Room-temperature near-band-edge photoluminescence from CuInSe2 heteroepitaxial layers grown by metalorganic vapor phase epitaxy

1997 ◽  
Vol 70 (14) ◽  
pp. 1840-1842 ◽  
Author(s):  
Shigefusa Chichibu
2000 ◽  
Vol 5 (S1) ◽  
pp. 675-681
Author(s):  
P. Li ◽  
S. J. Chua ◽  
M. Hao ◽  
W. Wang ◽  
X. Zhang ◽  
...  

InGaN thin films were grown by low-pressure metalorganic-vapor-phase-epitaxy (MOVPE) and characterized by cathodoluminescence (CL) and scanning electron microscopy (SEM). SEM images showed that InGaN samples have inverted hexagonal pits which are formed by the In segregation on the (1011) surfaces. Room temperature CL at the wavelengths corresponding to the GaN band edge, the In-poor and In-rich regions showed that the In–rich regions formed at the periphery of the hexagonal pits.


1999 ◽  
Vol 595 ◽  
Author(s):  
P. Li ◽  
S. J. Chua ◽  
M. Hao ◽  
W. Wang ◽  
X. Zhang ◽  
...  

AbstractInGaN thin films were grown by low-pressure metalorganic-vapor-phase-epitaxy (MOVPE) and characterized by cathodoluminescence (CL) and scanning electron microscopy (SEM). SEM images showed that InGaN samples have inverted hexagonal pits which are formed by the In segregation on the (1011) surfaces. Room temperature CL at the wavelengths corresponding to the GaN band edge, the In-poor and In-rich regions showed that the In–rich regions formed at the periphery of the hexagonal pits.


2006 ◽  
Author(s):  
Yasuyuki Kobayashi ◽  
Hiroki Hibino ◽  
Tomohiro Nakamura ◽  
Tetsuya Akasaka ◽  
Toshiki Makimoto ◽  
...  

2003 ◽  
Vol 83 (10) ◽  
pp. 1921-1922 ◽  
Author(s):  
R. P. Green ◽  
A. Krysa ◽  
J. S. Roberts ◽  
D. G. Revin ◽  
L. R. Wilson ◽  
...  

1999 ◽  
Vol 573 ◽  
Author(s):  
Jingxi Sun ◽  
F. J. Himpsel ◽  
A. B. Ellis ◽  
T. F. Kuech

ABSTRACTAn ammonia-based, in situ passivation of GaAs surfaces conducted within a metalorganic vapor phase epitaxy reactor is present. The shift of the GaAs surface Fermi level, and hence the surface charge density, resulting from this in situ passivation, has been studied using photoreflectance (PR) spectroscopy. Samples consisting of an undoped GaAs layer on highly doped n-GaAs (UN+) and p-GaAs (UP+) structures allow for the exact determination of the surface Fermi level position using PR These structures were grown by MOVPE and in situ thermal nitridation was performed after growth within the MOVPE system without exposure to the air. After nitridation, the surface Fermi level can be shifted by ∼ 0.23 eV towards the conduction band edge for UN+ structures and by ∼ 0.11 eV towards the valence band edge for UP+ structures from the normally mid-gap ‘pinned’ positions.


2017 ◽  
Vol 464 ◽  
pp. 211-214 ◽  
Author(s):  
Ryosuke Hasegawa ◽  
Akira Yoshikawa ◽  
Tomohiro Morishita ◽  
Yoshitaka Moriyasu ◽  
Kazuhiro Nagase ◽  
...  

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