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
| A partial cross-section specifies
the probability of a specific shell scattering through angles
up to a specific angle, β, and with energy losses covering an energy range, Δ,
above an ionization energy. For instance, the partial cross-section, σK(β,Δ), of K-shell, EK, can be given by, [1] For elements of low atomic number, σK(β,Δ) can be measured by EELS [1, 3-5], This approximation in Equation 954b is accurate for Δ ≥ 50 eV. [1,5] Based on Equation 954b, the Areal Density, N, namely the number of atoms per unit area of the TEM sample through the electron beam, can be obtained by, [1] In practice, σK(β,Δ) obtained by Equations 954a or 954b can be applied into Equation 954c for Areal Density, N, calculation. For large collection angles, the partial ionization cross-section, σ(β,Δ), becomes the total ionization cross-section, σ(Δ).
[1] R. F. Egerton, K-shell ionization cross-sections for use in microanalysis, 4(2), (1979) 169-179.
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