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Topochemical speciation of intercalated palladium in graphite by valence band X-ray spectrometry in the electron microprobe

机译:电子探针中价带X射线光谱法测定石墨中插层钯的拓扑化学形态

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The binding state of palladium was studied within the frame of an investigation on the mechanism of analyte fixation during the pyrolysis step in graphite furnace atomic spectrometry. One approach was the determination of the palladium intercalated in the pyrolytic coating of the graphite tube. Due to the low concentrations of intercalated palladium in the pyrolytic coating, precise determination of the shift of certain X-ray lines was chosen. From several investigated valence state sensitive X-ray transitions, the Pd Lbeta(2/15) (L-3-N-4,N-5) line shift was the one best determinable. The measured fine shifts are in the range of -0.14 to 0.71 eV at line widths of 13 eV (fwhm) and a line energy of 3.1729 keV. These very small line shifts were determined by electron probe microanalysis. The detection of the small line shifts was performed with a new method-by evaluation of the change of the intensity in the Ranks of the X-ray line. The measurements yielded the following results: inside the pyrolytic graphite, the palladium is distributed inhomogeneously in the form of clusters or islands and in the form of particles on the surface of the pyrolytic graphite. The differentiation between particles and clusters is a very practical one: as long as a particle can be seen in the SEM we talk of particles. Often, however, I'd is detected in an area on the tube or platform surface without detection of a particle. Hence, it can be assumed that the Pd is present in the form of clusters which might even be intercalated in the uppermost graphite layers. The valence state inside these clusters does not appear to be uniform. It can be interpreted as a mixture of I'd with PdO in the center of the clusters or particles (positive peak shift) and of Pd bound to the graphite (strong negative peak shift). On the basis of these observations, a way is proposed to determine how activated Pd atoms in intercalated Pd domains are forming strong covalent bonds to analytes. These bonds are responsible for the analyte fixation of even very volatile analytes. [References: 63]
机译:在研究石墨炉原子光谱法的热解步骤中分析物固定机理的框架内,研究了钯的结合状态。一种方法是测定插在石墨管热解涂层中的钯。由于热解涂层中插层钯的浓度较低,因此选择了精确确定某些X射线线偏移的方法。从几个调查的价态敏感X射线跃迁,Pd Lbeta(2/15)(L-3-N-4,N-5)线位移是最好的确定方法。在13 eV(fwhm)的线宽和3.1729 keV的线能量下,测得的精细位移在-0.14至0.71 eV的范围内。这些非常小的线位移通过电子探针显微分析确定。通过评估X射线线等级中强度的变化,通过一种新方法进行小线位移的检测。测量得到以下结果:在热解石墨内部,钯以团簇或岛的形式以及以颗粒形式在热解石墨的表面上不均匀地分布。粒子和团簇之间的区分是非常实用的区分:只要可以在SEM中看到粒子,我们就谈论粒子。但是,通常会在管子或平台表面的某个区域中检测到I而没有检测到颗粒。因此,可以假定Pd以簇的形式存在,甚至可以插在最上层的石墨层中。这些簇内的价态似乎不统一。它可以解释为Id和PdO在团簇或颗粒中心(正峰位移)和与石墨结合的Pd(强负峰位移)的混合物。基于这些观察结果,提出了一种方法来确定嵌入的Pd域中的活化Pd原子如何与分析物形成强共价键。这些键甚至负责挥发性非常高的分析物的分析物固定。 [参考:63]

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