Defect engineering of InP and InGaAs for optoelectronic applications
Abstract
InP and InGaAs lattice matched to InP hold a special place in the optoelectronics
industry because of their room temperature bandgaps of 1.27 and 0.73 e V; these translate into
emission/ detection wavelengths of - 0.9 and 1.6 μm As such, they are ideal for the
development of long wavelength technology, in particular the 1.3 and 1.5 5 μm emissions that
are achievable in lattice matched InGaAs/InP systems, which can be transmitted through
optical fibre with low signal loss for long distance telecommunications. However, the device
processing technologies of InP and InGaAs are less mature than those of, say, GaAs or Si, and
continuing research is needed to take full advantage of the intrinsic properties of these
materials.
One branch of current research involves defect production and diffusion, which is
known to greatly modify the electrical and optical properties of these semiconductors. Ion
implantation is one way of introducing a large amount of defects, and a significant part of this
work focuses on understanding the changes to the electrical and optical properties of InP and
InGaAs resulting from such implantation. Combined with structural studies, an insight into
multiple defective layers of varying optical and electrical properties after implantation has been
gleaned. In both InP and InGaAs, implantation was found to result in large concentrations of
shallow donors which reduced the resistance of the semiconductor. Depending on the
element implanted, this reduced resistivity was concentrated in one or two layers within the
damaged region. Implantation also resulted in the creation of non-radiative recombination
centers, which in some cases reduced the carrier lifetime of the material to the sub-picosecond
range. With the aim of creating materials suitable for ultrafast photodetectors, this work has
successfully found ways to increase the resistivity of both implanted InP and InGaAs while
keeping the response times as low as possible. In addition to the creation of defect.s, their diffusion was induced using annealing
techniques, and the corresponding structural, electrical and optical changes observed. 1bis
provided another parameter for varying the properties of defective InP and InGaAs with
device applications in mind. Annealing, in combination v.1:ith ion implantation and dielectric
capping layer techniques, was also used to promote interdiffusion of InP /InGaAs and
InGaAs/ AlGainAs quantum well structures, thereby tuning the emission/ detection
-wavelengths. The damage accumulation processes resulting from implantation in InP and
InGaAs at different temperatures was found to strongly influence the degree of interdiffusion
achieved. 1bis was related to whether implantation conditions were conducive to fonnation of
point defects or more complex clusters and loops, since the fonner were more mobile and
thus good vectors for interdiffusion. Strain, as well as the inteiplay of group III and group V
interdiffusion and surface chemistry, was found to play a major role in the amount of
wavelength tuning that was achievable. The quantum well structures studied showed a great
deal of versatility in temis of the obtained peak emission wavelength shifts, and in some cases
this emission/ detection wavelength was actually shifted to larger values (redshifted), something
not achievable in standard interdiffusion of AlGaAs/ GaAs and InGaAs/ Ga.As quantum wells.
1bis wotk has provided clear advances in the understanding of defective InP and
InGaAs with direct applications to devices. By varying implant dose, initial free carrier
concentration, annealing temperature and dielectric deposition parameters, bulk materials and
heterostructures can be obtained with the ideal characteristics for optoeletronic applications.
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