Effect of growth conditions on epitaxial lateral overgrowth of InP on InP/Si (001) substrate by hydride vapor phase epitaxy

Author(s):  
Yan-Ting Sun ◽  
Sebastian Lourdudoss
1998 ◽  
Vol 537 ◽  
Author(s):  
R. Zhang ◽  
L. Zhang ◽  
D.M. Hansen ◽  
Marek P. Boleslawski ◽  
K.L. Chen ◽  
...  

AbstractEpitaxial lateral overgrowth (ELO) of GaN on SiO2-masked (0001) GaN substrates has been investigated by using chloride-based growth chemistries via hydride vapor phase epitaxy (HVPE) and metal organic vapor phase epitaxy (MOVPE). Diethyl gallium chloride, (C2H5)2GaCl, was used in as the MOVPE Ga precursor. The lateral and vertical growth rates as well as the overgrowth morphology of ELO GaN structures are dependent on growth temperature, V/III ratio and the in-plane orientation of the mask opening. A high growth temperature and low V/III ratio increase the lateral growth rate and produce ELO structures with a planar surface to the GaN prisms. High-quality coalesced and planar ELO GaN has been fabricated by both growth chemistries. The use of the diethyl gallium chloride source allows for the benefits of HVPE growth to be realized within the MOVPE growth environment.


2000 ◽  
Vol 639 ◽  
Author(s):  
Kazumasa Hiramatsu ◽  
Hideto Miyake

ABSTRACTFacet structures of GaN grown by epitaxial lateral overgrowth (ELO) via low pressure-metalorganic vapor phase epitaxy (LP-MOVPE) are controlled by growth conditions such as reactor pressure and growth temperature, where this technique is called FACELO (Facet Controlled ELO). The mechanism of the morphological change is discussed based on stability of the surface atoms. The propagation mechanism of the threading dislocations for the different GaN facet structure is also investigated. The distribution and density of the threading dislocations are observed by the growth pit density (GPD) method. Two typical models employing the FACELO are proposed; in one model, the dislocation concentrates only on the window area and, in the other model, only in the coalescence region in the center of the mask. In the latter model, the dislocation density is dramatically dropped to the order of 105−6 cm−2 with good reproducibility.


1999 ◽  
Vol 4 (S1) ◽  
pp. 441-446 ◽  
Author(s):  
Yasutoshi Kawaguchi ◽  
Shingo Nambu ◽  
Hiroki Sone ◽  
Masahito Yamaguchi ◽  
Hideto Miyake ◽  
...  

Selective area growth (SAG) and epitaxial lateral overgrowth (ELO) of GaN using tungsten (W) mask by metalorganic vapor phase epitaxy (MOVPE) and hydride vapor phase epitaxy (HVPE) have been studied. The selectivity of the GaN growth on the W mask as well as the SiO2 mask is excellent for both MOVPE and HVPE. The ELO-GaN layers are successfully obtained by HVPE on the stripe patterns along the <1 00> crystal axis with the W mask as well as the SiO2 mask. There are no voids between the SiO2 mask and the overgrown GaN layer, while there are triangular voids between the W mask and the overgrown layer. The surface of the ELO-GaN layer is quite uniform for both mask materials. In the case of MOVPE, the structures of ELO layers on the W mask are the same as those on the SiO2 mask for the <11 0> and <1 00> stripe patterns. No voids are observed between the W or SiO2 mask and the overgrown GaN layer by using MOVPE.


1998 ◽  
Vol 537 ◽  
Author(s):  
Yasutoshi Kawaguchi ◽  
Shingo Nambu ◽  
Hiroki Sone ◽  
Masahito Yamaguchi ◽  
Hideto Miyake ◽  
...  

AbstractSelective area growth (SAG) and epitaxial lateral overgrowth (ELO) of GaN using tungsten (W) mask by metalorganic vapor phase epitaxy (MOVPE) and hydride vapor phase epitaxy (HVPE) have been studied. The selectivity of the GaN growth on the W mask as well as the SiO2 mask is excellent for both MOVPE and HVPE. The ELO-GaN layers are successfully obtained by HVPE on the stripe patterns along the <1100> crystal axis with the W mask as well as the SiO2 mask. There are no voids between the SiO2 mask and the overgrown GaN layer, while there are triangular voids between the W mask and the overgrown layer. The surface of the ELO-GaN layer is quite uniform for both mask materials. In the case of MOVPE, the structures of ELO layers on the W mask are the same as those on the SiO2 mask for the <1120> and <1100> stripe patterns. No voids are observed between the W or SiO2 mask and the overgrown GaN layer by using MOVPE.


2014 ◽  
Vol 11 (3-4) ◽  
pp. 549-552
Author(s):  
Yasuhiro Hashimoto ◽  
Hiroshi Furuya ◽  
Motohisa Ueno ◽  
Keisuke Yamane ◽  
Narihito Okada ◽  
...  

1999 ◽  
Vol 4 (S1) ◽  
pp. 465-470
Author(s):  
R. Zhang ◽  
L. Zhang ◽  
D.M. Hansen ◽  
Marek P. Boleslawski ◽  
K.L. Chen ◽  
...  

Epitaxial lateral overgrowth (ELO) of GaN on SiO2-masked (0001) GaN substrates has been investigated by using chloride-based growth chemistries via hydride vapor phase epitaxy (HVPE) and metal organic vapor phase epitaxy (MOVPE). Diethyl gallium chloride, (C2H5)2GaCl, was used in as the MOVPE Ga precursor. The lateral and vertical growth rates as well as the overgrowth morphology of ELO GaN structures are dependent on growth temperature, V/III ratio and the in-plane orientation of the mask opening. A high growth temperature and low V/III ratio increase the lateral growth rate and produce ELO structures with a planar surface to the GaN prisms. High-quality coalesced and planar ELO GaN has been fabricated by both growth chemistries. The use of the diethyl gallium chloride source allows for the benefits of HVPE growth to be realized within the MOVPE growth environment.


2002 ◽  
Vol 41 (Part 1, No. 1) ◽  
pp. 75-76 ◽  
Author(s):  
Shinya Bohyama ◽  
Kenji Yoshikawa ◽  
Hiroyuki Naoi ◽  
Hideto Miyake ◽  
Kazumasa Hiramatsu ◽  
...  

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