Native defect compensation in III-antimonide bulk substrates

Author(s):  
R. Pino ◽  
Youngok Ko ◽  
P.S. Dutta
Keyword(s):  
1995 ◽  
Vol 395 ◽  
Author(s):  
X. Zhang ◽  
P. Kung ◽  
D. Walker ◽  
A. Saxler ◽  
M. Razeghi

ABSTRACTWe report the growth and photoluminescence characterization of GaN grown on different substrates and under different growth conditions using metalorganic chemical vapor deposition. The deep-level yellow luminescence centered at around 2.2eV is attributed to native defect, most possibly the gallium vacancy. The yellow luminescence can be substantially reduced By growing GaN under Ga-rich condition or doping GaN with Ge or Mg.


1993 ◽  
Vol 48 (23) ◽  
pp. 17595-17598 ◽  
Author(s):  
H. Jia ◽  
J. Shinar ◽  
D. P. Lang ◽  
M. Pruski

1990 ◽  
Vol 216 ◽  
Author(s):  
M.A. Berding ◽  
A. Sher ◽  
A.-B. Chen

ABSTRACTNative point defects play an important role in HgCdTe. Here we discuss some of the relevant mass action equations, and use recently calculated defect formation energies to discuss relative defect concentrations. In agreement with experiment, the Hg vacancy is found to be the dominant native defect to accommodate excess tellurium. Preliminary estimates find the Hg antisite and the Hg interstitial to be of comparable densities. Our calculated defect formation energies are also consistent with measured diffusion activation energies, assuming the interstitial and vacancy migration energies are small.


2006 ◽  
Vol 527-529 ◽  
pp. 717-720 ◽  
Author(s):  
Sashi Kumar Chanda ◽  
Yaroslav Koshka ◽  
Murugesu Yoganathan

A room temperature PL mapping technique was applied to establish the origin of resistivity variation in PVT-grown 6H SiC substrates. A direct correlation between the native defect-related PL and resistivity was found in undoped (V-free) samples. In vanadium-doped samples with low vanadium content, the resistivity showed a good correlation with the total PL signal consisting of contributions from both vanadium and native point defects. Well-known UD1 and UD3 levels were revealed by low-temperature PL spectroscopy. Some correlation was observed between these low-temperature PL signatures and the resistivity distribution.


2005 ◽  
Vol 97 (12) ◽  
pp. 123509 ◽  
Author(s):  
M. E. Zvanut ◽  
Haiyan Wang ◽  
Mpumelelo Richards ◽  
V. V. Konovalov
Keyword(s):  

1993 ◽  
Vol 16 (1-3) ◽  
pp. 215-218 ◽  
Author(s):  
P. Höschl ◽  
R. Grill ◽  
J. Franc ◽  
P. Moravec ◽  
E. Belas
Keyword(s):  

2001 ◽  
Vol 40 (Part 1, No. 5A) ◽  
pp. 3089-3092 ◽  
Author(s):  
Tamotsu Okamoto ◽  
Shinji Kitamoto ◽  
Akira Yamada ◽  
Makoto Konagai

2001 ◽  
Vol 692 ◽  
Author(s):  
V. A. Kasiyan ◽  
R. Z. Shneck ◽  
Z. M. Dashevsky ◽  
S. R. Rotman

AbstractElectrical and optical measurements obtained with CdSe single crystals doped with chromium from a gas source CrSe over a wide temperature range (500–1050 °C) are compared with ZnSe annealed in liquid metal (Zn). These processes are intended to control the concentrations of the impurity and intrinsic defects. The low temperature annealing of CdSe crystals in CrSe atmosphere allows obtaining high electron mobility up to 9000 cm2/Vs at 80 K and demonstrates the low native defect concentration. A high temperature annealing gives rise to increased electron concentration with decreased mobility. Optical absorption measurements show that at the high annealing temperature effective doping with Cr takes place. The impurity absorption beyond the absorption edge is interpreted by the excitation of Cr++ and Cr+ deep levels


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