Spelling suggestions: "subject:"gallium arsenic"" "subject:"allium arsenic""
191 |
A study of deep levels of AlGaAs/GaAs heterojunction bipolar transistorsHuang, Chun-ta 10 July 1992 (has links)
A study of deep levels of the emitter region of a
heterojunction bipolar transistor is investigated using deep
level transient spectroscopy (DLTS), deep level admittance
spectroscopy (DLAS), thermally stimulated capacitance
(TSCAP), and capacitance-voltage (C-V) profiling. The DX
center, with an activation energy of 0.45 eV, is the only
deep level detected. By varying the DLTS rate window and
filling pulse widths, DX is found to be comprise of two
closely spaced DX centers, denoted DX1 and DX2. A positive
peak observed in the DLTS spectra is attributed to electron
capture, not minority carrier emission, and, thus, is an
experimental artifact. Finally, the reduction of current gain
(β) at low collector current and the effect of the DX center
on the switching characteristics of HBTs are briefly
discussed. / Graduation date: 1993
|
192 |
Wide bandwidth GaAs MESFET amplifierYan, Kai-tuan Kelvin 29 April 1992 (has links)
Graduation date: 1992
|
193 |
Modeling and testing of semi-insulating gallium arsenide interdigitated photodetectorsKollipara, Ravindranath Tagore 12 April 1991 (has links)
High speed photodetectors are a necessary element in
broad band digital and analog optical communication systems.
In this thesis easily integrable planar high speed
photodetectors made on undoped semi-insulating (SI) GaAs
substrates are modeled and tested. The fabrication process
of the detectors is fully compatible with GaAs
metal-semiconductor field effect transistor (MESFET)
processing technology. Interdigitated fingers are used as
the contacts to achieve both high sensitivity and large
bandwidth. Detectors made with both ohmic and Schottky
contacts are fabricated and tested.
The equivalent circuit elements of the interdigitated
structure are modeled using accurate lumped element circuit
models associated with the various discontinuities of the
structure. The results of the model agree well with the
experimental results as well as with other published
results. Numerical simulation of the SI-GaAs metal-semiconductor-
metal (MSM) photodetector is performed. The
carriers are tracked after an ideal optical pulse is applied
and the intrinsic current as a function of time is computed.
Then the influence of all the external circuit elements is
included and the output current across the load resistor is
computed. The simulated response is compared with other
published models.
The electrical and optical characteristics of the
detectors are measured. For ohmic contact detectors, the
dark current increases linearly with bias until some
critical field is reached beyond which the dark current
increases nonlinearly with bias. The time response of the
detectors is measured with a 10 ps pulsed laser operating at
- 600 nm and also with a pulsed GaAs /AlGaAs semiconductor
laser operating at 850 nm. The ohmic and Schottky contact
detectors have approximately the same rise time. The fall
time of the Schottky contact detector is much smaller than
the fall time of ohmic contact detector. The long fall time
of the ohmic detector does not depend on the spacing between
contacts. This long fall time is due to the large barrier
that exists near the ohmic metal/SI-GaAs cathode contact. No
such barrier exists for SI-GaAs MSM photodetector. The
simulated impulse response of the SI-GaAs MSM photodetector
is compared with the measured impulse response. / Graduation date: 1991
|
194 |
Reduction of phonon resonant terahertz wave absorption in photoconductive switches using epitaxial layer transferKasai, S, Katagiri, T, Takayanagi, J, Kawase, K, Ouchi, T 18 March 2009 (has links)
No description available.
|
195 |
Spin Polarization and Conductance in Quantum Wires under External Bias PotentialsLind, Hans January 2010 (has links)
We study the spin polarization and conductance in infinitely long quasi one-dimensionalquantum wires under various conditions in an attempt to reproduce and to explain some of theanomalous conductance features as seen in various experiments. In order to accomplish thistask we create an idealized model of a quantum wire in a split-gate semiconductorheterostructure and we perform self-consistent Hartree-Fock calculations to determine theelectron occupation and spin polarization. Based on those results we calculate the currentthrough the wire as well as the direct and differential conductances. In the frame of theproposed model the results show a high degree of similarity to some of the experimentallyobserved conductance features, particularly the 0.25- and 0.85-plateaus. These results lead usto the conclusion that those conductance anomalies are in fact caused by the electronsspontaneously polarizing due to electron-electron interactions when an applied potentialdrives a current through the wire.
|
196 |
Analysis of Zincblende-Phase GaN, Cubic-Phase SiC, and GaAs MESFETs Including a Full-Band Monte Carlo SimulatorWeber, Michael Thomas 06 October 2005 (has links)
The objective of this research has been the study of device properties for emerging wide-bandgap cubic-phase semiconductors. Though the wide-bandgap semiconductors have great potential as high-power microwave devices, many gaps remain in the knowledge about their properties. The simulations in this work are designed to give insight into the performance of microwave high-power devices constructed from the materials in question. The simulation are performed using a Monte Carlo simulator which was designed from the ground up to include accurate, numerical band structures derived from an empirical pseudo-potential model. Improvements that have been made to the simulator include the generalized device structure simulation, the fully numerical final state selector, and the inclusion of the overlap integrals in the final-state selection. The first comparison that is made among the materials is direct-current breakdown. The DC voltage at which breakdown occurs is a good indication of how much power a transistor can provide. It is found that GaAs has the smallest DC breakdown, with 3C-SiC and ZB-GaN being over 3 times higher. This follows what is expected and is discussed in detail in the work. The second comparison made is the radio-frequency breakdown of the transistors. When devices are used in high-frequency applications it is possible to operate them beyond DC breakdown levels. This phenomenon is caused by the reaction time of the carriers in the device. It is important to understand this effect if these materials are used in a high-frequency application, since this effect can cause a change in the ability of a material to produce high-power devices. MESFETs made from these materials are compared and the results are discussed in detail.
|
197 |
Spin polarization control through resonant states in an Fe/GaAs Schottky barrierHonda, S., Itoh, H., Inoue, J., Kurebayashi, H., Trypiniotis, T., Barnes, C. H. W., Hirohata, A., Bland, J. A. C. 12 1900 (has links)
No description available.
|
198 |
III-V channel MOS devices with atomic-layer-deposited high-k gate dielectrics : interface and carrier transport studiesShahrjerdi, Davood, 1980- 10 October 2012 (has links)
The performance scaling of metal-oxide-semiconductor field-effect-transistors (MOSFETs) has been historically achieved through shrinking the gate length of transistors for over four decades. Addressing the current challenges with CMOS scaling, the 2005 edition of International Technology Roadmap for Semiconductors has predicted the need for so-called technology boosters involving new materials for the gate dielectric and the channel as well as innovative structures. Theoretical studies suggest that the incorporation of high-mobility channel materials such as germanium and III-Vs could outperform bulk Si technology in terms of switching characteristics. Hence, this has recently led to tremendous research activity to explore the prospects of III-V materials for CMOS applications. Nevertheless, technological challenges such as formation of highquality interface between gate dielectric and III-V channel have hindered the demonstration of enhancement-mode III-V MOSFETs. Hence, tremendous effort has been devoted to study the exact origin of Fermi level pinning at the oxide/III-V interface. On the other hand, the advent of high-k materials has opened up the possibility of exploring new channel materials, for which it is challenging to achieve high-quality interface analogous to that of SiO2 on Si. Lately, III-Vs have been extensively explored in order to find compatible gate dielectrics which can unpin the Fermi level at the interface. Amongst various schemes, atomic layer deposition of high-k dielectrics offers some unique advantages such as reduction of GaAs interfacial oxides upon high-k deposition through an appropriate choice of precursor chemistry. The chief focus of this dissertation is to develop a simple wet clean process prior to high-k deposition, suitable for III-V substrates. The impact of various chemical treatments of GaAs substrates on the properties of high-k/GaAs interface was studied through extensive material and electrical characterization methods. The suitability of the ALD-grown high-k gate dielectrics on GaAs for MOSFET fabrication was explored. Charge trapping was found to result in significant errors in mobility extraction in high-k GaAs interface, where the role of high-k is not well understood. Hence, pulsed I-V and QV measurements and galvanomagnetic effects were utilized in order to directly measure the inversion charge in the channel without being affected by the charge traps as much as possible. It was also found that the material studies on GaAs substrates can be readily extended to other III-V channels, such as InGaAs. / text
|
199 |
Integration of thin film GaAs MSM photodetector in fully embedded board-level optoelectronic interconnectsLin, Lei 28 August 2008 (has links)
Not available / text
|
200 |
Electrical properties of single GaAs, Bi₂S₃ and Ge nanowiresSchricker, April Dawn 28 August 2008 (has links)
Not available / text
|
Page generated in 0.0748 seconds