Cubic GaN Heteroepitaxy on Thin-SiC-Covered Si(001)

1998 ◽  
Vol 537 ◽  
Author(s):  
Yuichi Hiroyama ◽  
Masao Tamura

We have investigated the growth conditions of cubic GaN (β-GaN) layers on very thin SiC-covered Si(001) by using gas-source molecular beam epitaxy as functions of SiC layer thickness, Ga-cell temperature and substrate temperature. Under the present SiC formation conditions on Si substrates by carbonization using C2H2, gas, the SiC layers with the thickness between 2.5 and 4 nm result in the epitaxial growth of β-GaN on thus SiC-formed Si substrates. At the highest GaN growth rate of 110 nm/h (a Ga-cell temperature of 950 °C), β-GaN layers grown at a substrate temperature of 700 °C show a nearly flat surface morphology and the fraction of included hexagonal GaN becomes negligible when compared to the results of β-GaN layers grown under other conditions of Ga-cell and substrate temperatures. Thus obtained β-GaN films have good performance in photoluminescence intensity although the FWHM of band-edge recombination peak is still wider (137 meV) than the reported values for the β-GaN on 3C-SiC and GaAs.

1999 ◽  
Vol 4 (S1) ◽  
pp. 155-160
Author(s):  
Yuichi Hiroyama ◽  
Masao Tamura

We have investigated the growth conditions of cubic GaN (β-GaN) layers on very thin SiC-covered Si(001) by using gas-source molecular beam epitaxy as functions of SiC layer thickness, Ga-cell temperature and substrate temperature. Under the present SiC formation conditions on Si substrates by carbonization using C2H2 gas, the SiC layers with the thickness between 2.5 and 4 nm result in the epitaxial growth of β-GaN on thus SiC-formed Si substrates. At the highest GaN growth rate of 110 nm/h ( a Ga-cell temperature of 950 °C), β-GaN layers grown at a substrate temperature of 700 °C show a nearly flat surface morphology and the fraction of included hexagonal GaN becomes negligible when compared to the results of β-GaN layers grown under other conditions of Ga-cell and substrate temperatures. Thus obtained β-GaN films have good performance in photoluminescence intensity although the FWHM of band-edge recombination peak is still wider (137 meV) than the reported values for the β-GaN on 3C-SiC and GaAs.


1992 ◽  
Vol 263 ◽  
Author(s):  
K. Werner ◽  
S. Butzke ◽  
J.W. Maes ◽  
O.F.Z. Schannen ◽  
J. Trommel ◽  
...  

ABSTRACTWe have studied the deposition of GexSi1−x layers on (100) Si substrates by gas source molecular beam epitaxy (GSMBE) using disilane and germane.The investigation of RHEED intensity oscillations during growth reveals the well known rate enhancement obtained when adding a small amount of germane to the disilane flux. However, when exposing a previously deposited Ge layer to a pure disilane flux the growth rate during the first few monolayers remains at an enhanced value but returns to its homoepitaxial value after about 10 to 15 monolayers. This behaviour was observed under a variety of growth conditions. It is in marked contrast to the experience obtained in conventional Si/Ge MBE and suggests a catalytic effect of the particular surface present during GSMBE growth. We propose that this effect is caused by the surface segregation of Ge species and leads to a smear-out of the Ge profile in the layer.


2013 ◽  
Vol 740-742 ◽  
pp. 339-343 ◽  
Author(s):  
Shota Sambonsuge ◽  
Eiji Saito ◽  
Myung Ho Jung ◽  
Hirokazu Fukidome ◽  
Sergey Filimonov ◽  
...  

3C-SiC is the only polytype that grows heteroepitaxially on Si substrates and, therefore, it is of high interest for various potentail applications. However, the large (~20 %) lattice mismatch of SiC with the Si substrate causes a serious problem. In this respect, rotated epitaxy of 3C-SiC(111) on the Si(110) substrate is highly promising because it allows reduction of the lattice mismatch down to a few percent. We have systematically searched the growth conditions for the onset of this rotated epitaxy, and have found that the rotaed epitaxy occurrs at higher growth temperatures and at lower source-gas pressures. This result indicates that the rotated epitaxy occurs under growth conditions that are close to the equilibrium and is thefore thermodynamically, rather than kinetically, driven.


1991 ◽  
Vol 241 ◽  
Author(s):  
W. J. Schaff ◽  
S. D. Offsey ◽  
X. J. Song ◽  
L. F. Eastman ◽  
T. B. Norris ◽  
...  

ABSTRACTThe effect of growth conditions on the properties of GaAs grown by molecular beam epitaxy at low substrate temperatures has been studied. It has been found that the response time to 100 fsec 830nm light pulses is a function of substrate temperature and arsenic flux. The reason for variation of optical response with growth conditions is related to the nature of the incorporation of excess arsenic. A recent model proposed by Warren and others is invoked to explain the change in optical response with growth conditions. Further substantiation of this model comes from experiments on the annealing of low substrate temperature GaAs which has been doped with silicon.


1998 ◽  
Vol 191 (1-2) ◽  
pp. 34-38
Author(s):  
Xiaobing Li ◽  
Dianzhao Sun ◽  
Jianping Zhang ◽  
Shirong Zhu ◽  
Meiying Kong

1998 ◽  
Vol 264-268 ◽  
pp. 1173-1176 ◽  
Author(s):  
B. Schöttker ◽  
J. Kühler ◽  
Donat J. As ◽  
D. Schikora ◽  
K. Lischka

2014 ◽  
Vol 32 ◽  
pp. 1460341 ◽  
Author(s):  
Usman Ilyas ◽  
P. Lee ◽  
T. L. Tan ◽  
R. V. Ramanujan ◽  
Sam Zhang ◽  
...  

This study reports the enhanced ferromagnetic ordering in ZnO:Mn nanoparticle thin films, grown at different substrate temperatures using pulsed laser deposition. The optimum growth conditions were deduced from X-ray, photoemission and magnetic measurements. The X-ray measurements reveal that there was an optimum substrate temperature where the thin films showed relatively stronger texture, better crystallinity and lower strain. Substrate temperature tuned the deep level recombination centers in ZnO:Mn , which changed the optical quality by altering the electronic structure. The M-H curves, in the present study, revealed superior ferromagnetic response of 20-nm sized particles in ZnO:Mn thin film grown at a substrate temperature of 450 °C. Ferromagnetic ordering becomes weaker at higher/lower substrate temperatures due to the activation of native defects in ZnO host matrix.


1992 ◽  
Vol 70 (10-11) ◽  
pp. 886-892 ◽  
Author(s):  
C. Qiu ◽  
R. V. Kruzelecky ◽  
D. A. Thompson ◽  
D. Comedi ◽  
G. Balcaitis ◽  
...  

The growth of InAsyP1−y onto (100) InP by gas-source molecular beam epitaxy was examined systematically, focusing on control of the resulting As/P incorporation ratio. The group V fluxes were obtained by passing phosphine and arsine through a dual-input low-pressure gas cracker. For a given flow ratio of the source gases, the arsenic fraction y of the resulting InAsyP1−y films is seen to increase with the film thickness over the first 1500 Å (1 Å = 10−10 m) as indicated by secondary ion mass spectroscopy, Auger depth profiling, and by Rutherford backscattering spectroscopy. Thin, strained InAsyP1−y layers (0.30 < y < 0.70, corresponding to a compressive strain of about 1.0–2.2%) contain about 5–20% less As than similarly grown thicker, relaxed layers. For a given growth rate and substrate temperature, the relative compositional shift is found to be linearly proportional to the effective strain corresponding to y. Substrate temperatures above 475 °C further reduce the incorporation ratio of As into both strained and relaxed InAsyP1−y layers, initially enhancing the strain-induced compositional shift. However, strain minimization via a compositional shift competes with a greater rate of relaxation of the InAsP lattice with film thickness at higher substrate temperatures.


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