Practical Electron Microscopy and Database

An Online Book, Second Edition by Dr. Yougui Liao (2006)

Practical Electron Microscopy and Database - An Online Book

Chapter/Index: Introduction | A | B | C | D | E | F | G | H | I | J | K | L | M | N | O | P | Q | R | S | T | U | V | W | X | Y | Z | Appendix

EELS Intensity Depending on Areal Density of Atoms

In Electron Energy Loss Spectroscopy (EELS), the quantification of elemental species is fundamentally based on the relationship between the element-specific core-loss signal and the areal density of atoms. The areal density of a given element is directly proportional to the , given by:

EELS Intensity Depending on Areal Density of Atoms -------------------------------------------- [4757a]

where,

represents the total spectrum intensity.
σ denotes the core-loss edge cross-section for inelastic scattering.

Accurate extraction of from the EELS spectrum requires careful background subtraction, typically achieved through conventional extrapolation techniques to remove the power-law background signal. Alternatively, multiple linear least-squares (MLLS) fitting can be employed to decompose the EELS spectrum into its component signals, allowing for precise quantification even in the presence of overlapping edges.

Figure 4757 shows the Nk as a function of It and σ. is inversely proportional to both and , which reflects the fact that as the total spectrum intensity increases or the cross-section for inelastic scattering becomes larger, fewer atoms are needed to produce the same core-loss signal. The contour plot visually represents this relationship: higher values of occur when both and are low, while decreases as either or σ increases

Areal density Nk as a function of It and σk

Figure 4757. Areal density Nk as a function of It and σ.