Links in this section:

 

Introduction
Fundamentals of the TEM technique
Beam-sample interaction
The Analytical TEM
Detector Protection
Qualitative Analysis
Quantitative Analysis
Microanalysis Examples (1)
Microanalysis Examples (2)
Microanalysis Examples (3)
Summary

 

Quantitative Analysis in the AEM

 

The corrections normally associated with the analysis of thick SEM specimens do not apply to thin TEM specimens. Consequently, quantitation may be performed by using a simple ratio technique first developed by Cliff and Lorimer at the University of Manchester Institute of Science and Technology (UMIST) in the early 1970’s (Cliff and Lorimer 1975).

 

Cliff and Lorimer observed that matrix corrections are not needed when analyzing very thin films because self absorption in the film is negligible. In this case, peak intensities are proportional to concentration and specimen thickness. They removed the effects of variable specimen thickness by taking ratios of intensities for elemental peaks and introduced a “k-factor” to relate the intensity ratio to concentration ratio:

 

CA/CB = KAB.IA / IB

 

Where IA = Peak intensity for element A and CA is concentration in weight % or mass fraction. Each pair of elements requires a different k-factor which depends on detector efficiency, ionization cross section and fluorescence yield of the two elements concerned.

 

An individual k-factor relates the concentration of two elements to their X-ray peak intensities. Where more than two elements are to be analyzed, a number of k- factors may be derived by using external standards to relate known concentrations with measured intensities. If all ratios are taken with respect to a single element (this is called the ratio standard element), a sensitivity response curve may be drawn for any given detector/ microscope analytical system (Figure 5).

 

 

Theoretical k factor values may be determined using the X-ray line type (K series, L series, etc) for the ratio standard you select. For a given X-ray line, A, and ratio standard line, R, the k factor kAR is calculated as follows:

 

kAR = AA wR QB aR eR / AR wA QA aA eA

 

where A = atomic weight; w = fluorescent yield; Q = ionisation cross section; a = the fraction of the total line, e.g. Kα / (Kα +Kβ ) for a Ka line, and e = the absorption due to the detector window at that line energy.

 

Once k factors are known relative to the ratio standard, any other k factors can be calculated using the formula

 

kAB = kAR / kBR

 

Any element can be selected as the ratio standard element (R) if theoretically derived k factors are employed. Conventionally, Si is selected, but other elements such as Fe may be used instead. This selection usually depends upon the type of sample that is commonly analyzed in the microscope.

 

k factors may also be derived experimentally. A variety of standards have been used to generate these curves and it is important that the composition of the materials used is accurately known, that they are insensitive to the electron beam, and thin enough to conform to the requirements of thin film analysis. It is also necessary to make a number of measurements per standard to take into account sample inhomogeneity and statistical variation in counts.

 

It must be noted that empirically derived k- factors are system specific in the sense that they are derived for specific beam energy and EDS window thickness. Also, both theoretically and empirically derived k- factors are kV dependent.

 

Back | Next