Annealing for Tailoring Au/GaN Schottky-Barrier Height
- Created on Tuesday, 01 January 2002
It should be possible to make metal/semiconductor contacts more reproducible.
Annealing has been found to be an effective means of tailoring the height of a Schottky barrier between gold and gallium nitride. This finding offers promise for the development of improved metal contacts on GaN semiconductors. Heretofore, the commercialization of GaN semiconductor devices has been impeded by difficulties of fabrication and by nonreproducibility of the Schottky-barrier heights and other properties of the metal/GaN interfaces. Now it appears that annealing may be the key to making GaN devices with smaller unit-tounit variations of contact properties and, in particular, tailorability of Schottky-barrier heights over a wide energy range.
Prior attempts to tailor Schottky contact properties had focused on details of surface cleaning and of growth and bulk properties of GaN. These attempts were not successful: unit-to-unit variations were still observed, even after cleaning and growth under controlled conditions. Although the causes of these variations are still not fully understood, more recent studies led to a partial explanation and to the annealing approach: It appears that the growth of GaN can result in a near-surface region wherein there are nonequilibrium concentrations of vacancies in Ga and N sites. These concentrations depend on aspects of the growth process that are difficult to control. These vacant sites act, variously, as electron acceptors or donors within the GaN semiconductor. As such, these sites affect the Schottky contact properties.
It was hypothesized that annealing of GaN prior to deposition of metal could be beneficial for tailoring Schottky contact properties because by suitable choice of annealing conditions (time, temperature, and either nitrogen atmosphere or high vacuum), it should be possible to produce a surface region with (1) a desired composition somewhere within a range from Ga-rich to N-rich and (2) corresponding values of nearsurface doping and Schottky-barrier height. This hypothesis was investigated in experiments on GaN specimens that were cleaned with HCl, then annealed prior to deposition of Au by vacuum evaporation. The specimens were then probed by ballistic-electron-emission microscopy (BEEM) for measurement of interface transmission efficiencies and Schottky-barrier heights. For comparison, some specimens were subjected to cleaning by HCl but not annealed. Other specimens were cleaned by other chemical treatments; these specimens were also not annealed. In the absence of annealing, neither the HCl treatment nor the other chemical treatments yielded substantial increases in interface transmission.
The figure shows a typical BEEM spectrum for a specimen that was not annealed, and for two other specimens that were annealed in ultrahigh vacuum for 15 minutes — one at a temperature of 340 °C and one at a temperature of 580 °C. Features of BEEM spectra can be correlated with interface properties. The voltage threshold for the onset of measurable current yields the interface Schottky-barrier height, and the magnitude of the current above this threshold indicates the fraction of the electrons injected by BEEM can cross the interface. This in turn gives information on the ideality of the interface, i.e., interface quality. Changes in these interface properties result in changes in features of the BEEM spectra. The figure shows that Schottky-barrier heights decrease, and interface transmission increases, as annealing temperature is increased. Other spectra taken after annealing at other temperatures confirm this trend. It has also been determined from BEEM spectroscopy that the starting interface properties and the direction of their change with temperature depend partly on the previous thermal history of the specimen. The changes in Schottky-barrier heights have been interpreted in terms of the creation of vacancies or the diffusion of vacancies toward the GaN surface.
This work was done by L. Douglas Bell and R. Peter Smith of Caltech for NASA’s Jet Propulsion Laboratory. For further information, access the Technical Support Package (TSP) free on-line at www.nasatech.com/tsp under the Materials category.
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