Hole trap generation by thermal treatment of nitrogen doped p-type ZnSe on GaAs characterized by deep level transient spectroscopy

1997 ◽  
Vol 71 (15) ◽  
pp. 2187-2189 ◽  
Author(s):  
K. Hellig ◽  
G. Prösch ◽  
M. Behringer ◽  
M. Fehrer ◽  
R. Beyer ◽  
...  
Keyword(s):  
Thermal Treatment ◽  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Hole Trap ◽  
Nitrogen Doped ◽  
Transient Spectroscopy ◽  
P Type

Defect States In p-ZnSe:N Grown By MOVPE

1996 ◽  
Vol 442 ◽  
Author(s):  
Shizuo Fujita ◽  
Ken-Ichi Ogata ◽  
Daisuke Kawaguchi ◽  
Zhi Gang Peng ◽  
Shigeo Fujita
Keyword(s):  
Vapor Phase ◽  
Deep Level Transient Spectroscopy ◽  
Annealing Temperature ◽  
Deep Level ◽  
Defect States ◽  
Nitrogen Doped ◽  
Activation Efficiency ◽  
Transient Spectroscopy ◽  
P Type

AbstractConcentration and origin of defect states in p-type nitrogen-doped ZnSe (p-ZnSe:N) grown by metalorganic vapor-phase epitaxy (MOVPE) are discussed by means of timeresolved photoluminescence and deep level transient spectroscopy. Thermal annealing, which is a useful tool for realizing p-type conductivity, results in deep defect states which seem to be associated with Zn vacancies and with nitrogen acceptors. By lowering the annealing temperature, the trap concentrations can be successfully reduced without seriously sacrificing the acceptor activation efficiency, although further reduction of Zn vacancies is pointed out as a remaining requirement for the improvement of quality of MOVPE-grown p-type layers.

scholarly journals Aluminum and Electron-Irradiation Induced Deep-Levels In N-Type And P-Type 6H-Sic

1998 ◽  
Vol 510 ◽  
Author(s):  
Min Gong ◽  
C. D. Beling ◽  
S. Fung ◽  
G. Brauer ◽  
H. Wirth ◽  
...  
Keyword(s):  
Electron Irradiation ◽  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Heavy Ion ◽  
Deep Levels ◽  
Hole Trap ◽  
Electron Traps ◽  
Transient Spectroscopy ◽  
P Type ◽  
Dlts Spectra

AbstractTwo deep levels, located at Ev+0.26eV and Ec-0.44eV, in Al-implanted n-type samples and one at Ev+0.48eV in p-type samples have been observed by the deep level transient spectroscopy. The level of is identified as the shallower aluminum-acceptor. The 1.7 MeV electron-irradiation, used as a probe to distinguish the implantation induced deep-levels, induces at least six electron traps in the n-SiC and one hole-trap in the p-type material. The peak positions of these deep-levels in DLTS spectra are quite different from those induced by Al-implantation. This result suggests that various damages are formed after heavy ion (Al) and light particle (e) irradiation.

scholarly journals Impact of Hydrogenation on Electrical Properties of NiSi2 Precipitates in Silicon

2005 ◽  
Vol 108-109 ◽  
pp. 279-284 ◽  
Author(s):  
O.F. Vyvenko ◽  
N.V. Bazlov ◽  
M.V. Trushin ◽  
A.A. Nadolinski ◽  
Michael Seibt ◽  
...  
Keyword(s):  
Electrical Properties ◽  
Deep Level Transient Spectroscopy ◽  
Molecular Hydrogen ◽  
Deep Level ◽  
Hydrogen Plasma ◽  
Extended Defects ◽  
Transient Spectroscopy ◽  
P Type ◽  
Plasma Hydrogenation ◽  
Type Sample

Influence of annealing in molecular hydrogen as well as of treatment in hydrogen plasma (hydrogenation) on the electrical properties of NiSi2 precipitates in n- and p-type silicon has been studied by means of deep level transient spectroscopy (DLTS). Both annealing and hydrogenation gave rise to noticeable changes of the shape of the DLTS-peak and of the character of its dependence on the refilling pulse duration that according to [1] allows one to classify the electronic states of extended defects as “band-like” or “localized”. In both n- and p-type samples DLTS-peak in the initial as quenched samples showed bandlike behaviour. Annealing or hydrogenation of n-type samples converted the band-like states to the localised ones but differently shifted the DLTS-peak to higher temperatures. In p-type samples, the initial “band-like” behaviour of DLTS peak remained qualitatively unchanged after annealing or hydrogenation. A decrease of the DLTS-peak due to precipitates and the appearance of the peaks due to substitutional nickel and its complexes were found in hydrogenated p-type sample after removal of a surface layer of 10-20µm.

Reactive-Ion-Etching Induced Deep Levels Observed in n-Type and p-Type 4H-SiC

2010 ◽  
Vol 645-648 ◽  
pp. 759-762
Author(s):  
Koutarou Kawahara ◽  
Giovanni Alfieri ◽  
Michael Krieger ◽  
Tsunenobu Kimoto
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Reactive Ion Etching ◽  
Deep Levels ◽  
Total Density ◽  
Ion Etching ◽  
Initial Concentration ◽  
Grown Sample ◽  
Transient Spectroscopy ◽  
P Type

In this study, deep levels are investigated, which are introduced by reactive ion etching (RIE) of n-type/p-type 4H-SiC. The capacitance of as-etched p-type SiC is remarkably small due to compensation or deactivation of acceptors. These acceptors can be recovered to the initial concentration of the as-grown sample after annealing at 1000oC. However, various kinds of defects remain at a total density of ~5× 1014 cm-3 in a surface-near region from 0.3 μm to 1.0 μm even after annealing at 1000oC. The following defects are detected by Deep Level Transient Spectroscopy (DLTS): IN2 (EC – 0.35 eV), EN (EC – 1.6 eV), IP1 (EV + 0.35 eV), IP2 (HS1: EV + 0.39 eV), IP4 (HK0: EV + 0.72 eV), IP5 (EV + 0.75 eV), IP7 (EV + 1.3 eV), and EP (EV + 1.4 eV). These defects generated by RIE can be significantly reduced by thermal oxidation and subsequent annealing at 1400oC.

Deep level transient spectroscopy on proton-irradiated Fe-contaminated p-type silicon

2012 ◽  
Vol 9 (10-11) ◽  
pp. 1992-1995 ◽  
Author(s):  
C. K. Tang ◽  
L. Vines ◽  
B. G. Svensson ◽  
E. V. Monakhov
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Type Silicon ◽  
Transient Spectroscopy ◽  
P Type

Investigation of the CaF2/p-type Si(100) interface by conductance and deep level transient spectroscopy

1991 ◽  
Vol 34 (8) ◽  
pp. 867-873 ◽  
Author(s):  
G. Couturier ◽  
H. Ricard ◽  
A. Thabti ◽  
A.S. Barrière ◽  
H. Ishiwara
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Transient Spectroscopy ◽  
P Type
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