1 Introduction

As the applications of semiconductors, MEMS and other technologies grow, the ability to make silicon wafers and films becomes more important. One of the more common ways to grow silicon wafers and thin films is through the technique called gas-source molecular beam epitaxy (GS-MBE). This process involves building up the silicon surface from silane ($\mbox{SiH}_4$) or disilane ( $\mbox{Si}_2\mbox{H}_6$) gas. This process is not limited to silicon other films are similarly formed, for example Germanium [5]. GS-MBE deposits the gas on a substrate at a particular rate. Once on the substrate the atoms diffuse to form surfaces, steps and in the end thin films. As this process becomes more and more prevalent the importance of understanding the interactions of hydrogen on the silicon surface increases. It is already well established that hydrogen on the surface inhibits surface diffusion of silicon. Hydrogen also affects the formation of the lattice causing the silicon to favor island growth over step flow growth [2,5,3]. The rate of deposition onto the substrate is a function of the temperature. This is because the hydrogen must be allowed to desorb before more silicon is deposited. Hydrogen desorbs, or leaves the surface, as $\mbox{H}_2$. Since hydrogen affects the kinetics and growth of silicon wafers its desorption is an important aspect to study [12].

Chris Siefert and Molly Moore 2002