MBE allows the controlled growth of semiconductor layers with monolayer precision. A simple schematic of a typical MBE system is shown in Prutton, Fig. 6.18. The layers are grown, as you should expect by now, under UHV conditions. Knudsen cells are used to deposit the various materials (eg Ga, As, In, Al etc…) onto a heated substrate which is rotated during growth to maximise growth homogeneity. Shutters are used to switch the molecular beams on and off and an ion gauge, as described in Section 3.4, monitors the pressure. The MBE growth chamber will typically be coupled, via a valve, to an analysis chamber where electron or optical spectroscopies or STM may be carried out. A very important in situ diagnostic tool used to monitor the film quality during growth is reflection high energy electron diffraction (RHEED) (the electron gun and, as for LEED, fluorescent screen used to monitor diffraction patterns are shown in Fig. 6.18 of Prutton). We'll return to a discussion of this technique and its importance in MBE growth in Section 6.
To date, most MBE growth has involved III-V compounds (GaAs, InAs, AlGaAs, InSb etc…) although there is increasing interest in MBE-grown Si and SiGe structures. While MBE homoepitaxial growth processes (eg GaAs on GaAs, InAs on InAs etc..) are certainly very important, a wealth of fascinating physics has arisen from our ability to produce high quality semiconductor heterostructures using MBE. For example, the band gap of the AlGaAs compound varies with the relative concentrations of Al and Ga – concentrations which are directly controllable in MBE. The ability to both control the band gap of a material via changes in its composition ( band gap engineering) and to epitaxially grow one layer of semiconductor on another revolutionised semiconductor fabrication processes and has led to the development of numerous important electronic and optoelectronic devices. (If you're interested in this topic, next semester's Semiconductor Physics & Devices module discusses some of those devices in detail).
Let's discuss some of the fundamental principles underlying MBE on the basis of the adsorption, diffusion and growth processes covered in the previous sections. Until very recently MBE focussed on the growth of lattice-matched materials such as AlGaAs on GaAs which exhibit a layer-by-layer (FM) growth mode. Layer-by-layer growth in MBE may proceed via two very distinct limiting mechanisms, related to the magnitude of the diffusion constant D (Fig. 4.18):
The step flow growth mechanism exhibits a considerable degree of anisotropy on GaAs(100) surfaces. Can you suggest some possible origins for this anisotropy?
An STM image of InAs islands grown by MBE on a GaAs substrate is shown in Fig 4.19. Give reasons why InAs, unlike AlGaAs or AlAs, for example, forms nanoscale dots on the GaAs substrate.