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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Titanium nitride (TiNx) thin films were deposited onto InP by means of the rapid-thermal-low-pressure-chemical-vapor-deposition (RT-LPMOCVD) technique, using the tetrakis (dimethylamido) titanium (Ti(NMe2)4 or DMATi) complex as the precursor. Depositions were successfully carried out at temperatures below 550 °C, pressure range of 5–20 Torr and duration of 50 to 90 s, to give layer thicknesses up to 200 nm and growth rates in the range of 0.8 to 4.5 nm/s. These films had a stoichiometric structure and contained nitrogen and titanium in a ratio close to unity, but also contained a significant amount of carbon and oxygen. The elements were spread uniformly through the films, the nitrogen was Ti bounded, and the carbon was partially titanium bonded and organic bonded as well. The film resistivity was in the range of 400–800 μΩ cm−2; the stress was always compressive, in the range of − 0.5 × 109 to − 2 × 1010 dyne cm−2, and the film had a good morphology. These layers performed as an ohmic contact while deposited onto p-In0.53Ga0.47As material, (Zn-doped 1.2 × 1018 cm−3), provided an excellent step coverage for high aspect ratio via holes and were deposited selectively onto the InP and based materials when using SiO2 mask. This represents the first report of TiNx films deposited in a commercial RT-LPMOCVD reactor using the DMATi precursor.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 2760-2768 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Near-surface damage created by Ar+ ion milling in InP and GaAs was characterized by capacitance-voltage, current-voltage, photoluminescence, ion channeling, and transmission electron microscopy. We find no evidence of amorphous layer formation in either material even for Ar+ ion energies of 800 eV. Low ion energies (200 eV) create thin (≤100 A(ring)) damaged regions which can be removed by annealing at 500 °C. Higher ion energies (≥500 eV) create more thermally stable damaged layers which actually show higher backscattering yields after 500 °C annealing. Heating to 800 °C is required to restore the near-surface crystallinity, although a layer of extended defects forms in GaAs after such a treatment. No dislocations are observed in InP after this type of annealing. The electrical characteristics of both InP and GaAs after ion milling at ≥500 eV cannot be restored by annealing, and it is necessary to remove the damaged surface by wet chemical etching. For the same Ar+ ion energies the damaged layers are deeper for InP than for GaAs after 500 eV ion milling at 45° incidence angle. Removal of ∼485 and ∼650 A(ring) from GaAs and InP, respectively, restores the initial current-voltage characteristics of simple Schottky diodes.
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effects of hydrogenation on the low-temperature (5 K) photoluminescence properties of GaAs grown on InP substrate by metalorganic chemical vapor deposition are investigated. An emission band at ∼1.4 eV originating from the GaAs/InP interfacial region shows a 30-fold increase in intensity relative to the GaAs band-edge emission after exposure to hydrogen plasma for 30 min at 250 °C. This improvement in intensity is attributed to hydrogen passivation of defects at the heterointerface caused by the large (≈4%) lattice mismatch between GaAs and InP. Annealing the hydrogenated sample at 350 °C nullifies the passivation effect. Further, the 1.4-eV band shifts to higher energy on annealing the sample in the temperature range 150–450 °C with the hydrogenated sample exhibiting a larger shift than the untreated sample. It is suggested that the annealing-induced peak shift arises due to modification of the interface and that it is greater in the hydrogenated sample compared to the untreated sample.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 785-792 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Structural and electrical damage imparted to InP and In0.72Ga0.28As0.6P0.4 (λg(approximately-equal-to)1.3 μm) surfaces during CH4/H2 reactive ion etching (RIE) have been examined. X-ray photoelectron spectroscopy was used to monitor changes in the surface chemistry, Rutherford backscattering spectrometry was used to measure crystallographic damage, and current-voltage and capacitance-voltage measurements were made to examine electrically active damage and its depth. Two classes of damage are observed: crystallographic damage originating from preferential loss of P (As) and/or ion bombardment-induced collision cascade mixing and, for p-type material, hydrogen passivation of Zn acceptors. Etching at 13.6 MHz, 60–90 mTorr, 10% CH4/H2, and bias voltages of ∼300 V contains gross ((approximately-greater-than)1%) damage as measured by RBS to within 40 A(ring) and electrically active damage to within 200 A(ring) of the surface. This is a factor of 3–6 shallower than other RIE processes operated below 10 mT with comparable or higher bias voltages. Acceptor passivation of both InP and InGaAsP, arising from the association of hydrogen with Zn sites, occurs to a depth of 2000 A(ring) after RIE and causes a decrease in carrier concentration in this layer. The effect is reversed, however, by rapid thermal processing at temperatures between 350 and 500 °C.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 3943-3947 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The fabrication, performance characteristics, and design rules of buried-facet optical amplifiers are described. Chip gain of 25 dB, gain ripple of 〈1 dB, and gain difference of ≤1 dB for TE- and TM-polarized light are observed. The gain ripple and polarization dependence of gain correlate well with the ripple and polarization dependence of the amplified spontaneous emission spectrum. The performance of buried-facet amplifiers is comparable to that of cleaved-facet amplifiers with very good antireflection (R〈10−4) coatings. The buried-facet design reduces the requirement on antireflection coatings and makes the fabrication process more reproducible.
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  • 6
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 57 (1990), S. 887-889 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Incorporation of atomic hydrogen into heteroepitaxial Si-doped GaAs layers grown directly on InP substrates by organometallic vapor phase epitaxy produces substantial increases in the reverse bias breakdown voltage of TiPtAu Schottky diodes fabricated on the GaAs-on-InP. Plasma hydrogenated diodes annealed at 400 °C to restore the electrical activity of the passivated shallow donors have reverse breakdown voltages (VB) of ∼6.5 V compared to 4.5 V for untreated samples. The increases in VB are stable to 500 °C annealing for 5 min. Atomic profiling of deuterated samples showed substantial outdiffusion of deuterium from the GaAs at 600 °C, with increasing accumulation at the heterointerface. The deuterium in this disordered region after 600 °C annealing is in a relatively immobile, electrically inactive state.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 58 (1991), S. 1256-1258 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Changes in cathodoluminescence (CL) intensity from a buried single AlGaAs/GaAs/AlGaAs quantum well (QW) as a result of exposure to electron cyclotron resonance (ECR) hydrogen or argon discharges are reported. For additional dc biases of 150 V on the sample during either H2 or Ar plasma exposure, we observe substantial decreases in CL intensity from the well. Ar+ ion bombardment creates damage more resistant to annealing than does H+ ion bombardment at the same energy. The ECR discharges alone with zero additional dc bias cause degradation in the well luminescence due possibly to defects created by energetic electron bombardment or ultraviolet illumination. At intermediate bias voltages (50 V) strong hydrogen passivation of nonradiative centers is observed, leading to 500% increases in CL intensity from the well. The initial characteristics of the QW under these conditions are restored by annealing at 400 °C.
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  • 8
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The use, transportation, and storage of the hazardous gas, arsine, raise serious safety issues. Consequently, there is considerable interest in the generation of arsine on demand from less hazardous substances. We report the first use of in situ generated arsine for III-V epitaxy. The gas has been generated electrochemically at an arsenic cathode in an aqueous electrolyte and used to supply a hydride vapor phase epitaxy reactor. InGaAs/InP test structures were grown on InP substrates and were similar to comparison structures grown using tank arsine. Recessed-gate enhanced Schottky metal-semiconductor field-effect transistors were fabricated and exhibited well-behaved current-voltage characteristics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 56 (1990), S. 1263-1265 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It is shown for the first time that carbon behaves predominantly as an acceptor in InGaAs and AlInAs under co-implantation conditions. The co-implanted ion, regardless of species, acts to create vacant lattice sites for occupation by the carbon. Implantation of 40 keV carbon ions alone at doses between 5×1012 and 5×1014 cm−2 followed by annealing in the range 600–950 °C for 10 s does not produce any measurable electrical activity in either material. In InGaAs, carbon implantation at 5×1014 cm−2 produced net acceptor activations of 20, 11, or 6% for Ga, Ar, or As co-implantation, respectively, at the same doses after 700 °C, 10 s anneals. Similar results were obtained for AlInAs after annealing at 900 °C. The diffusion coefficient for carbon is estimated from secondary-ion mass spectrometry measurements to be less than 3.3×10−14 cm2 s−1 at 800 °C in both materials.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 55 (1989), S. 2014-2016 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Carbon implanted into InP at doses between 5×1012 and 5×1014 cm−2, either by itself or with B, Ga, Al, or P coimplantation at room temperature or 200 °C, displays donor activity for all annealing temperatures (600–900 °C; 10 s). Phosphorus coimplantation enhances the donor activation percentage over carbon-only implantation, while coimplants of B, Ga, and Al reduce the donor activity. Peak carrier concentrations of 3×1019 cm−3 were obtained for C+P implantation at a dose of 5×1014 cm−2, followed by annealing at 700 °C for 10 s. Annealing at 〉700 °C leads to a reduction in net donor density through carbon site switching to produce self-compensation. The C diffusivity is estimated to be less than 2.5×10−14 cm−2 s−1 at 800 °C.
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