GaAs PN Diodes with Heavily Carbon-Doped P-Type GaAs Grown by MOMBE

1990 ◽  
Vol 29 (Part 2, No. 10) ◽  
pp. L1731-L1734 ◽  
Author(s):  
Shinji Nozaki ◽  
Ryuji Miyake ◽  
Takumi Yamada ◽  
Makoto Konagai ◽  
Kiyoshi Takahashi
Keyword(s):  
1995 ◽  
Vol 150 ◽  
pp. 221-226
Author(s):  
T. Tomioka ◽  
N. Okamoto ◽  
H. Ando ◽  
S. Yamaura ◽  
T. Fujii

2012 ◽  
Vol 249 (3) ◽  
pp. 459-463 ◽  
Author(s):  
Hideo Kawanishi ◽  
Tatsuya Tomizawa
Keyword(s):  

2011 ◽  
Vol 58 (5) ◽  
pp. 1302-1310 ◽  
Author(s):  
A Hokazono ◽  
H Itokawa ◽  
N Kusunoki ◽  
I Mizushima ◽  
S Inaba ◽  
...  

2003 ◽  
Vol 798 ◽  
Author(s):  
D. J. As ◽  
D. G. Pacheco-Salazar ◽  
S. Potthast ◽  
K. Lischka

ABSTRACTP-type doping of cubic GaN by carbon is reported with maximum hole concentration of 2 6.1×1018cm-3and hole mobility of 23.5 cm /Vs at room temperature, respectively. The cubic GaN:C was grown by rf-plasma assisted molecular beam epitaxy (MBE) under Ga-rich growth conditions on a semiinsulating GaAs (001) substrate (3 inches wafer). E-beam evaporation of a graphite rode with an C-flux of 1×1012cm-2s-1was used for C-doping of the c-GaN. Optical microscopy, Hall-effect measurements and photoluminescence were performed to investigate the morphological, electrical and optical properties of cubic GaN:C. Under Ga-rich growth conditions most part of the carbon atoms were incorporated substitutially on N-site giving p-type conductivity. Our results verify that effective p-type doping of c-GaN can be achieved under extrem Ga excess.


1991 ◽  
Vol 30 (Part 2, No. 9B) ◽  
pp. L1609-L1611 ◽  
Author(s):  
Jun-ichi Shirakashi ◽  
Takumi Yamada ◽  
Ming Qi ◽  
Shinji Nozaki ◽  
Kiyoshi Takahashi ◽  
...  

1996 ◽  
Vol 421 ◽  
Author(s):  
Wim Geerts ◽  
J.D. MacKenzie ◽  
C.R. Abernathy ◽  
S.J Pearton ◽  
Thomas Schmiedel

AbstractThe temperature dependence of the Hall voltage and resistivity of highly carbon doped GaN were measured. From the sign of the Hall voltage, the material appears to be p-type. Charge transport takes place in an impurity band and the valence band. The effective activation energy as estimated from the maximum in the temperature versus Hall voltage relation is 10–30 meV.


2009 ◽  
Vol 95 (13) ◽  
pp. 133103 ◽  
Author(s):  
T. S. Herng ◽  
S. P. Lau ◽  
C. S. Wei ◽  
L. Wang ◽  
B. C. Zhao ◽  
...  
Keyword(s):  

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