PACS: 68.55.Jk; 81.15.KkThe effects of indium doping on the structural properties of hexagonal GaN grown on GaAsf114gB substrates with AlAs intermediate layers are investigated. It is revealed that the In doping allows us to control the residual strain in GaN, and that the highest quality can be achieved by optimizing the In flow rate so as to minimize the strain.GaN on sapphire substrates has already achieved a remarkable success in optoelectronics [1], though there are still demands for alternative substrates to overcome the difficulty presented by the use of sapphire substrates. Among many candidates, GaAs looks quite attractive because of the conductivity and cleavability, and because the mismatch in the thermal expansion coefficients of GaN (0001) and GaAs is as small as 1.8%.In preceding studies, we investigated the growth of hexagonal (h-) GaN on GaAs(001) and f11ng (n = 1, 2, 3, 4, 8) substrates by metalorganic vapor-phase epitaxy (MOVPE) [2,3]. It was found that an AlAs intermediate layer effectively prevented the cubic phase from being included in the films, and that the highest-quality GaN was obtained on f114gB substrates with a tilt of the c-axis about 20 from the surface normal toward GaAsh111iB.In order to improve the film quality further, we try Indium doping in this study. There have already been several reports on the In doping to GaN grown on sapphire substrates [4][5][6], where the improvement of the optical properties [4] and the controllability of strain [5,6] were demonstrated. In this study, we show that the degree of the residual strain can be controlled by In doping also in h-GaN on GaAs, and that this characteristic can contribute to the improvement of the film quality and to the control of the crystallographic relationship between h-GaN and AlAs/GaAs.The samples were grown on GaAsf114gB substrates by atmospheric-pressure MOVPE, and have the structure shown schematically in Fig. 1. The role of AlAs was described above. The source precursors for AlAs were trimethylaluminum and tertiarybutylarsine, and for undoped and In-doped GaN, triethylgallium, trimethylindium (TMIn), and dimethylhydrazine. The structural properties were characterized by highresolution X-ray diffraction (XRD) using Cu Ka 1 as an X-ray source. Figure 2a shows the XRD line width estimated by the asymmetric w scan of GaN(0004) as a function of the TMIn flow rate ([TMIn]). The line width had the mini-