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Quantitative Analysis procedure for the analysis of the elemental Composition of materials by the libs technique

机译:使用libs技术分析材料元素组成的定量分析程序

摘要

Quantitative Analysis procedure for the analysis of the elemental Composition of materials by Laser Induced plasma Spectroscopy technique, known as libs,To determine the concentrations of the elements that Compose a set of samples of materials from which can generate a plasma induced by Laser RadiationWhere the procedure includes the following steps: 1.A step of obtaining characteristic parameters of the plasma Radiation which is detected by the system parameters, including the electron Density Nze.Tzj J, the temperature, the product (NL) ZJ total Density n, including Atoms and ions with a load Unit for All elements present in the sample,The length l along the line of sight and the product (u03b2a ZJ area) to cross the line of Sight by the instrumental factor beta SystemDefined as the number of Counts obtained per Watt of accumulated Radiation, being defined parameter values for different values of the indices (J, Z),Taking the index z values Z = 0 for the region Station lines of neutral Atoms and Z = 1 for the region of Ion Channel load Unit, the index J values taking J = 0, 1,...The index J, N = 0 corresponding to a model of plasma model known as homogeneous plasma.Stations in the regions of lines of neutral Atoms and ions are considered homogeneous load unit and corresponding values (J = 1,...N, a model called Model non homogeneous regions, in which stations lines of neutral Atoms and ions with charge unit is divided into a number of areas.Each subindex J considered Uniform, Defining the value of the parameter in each area.And also the limit value for the validity of the model is not homogeneous areas (u03c4lu0394u03bbl) zlim with Z = 0, 1, Product u03c4lu0394u03bbl, where u03c4l is Optical Depth LineDefined by * * * * (see formula) where C is the concentration of the element in the material expressed in Atomic percent (AT.u03c3l%), where is the cross section of line, given by the equation (see * * * * u03bbl formula) where d is the width of the lorentzian LineDetermined by multiplying the Stark width W for the electron Density Nze, 0, where KT is * * * * (see formula) where e is the Elementary charge, u03b50 is the permittivity of Free Space.M is the electron Mass, K is the Boltzmann Constant, u03bb0 is the central Wavelength of the transition, GI Is The degeneration of the lower level.The EK are Energies of the lower and Upper, F is the force of Oscillator, u is the partition function of the emitting species and RI is the factor of IonizationDefined as follows * * (see formula for neutral Atoms) * * * * * * (see formula) for ions with a load unit where S10 is the relation given by the Law of SahaIon density between the load unit and the density of neutral Atoms;
机译:用于通过激光诱导等离子体光谱技术分析材料的元素组成的定量分析程序,即libs,以确定组成一组材料样本的元素的浓度,这些材料样本可以从中产生激光辐射诱导的等离子体包括以下步骤:1.获得由系统参数检测的等离子体辐射特征参数的步骤,该系统参数包括电子密度Nze.Tzj J,温度,乘积(NL)ZJ总密度n,包括原子和样品中所有元素的负载单位为离子,沿视线的长度l和乘以仪器因子beta System乘以视线的乘积( u03b2a ZJ面积)定义为每瓦特获得的计数数的累积辐射量,是针对不同索引值(J,Z)定义的参数值,对于区域ne的站线,取索引z值Z> = 0离子通道负载单位区域的U原子和Z> = 1,索引J值>取J = 0,1,...索引J,N> = 0对应于称为均质等离子体的等离子体模型。中性原子和离子线区域中的测站被认为是均质载荷单位和相应的值(J = 1,... N,称为模型非均质区域的模型,其中中性原子和离子线具有电荷单位)分为多个区域,每个子索引J都视为均匀,定义每个区域中的参数值,并且模型有效性的极限值也不是Z均等的区域( u03c4l u0394 u03bbl) > = 0,1,产品 u03c4l u0394 u03bbl,其中 u03c4l是光学深度线,由* * * *定义(请参见公式),其中C是材料中元素的浓度,以原子百分比(AT。)表示。 %),其中线的横截面由公式给出(请参见* * * * u03bbl公式),其中d是t的宽度洛伦兹线是通过将电子密度Nze的斯塔克宽度W乘以0来确定的,其中KT为* * * *(参见公式),其中e为基本电荷, u03b50为自由空间的介电常数,M为电子质量, K是玻尔兹曼常数, u03bb0是过渡的中心波长,GI是下级的退化.EK是下层和上层的能量,F是振荡器的力,u是发射的分配函数物种和RI是电离因子定义如下* *(请参见中性原子的公式)* * * * * *(请参见公式)对于具有负载单位的离子,其中S10是由SahaIon密度定律在负载之间给出的关系中性原子的单位和密度;

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