IntroductionA fission track is a linear region of intense radiation damage formed by the passage of an energetic, charged nuclear particle through an insulating solid. According to a popular hypothesis, known as the 'ion explosion spike' model (Fleischer et al., 1975), the charged particle collides with atoms in its path, displaces them and removes their electrons, producing a narrow zone rich in positive ions, which repulse each other into interstitial positions and form vacancies. An elastic adjustment of the crystal or glass then occurs, straining the undamaged matrix (Fleischer, 2004). Another idea, called the 'thermal spike' model, sees the fast-moving fission fragment producing intense heat along its trajectory. After passage of the charged particle, the track core is quenched by heat loss to the adjacent lattice, leaving it in a disordered state. According to Chadderton (2003), it is likely that both mechanisms are involved in track formation. Maximum density damage exists at the site of fission and decreases to the track termini. This damaged zone persists in the solid after the fission fragment has come to a rest and is called a latent track. Its length is equal to the sum of the range of the two charged particles formed by nuclear fission, each moving in opposite directions. 238 U fission events form latent tracks that are 6-10 nm wide and 10-20 mm long and account for most tracks in natural, terrestrial materials. Latent tracks can only be observed with a transmission electron microscope but can be made visible by chemical etching (Young, 1958) and readily seen under an optical microscope. Etching takes place by rapid dissolution of the disordered region of the track core, which exists in a state of higher free energy than the undamaged material. As can be seen in Figure 1, the shape of the etched fission tracks varies in different materials, due mainly to differences in symmetry and magnitude of the difference between the track and bulk etch rates. Fission tracks in glass are relatively wide, conical pits due to its isotropic properties and a track etch rate that is not much greater than the bulk etch rate. Micas have diamond-shaped tracks, whereas tracks in zircon and apatite are needle-like because of the large difference between track and bulk etch rates, the former being much greater.Fission tracks have varied uses ranging from applications in the fields of engineering, medicine, nuclear physics, and space sciences to the earth sciences (Fleischer, 1998). The most important applications in the earth sciences are thermochronology (Reiners and Ehlers, 2005) and geochronology. Thermochronology -the more active field at present -focuses on understanding the thermal history of rocks and duration and rates of geological processes, such as crustal uplift.
643Geochronology, on the other hand, is primarily concerned with formation age, the topic of interest to us here.Zircon and glass are the most suitable phases for dating Quaternary deposits by fission-track (FT) methods, although apatite and sphene may ...