https://doi.org/10.1351/goldbook.L03483
For @Q04973@, this should be defined as the minimum distance of two points (areas) on the specimen corresponding to signal levels of 16 and 84%. For electron signals originating from top surface layers like @S05518@ or @A00521@ and secondary ions the lateral resolution for qualitative purposes corresponds to the @B00622@. For signals originating in a greater depth of the sample (@B00583@, X-rays) the lateral resolution is worse than the corresponding value of the beam diameter due to the @D01716@ of the @P04829@. The lateral resolution may be determined exactly with a sandwich specimen or a sharp edge specimen, or approximately with a specimen showing a regular microstructure of known dimensions. Recommended abbreviation: Lat. Res. (qualitative); unit: \(\text{m}\); range: \(\text{nm}\) or \(\unicode[Times]{x3BC} \text{m}\). For @Q04980@, this should be defined as the minimum distance of two points (areas) on the specimen corresponding to signal ratios of \(10^{4}\). This condition assures that the value for the lateral resolution defines the diameter of the analytical area which yields the total analytical signal. Due to the effect of electron @D01716@ in a solid and 'tail effects' in ion beam analysis the quantitative lateral resolution is significantly larger than the beam diameter. Recommended abbreviation: Lat. Res. (quantitative); unit: \(\text{m}\); range: \(\text{nm}\) or \(\unicode[Times]{x3BC} \text{m}\).