I. Introduction
MATERIALS such as dicaesium telluride (Cs2Te) and gallium arsenide (GaAs) are examples of photocathodes at either end of the visible spectrum, with a wide range of applications, e.g. in defence, security and remote sensing. One route to manufacturing these materials is through molecular beam epitaxy (MBE) [1], which gives significant control over the stoichiometry and crystallinity of the photocathode material. Varying the stoichiometry, and properties of the crystal structure such as the Miller index, can have a significant effect on the work function, the band structure and the electron affinity. By identifying the ideal material properties for a photocathode, MBE can be used to synthesise this material.