Close-spaced vapor transport reactor for III-V growth using HCl as the transport agent

2019 ◽  
Vol 506 ◽  
pp. 147-155 ◽  
Author(s):  
Christopher J. Funch ◽  
Ann L. Greenaway ◽  
Jason W. Boucher ◽  
Robert Weiss ◽  
Alex Welsh ◽  
...  
2019 ◽  
Vol 55 (9) ◽  
pp. 898-902 ◽  
Author(s):  
K. S. Nikonov ◽  
M. N. Brekhovskikh ◽  
T. K. Menshchikova ◽  
V. A. Fedorov

1989 ◽  
Vol 67 (4) ◽  
pp. 251-258 ◽  
Author(s):  
E. Koskiahde ◽  
D. Cossement ◽  
R. Paynter ◽  
J. P. Dodelet ◽  
A. Jean ◽  
...  

Using H2O as a transport agent, epitaxial GaAs layers were grown by the close-spaeed vapor transport technique (CSVT) on (100) heavily Si-doped GaAs substrates. Three kinds of GaAs sources were used for the deposition: (100) GaAs, heavily doped with Te or Si, and undoped semi-insulating (SI) (100) GaAs. The growth rates obtained with SI and Te-doped GaAs are quite similar and show a clear tendency to be superior to the growth rates measured for Si-doped GaAs sources. Uncompensated charge carrier density (ND – NA) profiles have been measured electrochemically for the layers grown with the three kinds of sources. When Te-doped GaAs is used, (ND – NA) obtained for the epitaxy is the same as that of the source, implying a complete transfer of the Te impurity. (ND – NA) values varying from 1016 to 1018 cm−3 are obtained from SI GaAs sources, depending upon the thickness of the epitaxial layer. (ND – NA) < 1015 cm−3 are measured for layers grown from Si-doped GaAs sources. In this case, layers thicker than 10 μm cannot be mesured electrochemically because of their excessively high resistance. The small (ND – NA) values obtained in that case are explained by the reaction of Si contained in the source with the transport agent (H2O), resulting in the formation, at the Si-doped GaAs surface, of a passivating SiOx layer revealed by Auger spectroscopy. This passivating layer also explains the smaller growth rates measured with these sources. p–n Junctions have been prepared by Zn diffusion in CSVT layers grown from SI GaAs sources. Their I–V characteristics show good rectification behavior, indicating that the CSVT layers could be used for photovoltaic purposes.


2005 ◽  
Vol 279 (1-2) ◽  
pp. 206-212 ◽  
Author(s):  
Lenka Hannevold ◽  
Ola Nilsen ◽  
Arne Kjekshus ◽  
Helmer Fjellvåg

2007 ◽  
Vol 304 (1) ◽  
pp. 37-41 ◽  
Author(s):  
Makoto Mikami ◽  
Sang-Hwui Hong ◽  
Takashi Sato ◽  
Seishi Abe ◽  
JiFeng Wang ◽  
...  

2005 ◽  
Vol 475-479 ◽  
pp. 1689-1692
Author(s):  
Huan Yong Li ◽  
Ke Wei Xu ◽  
Wan Qi Jie

Two chemical vapor transport methods with Zn(NH4)3Cl5 transport agent were developed to grow ZnSe bulk single crystals. Two kinds of Zn-rich ZnSe single crystals, conical crystal and flake crystal,were grown directly from untreated ZnSe polycrystals and two elements, respectively. The structure characters, purity and etch pit density were studied by rotating orientation XRD, PL spectrum and optical microscope. The contrastive investigation between two growth results indicated that the conical crystal was composed of (111) and (100) faces, and the flake crystal exhibited only (111) face. Moreover, the vicinal interface leaning to (111) face by the angle of 3.1° was the dominative growth face in vapor growth system, and growth occurs by layer-by-layer model. FWHM of RO-XRD pattern of ZnSe (111) face was 24sec for conical ZnSe crystal and 48s for ZnSe flake crystal. The results suggested that high-quality ZnSe crystals can be grown from the chemical vapor transport method with Zn(NH4)3Cl5 transport agent.


2018 ◽  
Vol 112 (26) ◽  
pp. 261901 ◽  
Author(s):  
Jie Xing ◽  
Xi Chen ◽  
Yuanyuan Zhou ◽  
James. C. Culbertson ◽  
Jaime A. Freitas ◽  
...  

2002 ◽  
Vol 719 ◽  
Author(s):  
K. Thonke ◽  
N. Kerwien ◽  
A. Wysmolek ◽  
M. Potemski ◽  
A. Waag ◽  
...  

AbstractWe investigate by photoluminescence (PL) nominally undoped, commercially available Zinc Oxide substrates (from Eagle Picher) grown by seeded chemical vapor transport technique in order to identify residual donors and acceptors. In low temperature PL spectra the dominant emission comes from the decay of bound exciton lines at around 3.36 eV. Zeeman measurements allow the identification of the two strongest lines and some weaker lines in-between as donorrelated. From the associated two-electron satellite lines binding energies of the major donors of 48 meV and 55 meV, respectively, can be deduced.


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