Zinc-blende and wurtzite phase separation in catalyst-free molecular beam epitaxy vapor-liquid-solid-grown Si-doped GaAs nanowires on a Si(111) substrate induced by Si doping

被引:0
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作者
Suzuki, Akio [1 ]
Fukuyama, Atsuhiko [1 ]
Suzuki, Hidetoshi [1 ]
Sakai, Kentaro [2 ]
Paek, Ji-Hyun [3 ]
Yamaguchi, Masahito [3 ]
Ikari, Tetsuo [1 ]
机构
[1] Miyazaki Univ, Fac Engn, Miyazaki 8892192, Japan
[2] Miyazaki Univ, Ctr Collaborat Res & Community Cooperat, Miyazaki 8892192, Japan
[3] Nagoya Univ, Dept Elect Engn & Comp Sci, Nagoya, Aichi 4648603, Japan
基金
日本学术振兴会;
关键词
CORE-SHELL NANOWIRES; III-V NANOWIRES;
D O I
10.7567/JJAP.54.035001
中图分类号
O59 [应用物理学];
学科分类号
摘要
The effect of Si-doping on the phase separation of wurtzite (WZ) and zinc-blende (ZB) phases in catalyst-free Si-doped GaAs nanowires (NWs) grown on a Si(111) substrate was investigated using transmission electron microscope (TEM), high-resolution X-ray diffraction (HR-XRD), lowtemperature photoreflectance (PR), and photoluminescence (PL) techniques. The appearance of WZ structure with an increase in the amount of Si dopant was observed through TEM, and the results showed that the thicknesses of ZB and WZ structures were random. Furthermore, all NW samples exhibited HR-XRD diffraction peaks at the (0002) and (111) planes, which correspond to the WZ and ZB structures, respectively. Their peak intensity ratio [WZ/(WZ + ZB)] increased with the amount of Si doping. The PR modulus and PL spectra at 4K for the sample with the middle amount of Si doping in three samples exhibited peaks at 1.43, 1.49, and 1.51 eV. The peaks at 1.51 and 1.49 eV were presumed to result from band-to-band and conduction-band-to-Si-acceptor transitions, respectively. In accordance with the prediction by a theoretical band alignment calculation of the conduction-and valence-bands discontinuities, the transition energy of 1.43 eV was due to the interband transition at the WZ-ZB interface. We also found that the 1.43 eV PR and PL peaks became dominant when the amount of Si doping increased. This indicate that this interband transition became significant when the amount of WZ phase increased, which resulted from the increased Si doping. The appearance of type-II band structures induced by Si doping was also confirmed. (C) 2015 The Japan Society of Applied Physics
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页数:5
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