Figure 3
Subshell-specific calculations of the minimum number of incident photons per pixel for a fixed incident photon energy of Einc = 10 keV, with and without the `jump ratio' approximation. The (E-D PCS + CK) calculations were carried out using excitation-dependent mass photoionization partial cross sections, while the less-accurate (JR + CK) calculations were carried out using the `jump ratio' approximation of equation (4) . In both cases, Coster–Kronig transitions were included (CK). As can be seen, the `jump ratio' approximation leads to inaccurately high calculated values of , in particular when considering fluorescence from L1 lines when the excitation energy Einc is well above the edge energy
EL1. We assumed a windowless EDS detector and a vacuum environment for these calculations so as to not affect at lower L fluorescence emission energies. Tabulated data from xraylib (Schoonjans et al., 2011 ). |