spin-dependent broadening caused by the dependence of the mean free path (as a function of energy) on the photoelectron spin is studied. It is shown that this factor considerably affects only the intensities of the peaks in the energy region lying within less than 12 eV from the main edge. 相似文献
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《X射线光谱测定》2003,32(4):312-316
An algorithm based on fundamental parameters and applied to the SEICXRF method, developed by one of the authors, is presented. The methodology used in the calculation is similar to the Rousseau fundamental parameters method, but the main difference is the considerations about the x‐ray secondary fluorescence. In the new experimental method, the fluorescence yield by photons corresponding to the absorption edges with energies greater than the absorption edge energy of analyte does not occur. This secondary fluorescence appears in the calculation of the total fluorescence as a consequence of the integral count of the fluorescent emission from the sample. It is created by the primary fluorescence yield of the atoms whose absorption edge energies are less than the primary fluorescence energy of the analyte. The algorithm also considers the effect of the decrease of the sample fluorescent background just at the jump, originated by the change of the absorption coefficient at the absorption edge energy of the element of interest. Considering these two effects, including the primary fluorescence in the calculation, allows one to obtain the net fluorescence originated by the analyte at its own absorption edge. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
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The photon energy dependence of the normal emission from the Te - 4d levels of an ordered Te c(2 × 2) overlayer on Ni(100) shows two distinct types of structure. The main feature is due to an atomic effect, a delayed onset, a peak followed by a Copper minimum. Superimposed on this atomic profile are intensity modulations of 30 to 40% due to coherent scattering from the substrate. The atomic contribution is in qualitative agreement with theoretical calculations, while the modulations due to solid-state effects are not reproduced by a LEED final state type calculation. 相似文献