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Is scanning electron microscopy/energy dispersive x-ray spectroscopy (SEM/EDS) quantitative? Effect of specimen shape

机译:扫描电子显微镜/能量色散X射线光谱(SEM / EDS)是否定量?标本形状的影响

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The extraordinary throughput of the silicon drift detector energy dispersive x-ray spectrometer (SDD-EDS) enables collection of EDS spectra with much higher integrated counts within practical time periods, e.g., 100 s or less, compared to past experience with the Si(Li)-EDS. Such high count SDD spectra, containing one million to ten million counts, yield characteristic peak intensities with relative standard deviation below 0.25%, a precision similar to that achieved with wavelength dispersive spectrometry (WDS), the "gold standard" of microprobe analysis, but at lower dose because of the greater solid angle of the SDD-EDS. Such high count SDD-EDS spectra also enable more accurate quantification, nearly indistinguishable from WDS for major and minor constituents when the WDS unknown-to-standard intensity ratio ("k-value") protocol is followed. A critical requirement to satisfy this measurement protocol is that the specimen must be a highly polished bulk target. The geometric character of specimens examined in the scanning electron microscope (SEM) often deviates greatly from the ideal flat bulk target but EDS spectra can still be readily obtained and analyzed. The influence of geometric factors such as local inclination and surface topography on the accuracy of quantitative EDS analysis is examined. Normalized concentration values are subject to very large errors, as high as a factor of 10, as a result of deviation of the specimen geometry from the ideal flat bulk target.
机译:硅漂移检测器能量色散X射线能谱仪(SDD-EDS)的超高通量使EDS光谱的收集能够在实际时间段内(例如100 s或更短)内与过去使用Si(Li )-EDS。如此高计数的SDD光谱,包含一百万至一千万个计数,可产生特征峰强度,相对标准偏差低于0.25%,其精度与微探针分析的“金标准”波长色散法(WDS)相似,但是由于SDD-EDS的立体角更大,因此剂量较低。当遵循WDS未知标准强度比(“ k值”)协议时,此类高计数SDD-EDS光谱还可以实现更准确的定量,几乎与WDS的主要成分和次要成分没有区别。满足此测量协议的关键要求是样品必须是高度抛光的大块目标。在扫描电子显微镜(SEM)中检查的样品的几何特征通常与理想的平坦大块靶物有很大的偏差,但EDS光谱仍然可以轻松获得和分析。研究了几何因素(例如局部倾斜度和表面形貌)对EDS定量分析准确性的影响。归一化的浓度值会由于样品几何形状与理想的平整目标之间的偏差而导致非常大的误差,误差高达10倍。

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