Influence of the growth temperature of the high-temperature AlN buffer on the properties of GaN grown on Si(111) substrate

2004 ◽  
Vol 263 (1-4) ◽  
pp. 4-11 ◽  
Author(s):  
Yuan Lu ◽  
Xianglin Liu ◽  
Xiaohui Wang ◽  
Da-Cheng Lu ◽  
Dabing Li ◽  
...  
2019 ◽  
Vol 14 (9) ◽  
pp. 972-975
Author(s):  
Jun Han ◽  
Fengfeng Shi ◽  
Yanhui Xing ◽  
Peiyuan Wan ◽  
Zhiyuan Gao ◽  
...  

Nanomaterials ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 928
Author(s):  
Yong Du ◽  
Zhenzhen Kong ◽  
Muhammet Toprak ◽  
Guilei Wang ◽  
Yuanhao Miao ◽  
...  

This work presents the growth of high-quality Ge epilayers on Si (001) substrates using a reduced pressure chemical vapor deposition (RPCVD) chamber. Based on the initial nucleation, a low temperature high temperature (LT-HT) two-step approach, we systematically investigate the nucleation time and surface topography, influence of a LT-Ge buffer layer thickness, a HT-Ge growth temperature, layer thickness, and high temperature thermal treatment on the morphological and crystalline quality of the Ge epilayers. It is also a unique study in the initial growth of Ge epitaxy; the start point of the experiments includes Stranski–Krastanov mode in which the Ge wet layer is initially formed and later the growth is developed to form nuclides. Afterwards, a two-dimensional Ge layer is formed from the coalescing of the nuclides. The evolution of the strain from the beginning stage of the growth up to the full Ge layer has been investigated. Material characterization results show that Ge epilayer with 400 nm LT-Ge buffer layer features at least the root mean square (RMS) value and it’s threading dislocation density (TDD) decreases by a factor of 2. In view of the 400 nm LT-Ge buffer layer, the 1000 nm Ge epilayer with HT-Ge growth temperature of 650 °C showed the best material quality, which is conducive to the merging of the crystals into a connected structure eventually forming a continuous and two-dimensional film. After increasing the thickness of Ge layer from 900 nm to 2000 nm, Ge surface roughness decreased first and then increased slowly (the RMS value for 1400 nm Ge layer was 0.81 nm). Finally, a high-temperature annealing process was carried out and high-quality Ge layer was obtained (TDD=2.78 × 107 cm−2). In addition, room temperature strong photoluminescence (PL) peak intensity and narrow full width at half maximum (11 meV) spectra further confirm the high crystalline quality of the Ge layer manufactured by this optimized process. This work highlights the inducing, increasing, and relaxing of the strain in the Ge buffer and the signature of the defect formation.


2005 ◽  
Vol 198 (1-3) ◽  
pp. 350-353 ◽  
Author(s):  
Xianfeng Ni ◽  
Liping Zhu ◽  
Zhizhen Ye ◽  
Zhe Zhao ◽  
Haiping Tang ◽  
...  

2008 ◽  
Vol 1068 ◽  
Author(s):  
Ewa Dumiszewska ◽  
Wlodek Strupinski ◽  
Piotr Caban ◽  
Marek Wesolowski ◽  
Dariusz Lenkiewicz ◽  
...  

ABSTRACTThe influence of growth temperature on oxygen incorporation into GaN epitaxial layers was studied. GaN layers deposited at low temperatures were characterized by much higher oxygen concentration than those deposited at high temperature typically used for epitaxial growth. GaN buffer layers (HT GaN) about 1 μm thick were deposited on GaN nucleation layers (NL) with various thicknesses. The influence of NL thickness on crystalline quality and oxygen concentration of HT GaN layers were studied using RBS and SIMS. With increasing thickness of NL the crystalline quality of GaN buffer layers deteriorates and the oxygen concentration increases. It was observed that oxygen atoms incorporated at low temperature in NL diffuse into GaN buffer layer during high temperature growth as a consequence GaN NL is the source for unintentional oxygen doping.


2007 ◽  
Vol 307 (2) ◽  
pp. 289-293 ◽  
Author(s):  
M.Z. Peng ◽  
L.W. Guo ◽  
J. Zhang ◽  
N.S. Yu ◽  
X.L. Zhu ◽  
...  

1994 ◽  
Vol 339 ◽  
Author(s):  
A. Ohtani ◽  
K. S. Stevens ◽  
R. Beresford

ABSTRACTWurtzite GaN films on AlN buffer layers were grown on Si (111) by electron cyclotron resonance microwave plasma assisted MBE (ECR-MBE). High resolution x-ray diffraction studies indicate that the mosaic disorder decreases with increasing growth temperature. The grain size is related to the growth temperature. The best (0002) diffraction peak full width at half maximum was 22 min. for a film 1.7 μm thick. Prominent exciton luminescence is observed at 3.46 eV at 10 K.The plasma I-V characteristics were measured with a Langmuir probe near the growth position. The nitrogen ion density has been extracted from the data, and is a strong function of the N2 flow rate, the microwave power and the aperture size of the ECR source. The crystal quality of AlN is strongly affected by the plasma conditions.


2003 ◽  
Vol 0 (7) ◽  
pp. 2095-2098 ◽  
Author(s):  
Kwang Suk Son ◽  
Dongyu Kim ◽  
Hyung Koun Cho ◽  
Kyuhan Lee ◽  
Sunwoon Kim ◽  
...  

2011 ◽  
Vol 110-116 ◽  
pp. 991-996
Author(s):  
Lee Siang Chuah ◽  
A. Mahyudin ◽  
Z. Hasan ◽  
C.W. Chin

A high-quality crack-free AlN cap layer on GaN layer has been achieved using an AlN buffer layer directly grown on a silicon substrate at high temperature by radio frequency (RF) plasma-assisted molecular beam epitaxy. A two dimensional (2D) growth process guide to AlN cap layer of high grade crystal quality. The nucleation and the growth dynamics have been studied by in situ reflection high energy electron diffraction (RHEED) and ex situ by high resolution transmission electron microscopy (HR-TEM). The microstructure was investigated by energy-dispersive X-ray spectroscopy (EDX). It was disclosed that AlN is single crystalline with low defect. High densities of V-shaped pits were not detected at the interface between AlN and GaN layers. Contradictory the earlier reported V-shaped defects in nitride-based alloys; these V-shaped pits were condensed on top of the AlN layer because of H2 etching of the surface when a high temperature growth discontinuity between AlN and GaN layers.


2014 ◽  
Vol 114 ◽  
pp. 26-28 ◽  
Author(s):  
Yiren Chen ◽  
Hang Song ◽  
Dabing Li ◽  
Xiaojuan Sun ◽  
Hong Jiang ◽  
...  

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