High-Temperature Growth of GaN Nanowires by Molecular Beam

Jun 29, 2015 - (27) The consequence of Ga-induced melt-back etching is observed in both optical and scanning electron micrographs (Figure 1f). In the ...
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Article pubs.acs.org/crystal

High-Temperature Growth of GaN Nanowires by Molecular Beam Epitaxy: Toward the Material Quality of Bulk GaN Johannes K. Zettler, Christian Hauswald, Pierre Corfdir, Mattia Musolino, Lutz Geelhaar, Henning Riechert, Oliver Brandt, and Sergio Fernández-Garrido* Paul-Drude-Institut für Festkörperlektronik, Hausvogteiplatz 5−7, 10117 Berlin, Germany ABSTRACT: In molecular beam epitaxy, the spontaneous formation of GaN nanowires on Si(111) substrates at elevated temperatures is limited by the long incubation time that precedes nanowire nucleation. In this work, we present three growth approaches to minimize the incubation time and to thus facilitate significantly higher growth temperatures (up to 875 °C). We achieve this advancement by (i) using III/V flux ratios of >1 to compensate for Ga desorption, (ii) introducing a two-step growth procedure, and (iii) using an AlN buffer layer to favor GaN nucleation. The GaN nanowire ensembles grown at so far unexplored substrate temperatures exhibit excitonic transitions with sub-meV linewidths comparable to those of state-of-the-art free-standing GaN layers grown by hydride vapor phase epitaxy.



INTRODUCTION In crystal growth, the concentration of point defects depends strongly on temperature. Their concentration is high at low temperatures because of limited kinetics, as well as at high temperatures where entropy governs the defect equilibrium. A minimum concentration of point defects is obtained at intermediate temperatures. For covalently bonded semiconductors, this optimal growth temperature has been theoretically predicted to be close to half of their melting point.1,2 In plasma-assisted molecular beam epitaxy (PA-MBE), however, the maximum achievable temperature for the growth of GaN films is limited by thermal decomposition because this material is thermodynamically unstable at pressures typical in the molecular beam regime (