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Defect structure and deformation of gallium arsenideLaister, David January 1969 (has links)
No description available.
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On the electrical characterisation of bulk and epitaxial n-type Te doped GaSbMurape, Davison Munyaradzi January 2014 (has links)
Since the development of the transistor in the Bell Telephone Laboratories in 1948 [78], the semiconductor industry has transformed the world we live in. It is difficult to picture a world without the modern day cutting edge technology. Imagine performing every day functions without “trivial” devices such as computers, cell phones or microwave ovens. The ability to tailor the band gaps of various binary, ternary and quaternary semiconductor systems has opened up a whole new spectrum of potential purpose designed devices [27]. This thesis focuses on the electronic properties of gallium (III) antimonide (V). The antimonides, in general, have the smallest band gap and highest electron mobility of the III-V compound semiconductors and are well suited for long wavelength emission and detection as well as high frequency switching device applications. Furthermore, III-V ternaries and quaternaries, such as (AlGaIn)(AsSb), lattice matched to gallium antimonide (GaSb) are considered serious competitors for HgCdTe and PbSe in long-wavelength infrared (LWIR) and very long-wavelength infrared (VLWIR) technology [4, 10, 11]. Epitaxial material systems based on GaSb are suitable for a wide range of applications such as missile and surveillance systems and a host of other military and civil applications. In addition, an assortment of devices on InAs, GaSb, and AlSb, including resonant tunnelling devices, infrared detectors and mid-infrared semiconductor lasers have been demonstrated [14, 15]. Furthermore, antimonide based devices could potentially reduce optical fibre power loss by a few orders of magnitude, as their implementation can lead to use of non-silica based optical fibres that minimise Raleigh scatter related power loss [8]. GaSb related technology faces a number of challenges. A significant amount of effort is required to exploit the potential it offers. GaSb oxidises readily in the ambient, resulting in the formation of a native oxide layer as well as deposits of elemental antimony (Sb) at the oxide/substrate interface therefore it has poor surface electronic properties resulting from high surface state densities[4, 17, 18]. As grown GaSb is characterised by a high density of surface states of which many are classified as non-radiative (Auger) recombination centres. The elemental Sb layer constitutes an unwanted conduction path parallel to the active surface region [17]. The potential that GaSb and GaSb-based strained layer superlattices offer as successors to the current generation of LWIR and VLWIR optoelectronic materials has therefore been largely impeded [4]. Furthermore, processing steps in device fabrication leads to an unintentionally damaged GaSb surface exacerbating the situation. Any efforts to engineer devices of superior quality on GaSb have to address these and more material specific problems [19]. This study attempts to contribute towards an improved understanding of the structural and electrical properties of the near surface region of Te-doped bulk (100) and MOVPE grown epitaxial Te doped n- GaSb. The main focus of this study is to develop means to de-oxidise and stabilize the highly reactive GaSb surface and to develop diode structures to demonstrate the improved interface characteristics and use related current–voltage (I-V) measurements to quantify the surface state density before and after treatment. These devices were also used to probe the near surface region for electrically active deep level defects that often act as non-radiative recombination centers. Au, Pd and Al were used as metals to establish a metal semiconductor barrier and subsequent depletion region. Sulphur based chemicals, ([(NH4)2S / (NH4)2SO4] + S), not previously reported for the treatment of (100) n-GaSb surfaces, and the commonly used passivants Na2S:9H2O and (NH4)2S were compared by assessing the electrical and structural properties both before and after treatment. The effect of treatment on the electrical response of the material was determined using current-voltage, capacitance-voltage (C-V) and deep level transient spectroscopy (DLTS) measurements, while the surface morphology and composition were studied by SEM, AES and XPS.
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Radiation damage in GaAs and SiCJanse van Vuuren, Arno January 2011 (has links)
In this dissertation the microstructure and hardness of phosphorous implanted SiC and neutron irradiated SiC and GaAs have been investigated. SiC is important due to its application as a barrier coating layer in coated particle fuel used in high temperature gas cooled reactors. The characterisation of neutron irradiated GaAs has been included in this study in order to compare the radiation damage produced by protons and neutrons since proton bombardment of SiC could in principle be used for out-of-reactor simulations of the neutron irradiation damage created in SiC during reactor operation. The following SiC and GaAs compounds were investigated: As-implanted and annealed single crystal 6H-SiC wafers and polycrystalline 3C-SiC bulk material implanted with phosphorous ions. As-irradiated and annealed polycrystalline 3C-SiC bulk material irradiated with fast neutrons. As-irradiated and annealed single crystal GaAs wafers irradiated with fast neutrons. The main techniques used for the analyses were transmission electron microscopy (TEM) and nano-indentation hardness testing. The following results were obtained for the investigation of implanted and irradiated SiC and GaAs: Phosphorous Implanted 6H-SiC and 3C-SiC The depth of the P+ ion damage was found to be in good agreement with predictions by TRIM 2010. Micro-diffraction of the damage region in P+ implanted 6H-SiC (dose 5×1016 ions/cm2) indicates that amorphization occurred and that recrystallisation of this layer occurred during annealing at 1200°C. TEM analysis revealed that the layer recrystallised in the 3C phase of SiC and twin defects also formed within the layer. Micro-diffraction of the damage region in P+ implanted 3C-SiC (dose 1×1015 ions/cm2) indicates that amorphization also occurred for this sample and that recrystallisation of this layer occurred during annealing at 800°C. Nano-hardness testing of the P+ implanted 6H-SiC indicated that the hardness of the implanted SiC was initially much lower than unimplanted SiC due to the formation of an amorphous layer during ion implantation. After annealing the implanted SiC at 800°C and 1200°C, the hardness increased due to re-crystallisation and point defect hardening. Neutron Irradiated 3C-SiC TEM investigations of neutron irradiated 3C-SiC revealed the presence dark spot defects for SiC samples irradiated to a dose of 5.9×1021 n/cm2 and 9.6×1021 n/cm2. Neutron Irradiated GaAs TEM investigation revealed a high density of dislocation loops in the unannealed neutron irradiated GaAs. The loop diameters increased after post-irradiation annealing in the range 600 to 800 °C. The dislocation loops were found to be of interstitial type lying on the {110} cleavage planes of GaAs. This finding is in agreement with earlier studies on 300 keV proton bombarded and 1 MeV electron irradiated GaAs where interstitial loops on {110} planes became visible after annealing at temperatures exceeding 500 °C. The small dislocation loops on the {110} planes of the neutron irradiated GaAs transformed to large loops and dislocations after annealing at 1000 °C.
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Studies of scandium-germanium systems and studies of zinc and selenium doped gallium arsenideDell'Oca, Conrad Joseph January 1965 (has links)
This investigation is concerned with a study of the properties of scandium-germanium systems, and a study of the properties of selenium and zinc doped gallium arsenide„
In part one the physical properties of scandium and germanium are used to empirically estimate the relative solubility of scandium in germanium. It was shown that scandium and germanium are miscible in the liquid phase and that scandium has a very low solid solubility in germanium.
Crystals of scandium-doped germanium were grown and analyzed using Hall constant and resistivity measurements from liquid nitrogen temperature to room temperature. The results show that the crystals grown are p-type, but that this behaviour cannot be completely attributed to scandium. However, it was shown that if scandium does not form compounds on crystal growth, it has a maximum solubility in germanium of less than one part per million.
Methods for analysing the results of experimental measurements, to determine the concentration of acceptors, donors and free carriers, and the ionization energies are given.
In part two the properties of selenium and zinc doped gallium arsenide were studied, again using resistivity and Hall measurements. Selenium and zinc were determined to be shallow donors and acceptors respectively. The concentration of the impurities present were determined and the properties of the material were discussed. / Science, Faculty of / Physics and Astronomy, Department of / Graduate
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Characterization of semi-insulating liquid encapsulated Czochralski gallium arsenideHui, David C. W. January 1989 (has links)
This thesis consists of a study of several qualification techniques for SI LEC GaAs and the application of these techniques to various ingots.
For use on the starting material before any doping procedures, the technique of studying the semi-insulating properties by monitoring the activation energy of dark resistivity with temperature was investigated. Experiments were performed on both ring dot as well as cloverleaf samples. Different activation energies for the dark resistivity were observed for temperatures above and below 290 K. Also, ingots with different background impurity concentrations were tested.
Another technique applicable to the undoped starting material is Optical Transient Current Spectroscopy (OTCS). The occurrence of 'negative' peaks was simulated using a depletion layer model. The results showed that under certain conditions a recombination centre can produce a positive peak, a negative peak, or both a positive and a negative peak. Further analysis of the negative peaks led to the formulation of a field enhanced injection model to explain their occurrence. More than one negative peak was observed experimentally. In addition, the effect of different electrode structures on OTCS experiments was investigated. The effect of polarity on negative peaks was studied using ring dot structures and was found to agree with the proposed model.
Some peculiar anomalies which were observed in investigating OTCS led to the discovery of a photocurrent memory effect with decay time constants of the order of minutes at a temperature of 266 K. This memory effect was found to be associated with surface modifications. The effects of surface passivation with Na₂S were investigated. The method of normalizing the OTCS peak height with photocurrent was investigated.
A microscopic spatial analysis tool, scanning OTCS, with a spot size of about 2 µm was developed in order to probe the spatial variation of deep levels and compare with that of dislocations or other defects. An experiment on an abraded surface was performed using the scanning OTCS and showed that the negative peak does indeed correlate with mechanical damage.
Wafer performance during implantation doping is an important qualification test. Comparisons between standard furnace annealing and rapid thermal annealing were performed. A comparison of the estimated percentage activation using C(V) measurements with that from Hall measurements, with and without a correction for the surface depleted region, was performed. The C(V) analysis technique, used in the industry to obtain doping profiles of implanted wafers, was studied. The effect of using serial and parallel measurement modes was investigated. Simulations of C(V) measurements on implanted devices by solving the Poisson-Boltzmann equation for the charge distribution under different biases were performed. The limitation of the C(V) profiling technique in detecting sharp dopant profiles was investigated. A system for quick analysis of the percentage of activation using a mercury probe was designed. The effect of serial and parallel analysis of the impedance measured by the mercury probe on the estimated dopant profile was investigated. The effect of different electrode structures (Schottky to Schottky as compared to Schottky to Ohmic) on estimated doping profiles was studied.
The mobility profile as a tool for qualification was investigated. The effect of surface states on mobility was studied.
A crucial factor in wafer qualification is the uniformity of transistor characteristics across the wafer. In order to test this on a wafer, thousands of transistors have to be measured. A technique of perforating measurements automatically with
consistency is needed. An automatic probing station for measuring large arrays of transistors was engineered. Tests on arrays of transistors were performed to investigate the effect of different fabrication processes, in particular the amount of surface etch, on the uniformity of threshold voltage. / Applied Science, Faculty of / Electrical and Computer Engineering, Department of / Graduate
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The effect of short term anneals on the cathodoluminescence of GaAsThird, Christine Elizabeth January 1990 (has links)
This study examines the effect of furnace annealing and rapid thermal annealing (RTA) on the room-temperature cathodoluminescence (CL) image of liquid encapsulated Czochralski (LEC) GaAs substrates. Furnace annealed samples were heated in a tube furnace for 20 minutes at temperatures from 600 to 950 °C. RTA annealed samples were heated in a commercial RTA furnace for 5 s at temperatures from 650 to 950 °C. The times used for both methods are typical of those used for post-ion implantation annealing although selected samples were RTA annealed at times from 10 to 160 s. The temperature range examined has been extended beyond typical post-ion implantation anneal temperatures to investigate the effect of temperature on the substrate. Examination of RTA annealed GaAs using CL has not been reported previous to this investigation.
The CL images of the annealed samples are compared with those of the as-received (un-annealed) material. The CL images of the LEC GaAs wafers prior to annealing have dark spots which correspond to the location of dislocations with regions of higher CL intensity surrounding them. These regions of higher CL intensity are referred to as 'halos'. The remaining material has a CL intensity lower than these halos. The dislocations in LEC GaAs form into cellular networks to reduce the strain energy in the crystal. When viewed at low magnification the overlap of the halos makes the cell walls appear bright and the cell interiors appear dark in a CL image.
The furnace annealed substrates show an increase in CL intensity in the interior of the cells. The halos are still present at the cell walls but a region of low CL intensity persists outside the halos making the cell walls appear dark with a brighter interior. This behaviour was seen in all the furnace annealed material although the contrast decreases with increasing anneal temperature.
The RTA anneal samples show similar behaviour to the furnace annealed samples at temperatures below 800 °C. Above this temperature the halos are no longer noticeable in the surface CL images, although the region of lower CL intensity can be seen along some cell walls. When a cleaved cross-section is examined using CL, there are regions of higher CL intensity adjacent to both surfaces. These regions typically extend from 100 to 200 μm in from the surface and are nearly uniform in depth. The centre region of the sample appeared the same as the as-received material with dislocation spots, surrounding halos and low CL intensity in the interiors of the cells.
The bright regions seen in the cross-section CL images of the RTA samples were examined using photoluminescence at liquid helium temperatures. This investigation found a correlation between the bright regions and the presence of Cu. In addition, the amount of residual Cu on the surface has a significant affect on the depth of the bright bands. Low residual Cu levels results in shallower band depths than high residual Cu levels. It is proposed that the presence of the Cu acts to increase the recombination rate thus increasing the brightness of the CL image. / Applied Science, Faculty of / Materials Engineering, Department of / Graduate
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Reactions of the {100} face of gallium arsenide with molecular and atomic bromineSalusbury, Ian McKenzie January 1990 (has links)
The reaction of gallium arsenide {100} with molecular and atomic bromine was studied at temperatures between 100 and 225°C and at pressures of bromine between 0.1 and 40 Torr. Samples of GaAs were placed on a silicon platform within a Pyrex reactor flow system and the etch rate was determined by profilometry or weight change of the sample. Atomic bromine was produced by a 2450 MHz microwave discharge and the samples were etched downstream. The atomic concentration was measured by an isothermal calorimetric detector.
Pressure dependence studies for molecular Br₂ etching showed that below 1-2 Torr of bromine, a first order reaction was rate-limiting whereas above this pressure a half order reaction was rate-limiting. Temperature dependence studies for the low pressure and high pressure regimes gave activation energies and pre-exponential values for the two respective rate controlling reactions. The first order reaction was found to have an activation energy of 29.2 ±4.0 kJ mol⁻¹ and a pre-exponential value of (3.4 ± 4.4) x 10²¹ molecule cm⁻² s⁻¹ Torr⁻¹. The activation energy for the half order reaction was found to be 8.4 ± 0.7 kJ mol⁻¹ with a pre-exponential of (6.4 ± 1.3) x 10¹⁸ molecule cm⁻² s⁻¹ Torr⁻¹⁄².
The activation energy for atomic etching was calculated to be 12.9 ± 0.9 kJ mol⁻¹ and the pre-exponential, (7.1 ± 2.0) x 10²⁰ atom cm⁻² s⁻¹ Torr⁻¹. / Science, Faculty of / Chemistry, Department of / Graduate
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Radiative heat transfer in gallium arsenide lec crystal pullersBakeer, Muna January 1990 (has links)
A numerical analysis of radiative heat transfer in a liquid encapsulant Czochralski gallium arsenide crystal puller is developed. The heat transfer and equivilent ambient temperature
of each surface element are calculated using the Gebhart radiative model. The effective ambient temperature, to which each surface element is radiating, is found to vary indicating that assuming a constant ambient temperature for all surfaces (simplified radiative model) is incorrect.
The importance of including the middle and top cylinders of the growth chamber in numerical analysis of radiative heat transfer in the system is evaluated in the study. The upper section could be replaced by one isothermal surface without significant change of the effective ambient temperature distribution.
Fluid flow and heat transfer in the GaAs melt, crystal and encapsulant are calculated
using a three dimensional axisymmetric finite difference code which includes the detailed radiative model. The mathematical modelling of the fluid and heat flow describes
steady state transport phenomena in a three dimensional solution domain with latent heat release at the liquid/solid interface.
The predicted flow and temperature fields using the detailed radiative model differ considerably from the predicted fields using the simplified model. The simplified model shows high axial and low radial temperature gradients in the crystal near the encapsulant region; the axial gradient decreases and the radial gradient increases with increasing distance from the encapsulant top. The detailed model shows a high radial temperature gradient in the crystal near the crystal-encapsulant-ambient junction and nearly flat isotherms in the top half of the crystal. / Applied Science, Faculty of / Mechanical Engineering, Department of / Graduate
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Semi-insulating gallium arsenide-deep trapping levels, dislocations and backgatingTang, Wade Wai Chung January 1984 (has links)
Work is reported on three topics relating to problems which hold back the development of GaAs integrated circuits. These topics are deep trapping levels in the starting semi-insulating GaAs, the effect of dislocations on device characteristics, and backgating. (The latter is the influence of voltages on nearby contacts on device performance).
Deep trapping levels in undoped semi-insulating liquid-encapsulated— Czochralskl GaAs grown in the <100> direction were characterized using photocurrent deep level transient spectroscopy (photocurrent-DLTS). Three electron levels were found using photocurrent-DLTS in the temperature range 200K to 400K. By using Cr electrodes, instead of Au-Ge electrodes, it became possible to extend the experiment to a higher temperature range than previously used in this laboratory, and hence to observe the trap known as EL2. This trap has not previously been observed in undoped liquid-encapsulated-Czochralski GaAs by using photocurrent-DLTS.
The possibility of an effect of dislocations on device characteristics was investigated using a dislocation etch procedure and measurements on an array of MESFET. Due to problems in controlling the fabrication processes, the scatter was such that no correlation between device characteristics and the distance to nearest dislocation would be established. However, scatter of threshold voltage was larger for devices fabricated on areas of honeycomb-like dislocations network as opposed to areas with unconnected wavy lines of dislocation. Backgating (which causes unwanted communication between devices) was investigated in conjunction with substrate conduction measurement. A model was proposed for the effect as present in the devices used in this experiment. / Applied Science, Faculty of / Electrical and Computer Engineering, Department of / Graduate
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Effets sur l'As-Ga d'une bande d'impuretés à basse temperatureBenzaquen, M. (Moïses) January 1984 (has links)
No description available.
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