We describe the recent inclusion in Geant4 of state-of-the-art proton and alpha particle shell ionisation cross sections based on the ECPSSR approach as calculated by Cohen et al., called here ANSTO ECPSSR. The new ionisation cross sections have been integrated into Geant4. We present a comparison of the fluorescence X-ray spectra generated by the ANSTO ECPSSR set of cross sections and, alternatively, the currently available sets of Geant4 PIXE cross sections. The comparisons are performed for a large set of sample materials spanning a broad range of atomic numbers. The two alternative PIXE cross sections approaches (Geant4 and ANSTO) have been compared to existing experimental measurements performed at ANSTO with gold, tantalum and cerium targets of interest for nanomedicine applications. The results show that, while the alternative approaches produce equivalent results for vacancies generated in the K and L shell, differences are evident in the case of M shell vacancies. This work represents the next step in the effort to improve the Geant4 modelling of the atomic relaxation and provide recommended approaches to the Geant4 user community. This new Geant4 development is of interest for applications spanning from life and space to environmental science.
Abstract 7We describe the recent inclusion in Geant4 of state-of-the-art proton and alpha particle shell 8 ionisation cross sections based on the ECPSSR approach as calculated by Cohen et al., called 9 21 Keywords 22 Geant4, PIXE, ionisation cross sections, ECPSSR. 23 detector and to reduce the low energy X-ray yield from light elements such as the underlying Si 126 in some of the samples, a 100µm thick Mylar absorber (or filter) was placed in front of the 127 detector. The data were collected using the Data Acquisition System mpsys4 from Melbourne 128 University together with a Canberra Model 2060 digital signal processor. The irradiated samples 129 were 100nm thick Au layer on silicon and 25nm TaO layer on graphite. Additionally, a sample of 130 CeO 2 embedded in a boron oxide pellet was used. 131 4. Results 132 4.1. Ionisation cross section comparison 133 The proposed ANSTO ionisation cross sections have been calculated for all elements. As 134 example Figures 1 and 2 show the cross sections for a gold target against the kinetic energy of 135 incident protons and alpha particles, respectively.