Zinc Bis(Amide) Compounds Evaluated as Designed Precursors for Site-Selective P-type Doping of ZnSe

1995 ◽  
Vol 415 ◽  
Author(s):  
David A. Gaul ◽  
Oliver Just ◽  
William S. Rees

ABSTRACTZinc selenide doped with nitrogen deposited by organometallic vapor phase epitaxy (OMVPE) is one example which leads to a material that produces a blue emission. However, the effective incorporation of the nitrogen dopant into the zinc selenide lattice has not yet resulted in the demanded efficiency. One potential solution involves the design of a precursor introducing the nitrogen dopant bonded to zinc that survives the thermal decomposition process. Several new zinc bis(amide) compounds with the general formula Zn[N(R)(R′)]2 have been synthesized. Investigations into the thermal decomposition mechanisms of these compounds have provided insight into the potential usefulness of the designed precursor in the preparation of ZnSe:N.

1997 ◽  
Vol 484 ◽  
Author(s):  
M. L. Timmons ◽  
K. J. Bachmann

AbstractThis paper describes the application of organometallic vapor phase epitaxy to the growth of II-1V-V2 chalcopyrite materials that have high figures of merit for nonlinear optical (NLO) applications. ZnGeAs2, although not a particularly interesting NLO material, is used as a model for the growth of ZnGeP2, which is. Both compounds, as well as others, have been successfully grown by vapor phase on III-V substrates that provide a close lattice match. Doping studies using Group II and VI elements have been undertaken to control the p-type conductivity found in both compounds. Except for the possible case of indium, the results of these experiments are less than encouraging. Minority-carrier lifetimes of 150 ns have been measured in ZnGeAs2.The results of this work are used to make projections about the growth of CdGeAs2. CdGeAs2 is promising for the next generation of NLO mid-infrared materials if an absorption band that occurs at about 5 μm can be reduced. The growth projections suggest that this compound will be difficult to grow epitaxially and has no III-V substrate that provides a close lattice match. Mixing CdGeAs2 with other II-IV-V2 materials may offer solutions to the substrate problem. The defect properties of CdGeAs2 have not, to our knowledge, been studied.


1988 ◽  
Vol 131 ◽  
Author(s):  
R. Löckerath ◽  
H. J. Koss ◽  
P. Tommack ◽  
W. Richter ◽  
P. Balk

ABSTRACTThe thermal decomposition of AsH3 and TMG is measured insitu under different experimental conditions. Simultaneously the production of H2, CH4 and C2H6 is observed. The data indicate a situation where AsH3 is only partially decomposed at the GaAs surface. The hydrogen released removes additional CH3 groups from the trimethyl-gallium (TMG) molecule, enhances the decomposition of TMG, and thereby forms methane.


1997 ◽  
Vol 484 ◽  
Author(s):  
C. A. Wang ◽  
H. K. Choi ◽  
D. C. Oakley ◽  
G. W. Charache

AbstractThe effect of substrate misorientation on the growth of GaInAsSb was studied for epilayers grown lattice matched to GaSb substrates by low-pressure organometallic vapor phase epitaxy. The substrates were (100) misoriented 2 or 6° toward (110), (111)A, or (111)B. The surface is mirror-like and featureless for layers grown with a 6° toward (111)B misorientation, while a slight texture was observed for layers grown on all other misorientations. The optical quality of layers, as determined by the full width at half-maximum of photoluminescence spectra measured at 4K, is significantly better for layers grown on substrates with a 6° toward (111)B misorientation. The incorporation of Zn as a p-type dopant in GaInAsSb is about 1.5 times more efficient on substrates with 60 toward (111)B misorientation compared to 2° toward (110) misorientation. The external quantum efficiency of thermophotovoltaic devices is not, however, significantly affected by substrate misorientation.


1990 ◽  
Vol 216 ◽  
Author(s):  
K.K. Parat ◽  
N.R. Taskar ◽  
H. Ehsani ◽  
I.B. Bhat ◽  
S.K. Ghandri

ABSTRACTHg1-xCdxTe layers, grown by the organometallic vapor phase epitaxy (OMVPE), are p-type with carrier concentrations around 4 × 1016/cm3 due to the Group II vacancies in them. Following a Hg saturated anneal at 220°C, these layers become n-type with carrier concentrations around 4 × 1014/cm3. In order to fabricate p-n junction diodes, Hg1-xCdxTe layers were grown with a 0.5–0.8 μm thick CdTe cap. By opening windows in this CdTe cap, the underlying Hg1-xCdxTe Te layer was annealed in a selective manner, thus forming planar p-n junctions. The CdTe cap, which is used as the diffusion barrier for Hg during the selective anneal, also served as the junction passivant for the photodiodes. Details of device fabrication and characterization are presented in this paper.


2011 ◽  
Vol 1342 ◽  
Author(s):  
Jonathan Poplawsky ◽  
Nathaniel Woodward ◽  
Atsushi Nishikawa ◽  
Yasufumi Fujiwara ◽  
Volkmar Dierolf

ABSTRACTIn-situdoped Eu ions in GaN grown by Organometallic Vapor-phase Epitaxy (OMVPE) at different pressures were investigated under different excitation methods and through the use of the following experimental techniques: (1) resonant site-selective laser irradiation (2) electron beam excitation, and (3) a dual excitation using a combination of electron beam and laser irradiation. With these means, we have examined the difference in the excitation pathways that result from resonant laser and electron hole (e-h) pair excitation of Eu ions for two different distinct incorporation sites, which are responsible for most of the luminescence. We have obtained clear evidence that e-h pairs do not have the ability to excite all of the ions and that there is excitation trapping by defects involved in the Eu excitation.


1988 ◽  
Vol 86 (1-4) ◽  
pp. 228-232 ◽  
Author(s):  
N.R. Taskar ◽  
V. Natarajan ◽  
I.B. Bhat ◽  
S.K. Grandhi

2016 ◽  
Vol 75 (3) ◽  
pp. 279-284 ◽  
Author(s):  
V. P. Makhniy ◽  
O. V. Kinzersky ◽  
I. M. Senko
Keyword(s):  

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