Authors: S. Sanorpim, D. Kaewket, Sukkaneste Tungasmita, R. Katayama, Kentaro Onabe
Abstract: Optical transitions in the In0.050Ga0.950P0.975N0.025/GaP lattice-matched single quantum
wells (SQWs) with different well widths (LZ = 1.6 - 6.4 nm) have been investigated by
low-temperature photoluminescence (PL) and PL-excitation (PLE). PL spectra showed the strong
visible emission from the samples which attracted to a variety of optoelectronic device applications
such as light emitting and laser diodes. Comparing to the bulk film, the PL peak position and the
fundamental absorption edge of PLE spectra exhibit blue-shift, which is corresponded to the quantum
confinement effect by the well. Comparison between the absorption edge of PLE spectra and the finite
square well calculation demonstrate that the effective bandgap energy of the InGaPN/GaP system is
might be originated mainly from the N-related localized states.
224
Authors: S. Sanorpim, P. Kongjaeng, R. Katayama, Kentaro Onabe
Abstract: The use of an InGaAs buffer layer was applied to the growth of thick InxGa1-xAs1-yNy layers
with higher In contents (x > 30%). In order to obtain the lattice-matched InGaAsN layer having the
bandgap of 1.0 eV, the In0.2Ga0.8As was chosen. In this work, the In0.3Ga0.7As0.98N0.02 layers were
successfully grown on closely lattice-matched In0.2Ga0.8As buffer layers (InGaAsN/InGaAs).
Structural quality of such layers is discussed in comparison with those of the In0.3Ga0.7As0.98N0.02
layers grown directly on the GaAs substrate (InGaAsN/GaAs). Based on the results of transmission
electron microscopy, the misfit dislocations (MDs), which are located near the InGaAsN/GaAs
heteroepitaxial interface, are visible by their strain contrast. On the other hand, no generation of the
MDs is evidenced in the InGaAsN layer grown on the In0.2Ga0.8As pseudosubstrate. Our results
demonstrate that a reduction of misfit strain though the use of the pseudosubstrate made possible the
growth of high In-content InGaAsN layers with higher crystal quality to extend the wavelength of
InGaAsN material.
221
Authors: S. Sanorpim, F. Nakajima, R. Katayama, Kentaro Onabe
Abstract: The high quality GaAsN epitaxial films with the typical thickness of 150-200 nm and the N
contents up to 5.5% were grown by MOVPE. The maximum N content of 2.75% at the growth
temperature of 550 oC was enhanced to 5.1% at 500 oC and 5.5% at 450 oC. The lower growth
temperature may efficiently suppress desorption of N atoms from the growing surface. The narrow
high-resolution X-ray diffraction peaks and the clear Pendellösung fringes indicate that the GaAsN
films with high uniformity and fairly flat interface were obtained. The 6K-photoluminescence (PL)
peak energy of the GaAsN films was varied from 1.38 eV to 1.01 eV with increasing N content up to
2.75%, but no near-band-edge emission was observed in the higher-N-content films, indicating the
increase of nonradiative recombination centers caused by the N-related lattice imperfections. Besides,
after post growth thermal annealing at 650 oC for 2 min, PL spectrum shows that the near-band-edge
emission as low as 0.97 eV (1.3 μm) have been achieved with the film of 5.1% N.
218
Authors: Zong You Yin, Xiao Hong Tang, Ji Xuan Zhang, Deny Sentosa, Jing Hua Teng, An Yan Du, Mee Koy Chin
Abstract: Morphology and crystal-quality of InAs/In0.53Ga0.47As/InP quantum dots (QDs) grown by
metal-organic vapor phase epitaxy (MOVPE) in N2 ambient using different growth modes have
been studied. It is found that the morphology and crystal-quality of InAs QDs are dependant on the
growth modes. After optimizing the dots’ growth modes, dots’ size dispersion and crystal-quality
are both improved greatly, resulting in the enhancement factor of ∼ 2.9 in the photoluminescence
(PL) peak-intensity from single QD. When the dots are buried, the dot size decrease compared with
the free-standing dots due to the soon capping layer deposition during dots’ being buried. The
thermal activation energy measured is comparable to the valence-band offset in the QD system
calculated by 8 kp theory model. This indicates the PL quenching induced by the interface defects is
suppressed due to the defect density lowering in the QDs grown by such optimized growth mode.
17
Authors: M.K. Hudait, S.B. Krupanidhi
15
Authors: Andrey Bakin, A.A. Ivanov, Kensaku Hisada, T. Riedl, F. Hitzel, H.-H. Wehmann, A. Schlachetzki
163
Authors: Y. Takano, Shunro Fuke
77
Authors: H. Lahrèche, V. Bousquet, M. Laügt, Olivier Tottereau, P. Vennéguès, B. Beaumont, Pierre Gibart
1487
Authors: Robert F. Davis, O.H. Nam, T.S. Zheleva, Thomas Gehrke, Kevin J. Linthicum, Pradeep Rajagopal
1471