Abstract
Ion tracks in solids can be visualized by appropriate etching. During the etching procedure, size and depth of the etch pits grow linearly with time. Their shape is mainly controlled by the crystal structure. For example, in muscovite, ion tracks have a rhombic cross-section after HF etching, whereas in polycarbonate etch pits are circular after NaOH etching. Natural phlogopite (dark mica) may contain fission tracks and alpha-recoil tracks (ART) as latent radiation damage. HF can be used to make them visible by optical, scanning electron and scanning force microscopy (SEM, SFM). ART, generated by collisions of the recoil nuclei with the lattice atoms, provide etch pits, which are triangular at the surface, whereas the fission tracks, created via electronic energy loss (d E/d x), have hexagonal etch pits. After ion irradiation of phlogopite in the electronic d E/d x regime, the etch pits are triangular below 5.7 keV/nm and hexagonal above 8.8 keV/nm in shape. To examine more precisely the shape transition and its relation to the radiation damage, phlogopite from the Kerguelen Islands (French territory, Indian Ocean) was first annealed (500 °C, 3.5 h) and subsequently irradiated at GSI with 58Ni (kinetic energy ∼81 MeV), d E/d x amounting to 10.4 keV/nm (according to SRIM 2000). Using polyethylene terephthalate (PET) foils of seven different thicknesses as a degrader, d E/d x in the sample could be reduced stepwise to 2.4 keV/nm. The irradiated samples were etched with 4% HF at room temperature and afterwards imaged with SEM and SFM. It was observed that the triangles relate to the octahedral sites (represented by OH, O, Fe, Mg and other ions) and the hexagons to the SiO 4-tetahedral positions in the tetrahedral sheet. We interpret our findings as evidence that the d E/d x-dependent etch-pit morphologies are controlled by the lattice structure.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
More From: Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.