Electrical Characterization Of Defects Introduced During Plasma-Based Processing Of GaAs

1996 ◽  
Vol 442 ◽  
Author(s):  
F. D. Auret ◽  
G. Myburg ◽  
W. E. Meyer ◽  
P. N. K. Deenapanray ◽  
H. Nordhoff ◽  
...  

AbstractDLTS revealed that each plasma type (He and SiCl4) introduced its own characteristic set of defects. Some of the defects created during He processing and one defect introduced by SiCl4 etching had identical electronic properties to those introduced during high energy (MeV) He ion bombardment. SiC14etching introduced only two prominent defects, one of which is metastable with electronic properties similar to a metastable defect previously reported in high and low energy He-ion bombardment of Si-doped GaAs. IV measurements demonstrated that the characteristics of SBDs fabricated on He-ion processed surfaces were very poor compared to those of control diodes (diodes fabricated on surfaces cleaned by conventional wet etching). In contrast, the properties of SBDs fabricated on SiCl4 etched surfaces were as good as, and in some cases superior to, those of control diodes. SBDs fabricated on annealed (at 450°C for 30 minutes) He-processed samples exhibited improved but still poor rectification. In contrast, SBDs fabricated on annealed SiCl4 etched surfaces had virtually the same characteristics as those fabricated on unannealed SiCl4 etched samples.

1998 ◽  
Vol 537 ◽  
Author(s):  
S. A. Goodman ◽  
F. D. Auret ◽  
F. K. Koschnick ◽  
J.-M. Spaeth ◽  
B. Beaumont ◽  
...  

AbstractWe report on the electrical properties of defects as determined by deep level transient spectroscopy (DLTS) introduced in epitaxially grown n-GaN by 2.0 MeV protons and 5.4 MeV He-ions. After He-ion bombardment three electron traps ER3 (Ec - 0.196 eV), ER4 (Ec - 0.78 eV), and ER5 (Ec - 0.95 eV) were introduced uniformly in the region profiled by DLTS with introduction rates of 3270 ± 200, 1510 ± 300, and 3030 ± 500 cm-1 respectively. Capture cross section measurements revealed that the electron capture kinetics of ER5 is similar to that of a line defect. A defect with similar electronic properties as ER3 is observed after 2.0 MeV proton irradiation. The emission rate of ER3 depends on the electric field strength in the space-charge region. This emission rate is modelled according to the Poole-Frenkel distortion of a square well with a radius of 20 ± 2 Å or alternatively, a Gaussian well with a characteristic width of 6.0 ± 1 Å. Hence, we conclude that ER1 is a point defect which appears to have an acceptor like character. Two additional electron traps, ER1 (Ec -0.13 eV) and ER2 (Ec - 0.16eV) with introduction rates of 30 ± 10 and 600 ± 100 cm-1 not thusfar observed after electron or He-ion bombardment were observed after proton irradiation.


1999 ◽  
Vol 4 (S1) ◽  
pp. 606-611 ◽  
Author(s):  
S. A. Goodman ◽  
F. D. Auret ◽  
F. K. Koschnick ◽  
J.-M. Spaeth ◽  
B. Beaumont ◽  
...  

We report on the electrical properties of defects as determined by deep level transient spectroscopy (DLTS) introduced in epitaxially grown n-GaN by 2.0 MeV protons and 5.4 MeV He-ions. After He-ion bombardment three electron traps ER3 (Ec − 0.196 eV), ER4 (Ec − 0.78 eV), and ER5 (Ec − 0.95 eV) were introduced uniformly in the region profiled by DLTS with introduction rates of 3270 ± 200, 1510 ± 300, and 3030 ± 500 cm−1 respectively. Capture cross section measurements revealed that the electron capture kinetics of ER5 is similar to that of a line defect. A defect with similar electronic properties as ER3 is observed after 2.0 MeV proton irradiation. The emission rate of ER3 depends on the electric field strength in the space-charge region. This emission rate is modelled according to the Poole-Frenkel distortion of a square well with a radius of 20 ± 2 Å or alternatively, a Gaussian well with a characteristic width of 6.0 ± 1 Å. Hence, we conclude that ER1 is a point defect which appears to have an acceptor like character. Two additional electron traps, ER1 (Ec −0.13 eV) and ER2 (Ec − 0.16eV) with introduction rates of 30 ± 10 and 600 ± 100 cm−1 not thusfar observed after electron or He-ion bombardment were observed after proton irradiation.


1998 ◽  
Vol 510 ◽  
Author(s):  
P.N.K. Deenapanray ◽  
F.D. Auret ◽  
M.C. Ridgway ◽  
S.A. Goodman ◽  
G. Myburg

AbstractWe report on the electrical properties of defects introduced in epitaxially grown n-Si by 1 keV He-, Ne-, and Ar-ion bombardment. Epitaxial layers with different O contents were used in this study. We demonstrate using deep level transient spectroscopy that the low energy ions introduced a family of similarly structured defects (DI) with electronic levels at ∼0.20 eV below the conduction band. The introduction of this set of identical defects was not influenced by the presence of O. Ion bombardment of O-rich Si introduced another family of prominent traps (D2) with levels close to the middle of the band gap. Both sets of defects were thermally stable up to ∼400 °C, and their annealing was accompanied by the introduction of a family of secondary defects (D3). The “D3” defects had levels at ∼0.21 eV below the conduction band and were thermally stable at 650 °C. We have proposed that the “DI”, “D2”, and “D3” defects are higherorder vacancy clusters (larger than the divacancy) or complexes thereof.


2011 ◽  
Vol 406 (20) ◽  
pp. 3876-3884 ◽  
Author(s):  
G.M. Zhao ◽  
Y.Q. Yang ◽  
W. Zhang ◽  
X. Luo ◽  
R.J. Zhang ◽  
...  

1997 ◽  
Vol 70 (1) ◽  
pp. 69-71 ◽  
Author(s):  
J. Gerster ◽  
J. M. Schneider ◽  
C. Ehret ◽  
W. Limmer ◽  
R. Sauer ◽  
...  

2015 ◽  
Vol 70 (1) ◽  
pp. 10102
Author(s):  
Simeon Simeonov ◽  
Silvia Bakalova ◽  
Anna Szekeres ◽  
Ivaylo Minkov ◽  
Gabriel Socol ◽  
...  

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