W. Mtangi
University of Pretoria
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Featured researches published by W. Mtangi.
Journal of Applied Physics | 2010
Lasse Vines; Edouard Monakhov; R. Schifano; W. Mtangi; F.D. Auret; B. G. Svensson
Hydrothermal grown n-type ZnO samples have been investigated by deep level transient spectroscopy (DLTS), thermal admittance spectroscopy (TAS), temperature dependent Hall effect (TDH) measurements, and secondary ion mass spectrometry (SIMS) after thermal treatments up to 1500 °C, in order to study the electrical properties of samples with different lithium content. The SIMS results showed that the most pronounced impurities were Li, Al, Si, Mg, Ni, and Fe with concentrations up to ∼5×1017 cm−3. The Li concentration was reduced from ∼1017 cm−3 in as-grown samples to ∼1015 cm−3 for samples treated at 1500 °C, while the concentration of all the other major impurities appeared stable. The results from DLTS and TAS displayed at least five different levels having energy positions of Ec−20 meV, Ec−55 meV, Ec−0.22 eV, Ec−0.30 eV, and Ec−0.57 eV (Ec denotes the conduction band edge), where the Ec−55 meV level is the dominant freeze out level for conduction electrons in samples treated at temperatures <1300 °C, wh...
Journal of Applied Physics | 2012
W. Mtangi; F.D. Auret; W.E. Meyer; M. J. Legodi; P.J. Janse van Rensburg; Sergio M.M. Coelho; M. Diale; J.M. Nel
Effects of annealing ZnO in hydrogen, oxygen, and argon have been investigated using deep level transient spectroscopy (DLTS) and Laplace-DLTS (LDLTS) measurements. Current-voltage (IV) measurements indicate a decrease in zero–bias barrier height for all the annealed samples. Conventional DLTS measurements reveal the presence of three prominent peaks in the un-annealed and annealed samples. A new peak with an activation enthalpy of 0.60 eV has been observed in the H2 annealed samples, while an estimated energy level of 0.67 eV has been observed in Ar annealed samples. O2 annealing does not introduce new peaks but causes a decrease in the concentration of the E3 peak and an increase in concentration of the E1 peak. The concentrations of all the intrinsic defects have decreased after H2 and Ar annealing; with Ar annealing giving peaks with the lowest concentrations. The E2 peak anneals out after annealing ZnO in Ar and H2 at 300 °C. From the annealing behaviour of E3, we have attributed to transition metal ...
Journal of Applied Physics | 2009
R. Schifano; Edouard Monakhov; Lasse Vines; B. G. Svensson; W. Mtangi; F.D. Auret
Temperature dependent Hall (TDH) effect measurements have been performed on three virgin and hydrothermally grown ZnO samples with resistivities between ∼5 and ∼200 Ω cm at room temperature. The electrical conduction observed experimentally in the temperature range of 330–70 K can be accurately described by three donor levels with positions 41–48, 60–66, and ∼300 meV below the conduction band edge (EC) and an acceptor level in the lower part of the energy band gap (EG). Correlation of the TDH data with results from secondary ion mass spectrometry and admittance spectroscopy on the same samples suggests a rather firm association of the intermediate donor level with complexes involving Al impurities, while the shallowest one is tentatively ascribed to H-related centers. A large fraction of the deep donor remains nonionized in the temperature range studied and contributes substantially to the neutral-impurity-scattering of the conducting electrons. A detailed analysis of the TDH data, using the relaxation ti...
Journal of Applied Physics | 2011
W. Mtangi; F.D. Auret; P.J. Janse van Rensburg; Sergio M.M. Coelho; M. J. Legodi; J.M. Nel; W.E. Meyer; Albert Chawanda
very low reverse currents of the order of 10 � 10 A at a reverse voltage of 1.0 V whereas the e-beam deposited contacts have reverse currents of the order of 10 � 6 A at 1.0 V. Average ideality factors have been determined as (1.43 60.01) and (1.66 60.02) for the resistively evaporated contacts and e-beam deposited contacts, respectively. The IV barrier heights have been calculated as (0.721 60.002) eV and (0.624 60.005) eV for the resistively evaporated and e-beam deposited contacts, respectively. Conventional DLTS measurements reveal the presence of three prominent defects in both the resistive and e-beam contacts. Two extra peaks with energy levels of 0.60 and 0.81 eV below the conduction band minimum have been observed in the e-beam deposited contacts. These have been explained as contributing to the generation recombination current that dominates at low voltages and high leakage currents. Based on the reverse current at 1.0 V, the degree of rectification, the dominant current transport mechanism and the observed defects, we conclude that the resistive evaporation technique yields better quality Schottky contacts for use in solar cells and ultraviolet detectors compared to the e-beam deposition technique. The 0.60 eV has been identified as possibly related to the unoccupied level for the doubly charged oxygen vacancy, Vo 2þ . V C 2011 American Institute of Physics. [doi:10.1063/1.3658027]
Journal of Applied Physics | 2013
W. Mtangi; Matthias Schmidt; F.D. Auret; W.E. Meyer; P.J. Janse van Rensburg; M. Diale; Jackie M. Nel; A.G.M. Das; Francis Chi-Chung Ling; Albert Chawanda
We report on the space charge spectroscopy studies performed on thermally treated melt-grown single crystal ZnO. The samples were annealed in different ambients at 700 °C and also in oxygen ambient at different temperatures. A shallow donor with a thermal activation enthalpy of 27 meV was observed in the as-received samples by capacitance-temperature, CT scans. After annealing the samples, an increase in the shallow donor concentrations was observed. For the annealed samples, E27 could not be detected and a new shallow donor with a thermal activation enthalpy of 35 meV was detected. For samples annealed above 650 °C, an increase in acceptor concentration was observed which affected the low temperature capacitance. Deep level transient spectroscopy revealed the presence of five deep level defects, E1, E2, E3, E4, and E5 in the as-received samples. Annealing of the samples at 650 °C removes the E4 and E5 deep level defects, while E2 also anneals-out at temperatures above 800 °C. After annealing at 700 °C, t...
Journal of Applied Physics | 2012
W. Mtangi; F.D. Auret; M. Diale; W.E. Meyer; Albert Chawanda; H. de Meyer; P.J. Janse van Rensburg; J.M. Nel
We have systematically investigated the effects of high-temperature annealing on ZnO and ZnO devices using current voltage, deep level transient spectroscopy (DLTS) and Laplace DLTS measurements. Current–voltage measurements reveal the decrease in the quality of devices fabricated on the annealed samples, with the high-temperature annealed samples yielding devices with low barrier heights and high reverse currents. DLTS results indicate the presence of three prominent defects in the as-received samples. Annealing the ZnO samples at 300 °C, 500 °C, and 600 °C in Ar results in an increase in reverse leakage current of the Schottky contacts and an introduction of a new broad peak. After 700 °C annealing, the broad peak is no longer present, but a new defect with an activation enthalpy of 0.18 eV is observed. Further annealing of the samples in oxygen after Ar annealing causes an increase in intensity of the broad peak. High-resolution Laplace DLTS has been successfully employed to resolve the closely spaced ...
Physica B-condensed Matter | 2009
W. Mtangi; F.D. Auret; C. Nyamhere; P.J. Janse van Rensburg; A. Chawanda M. Diale
Physica B-condensed Matter | 2009
W. Mtangi; F.D. Auret; C. Nyamhere; P.J. Janse van Rensburg; Albert Chawanda; M. Diale; Jackie M. Nel; W.E. Meyer
Physica B-condensed Matter | 2012
Albert Chawanda; W. Mtangi; Francois D Auret; J.M. Nel; C. Nyamhere; M. Diale
Journal of Alloys and Compounds | 2010
Albert Chawanda; C. Nyamhere; F.D. Auret; W. Mtangi; M. Diale; J.M. Nel