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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 2736-2736 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    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 66 (1989), S. 3839-3849 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The etch rate of GaAs during reactive ion etching (RIE) in a CCl2F2:O2 discharge (4 mTorr, 0.56 W cm−2) shows a strong temperature dependence, increasing from ∼500 A(ring) min−1 at 50 °C to 2800 A(ring) min−1 at 400 °C. Arrhenius plots of the etch rate show two activation energies (0.17 eV from 50 to 150 °C and 0.11 eV from 150 to 400 °C). There is no significant plasma power density dependence of the etch rate at elevated temperatures (≥100 °C) in contrast to the strong dependence at 50 °C. The surface morphology undergoes smooth-to-rough-to-smooth-to-rough transitions at ∼150, 250, and 400 °C, respectively, although TiPtAu Schottky diodes exhibit near-ideal behavior on GaAs etched at 150 °C. The As-to-Ga ratio in the first 100 A(ring) from the surface increases with increasing RIE temperature, with chloride residues absent above 150 °C. Fluorocarbon residues were present on all samples, but were limited to the first 10–15 A(ring). As determined by x-ray photoelectron spectroscopy, fluorine was present almost exclusively as metallic gallium fluorides, while oxygen was present as both Ga and As oxides. Ion channeling detected lattice disorder to depths of ∼200 A(ring) for etch temperatures from 50 to 250 °C, while there was less damage for etching at 400 °C. No new RIE-induced deep levels were observed by capacitance transient spectroscopy in any of our samples, although the concentration of the midgap donor EL2 increased with increasing temperature during the RIE process.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 66 (1989), S. 2137-2147 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The etch rate and surface chemistry of AlxGa1−xAs after reactive ion etching (RIE) in CCl2F2:O2 was examined as a function of etch time (1–22 min), plasma power density (0.3–1.3 W cm−2), pressure (1–30 mTorr), gas composition (0%–80% O2), gas flow rate (10–50 sccm), sample temperature (50–350 °C), and Al composition (x=0.15–1). The etch rate is nonlinear with time, and decreases rapidly with increasing AlAs mole fraction. Essentially no temperature dependence of the etch rate is observed under our conditions, and there are no major differences in the surface chemistries of AlGaAs etched at different temperatures. The formation of a thin layer (50–90 A(ring)) of AlF3 during the RIE treatment appears to control the etch rate, and the surface morphology becomes progressively smoother for increasing Al composition. No residual lattice disorder is detected by cross-sectional transmission electron microscopy under any of our conditions, although current-voltage measurements on Schottky barrier diodes fabricated after RIE show higher ideality factors and barrier heights than unetched control samples. Annealing at 500 °C for 30 s almost restores the initial electrical properties of the material.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 1281-1292 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The reactive ion etching of GaAs with a CCl2F2:O2 discharge was investigated as a function of gas flow rate (10–60 sccm), total pressure (2–50 mTorr), power density (0.25–1.31 W cm−2), gas composition (0%–70% O2), and etch time (1–64 min). The etch rate decreases with increasing gas flow rate, increases with increasing power density, and goes through a maximum at a gas composition of 75:25 CCl2F2:O2 under our conditions. After etching at low-power densities (0.56 W cm−2) and for high CCl2F2 ratios (19:1 to O2), carbon and chlorine could be detected in the GaAs to a depth of less than 15 A(ring) by x-ray photoelectron spectroscopy. Under these conditions there was a Ga deficiency to a depth of ∼100 A(ring), which we ascribe to surface roughening and the preferential vaporization of As2O3 over Ga2O3. At high-power densities (1.31 W cm−2) a polymeric layer several hundred angstroms thick containing CCl and CF bonds was observed on the GaAs surface. Etching under O2-rich conditions did not lead to any additional creation of surface oxides. Both ion channeling and electron microscopy detected a thin disordered layer on the GaAs after etching. Small (〈100 A(ring) diam) dislocation loops were present at a depth varying from ∼400 A(ring) for 0.56 W cm−2 (380-V self-bias) plasma power density to ∼2200 A(ring) for 1.31 W cm−2 (680-V self-bias). The disorder was stable against a 500 °C annealing treatment.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5208-5212 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Tantalum nitride films were reactive sputter deposited onto chemical vapor deposited (CVD)-diamond self-standing thick layers, to be used as resistors for microelectronic applications. The TaN films had excellent morphology and were very stable through heating cycles at temperatures up to 400 °C for a few hours. Post-deposition sintering of the films at temperatures up to 300 °C stabilized the film resistance at values in the range of 75–85 Ω. The deposited film was later patterned with photoresist and dry etched, at rates of up to 70 nm min−1 and the resulting features served as masks for further self-aligned etching processes of the underlying CVD-diamond layer.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The process kinetics, chemical composition, morphology, microstructures, and stress of rapid-thermal low pressure metalorganic chemical vapor deposited (RT-LPMOCVD) TiNx films on InP, using a combined reactive chemistry of ammonia (NH3) gas and tetrakis (dimethylamido) titanium (DMATi) liquid precursors, were studied. Enhanced deposition rates of 1–3 nm s−1 at total chamber pressures in the range of 3–10 Torr and temperatures of 300 °C–350 °C at a NH3:DMATi flow rate ratio of 1:8 to 1:15 were achieved. Stoichiometric film compositions were obtained, with carbon and oxygen impurity concentrations as low as 5%. Transmission electron microscopy analysis identified the deposited films as TiN with some epitaxial relationship to the underlying (001) InP substrate. This process provides a superior film to the preview RT-LPMOCVD TiNx film deposited using only the DMATi precursor.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 7664-7673 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: WSix thin films deposited on InP substrates have been investigated for possible use as refractory ohmic contact materials for self-aligned laser devices. The films have been rf diode sputtered using various Ar gas pressures from a single commercial target composed of W and Si with an atomic ratio of 1:1. Following the deposition, the WSix/InP samples were rapid thermal processed using a rapid thermal metalorganic chemical vapor deposition system in a controlled low-pressure ambient of N2:H2 (9:1) and tertiarybutylphosphine. The as-deposited films (∼100 nm thick) were amorphous but crystallized in the temperature range of 600–650 °C. The WSi2 phase forms first at 600 °C and then the W5Si3 nucleate with further heating at 650 °C. As a result of the crystallization, a reduction in the specific contact resistance to a value of 7.5×10−6 Ω cm2 and a decrease in the sheet resistance to values lower than 2 Ω/(D'Alembertian) were observed. In addition, a significant reduction in the internal stress and an improvement in the WSix-to-InP adhesion were found, demonstrating the potential of WSix as a contact material for InP-based self-aligned devices.
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  • 8
    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.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 3808-3815 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The possibility of replacing Pt in the Ti/Pt/Au base and traditionally used metallurgical structure by Ni, while bonding InP laser chip to a submount with AuSn (80% Au) solder, has been investigated. Various Ni-based metal alloys have been prepared by evaporation. Reflow experiments were conducted in a chamber under forming gas-controlled ambient. The Ti/Ni/AuSn system provided much longer surface local freezing duration compared to the Ti/Pt/AuSn system. Scanning electron microscopy analysis revealed a smoother surface morphology for the Ti/Ni/AuSn system after the metal refroze. Auger electron spectroscopy depth profiles indicated the formation of a Ni-Sn-Au interacted layer. The interaction took place in two steps: the first stage was the dissolution of Ni into the Au-Sn liquid followed by precipitation of a Ni-Sn-Au intermetallic compound; the second stage was a solid-state interdiffusion of Sn, Au, and Ni which occured in the interacted layer and in the original Ni layer. The latter step was a diffusion-controlled process, resulting in a very slow growth rate. Both Au and Sn reacted to form Ni alloy layers of almost equal thickness, regardless of the reaction duration (up to about 5 min). This intensive reaction, however, did not lead to full consumption of the Ti interfacial layer, which provided an excellent adhesion layer between the submount and the metallurgical structure.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 563-567 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An attempt to apply a more stable metallurgical soldering system than the traditionally used Ti/Pt/Au-Sn reactive system was explored by replacing the barrier metals in between the chemical vapor deposited diamond (CVDD) submount and the Au-Sn solder with either W or Cr layers. In the case of the W layer a thin layer of Ti was added to improve the adhesion of Au-Sn solder to the W layer. The CVDD/W(100 nm)/Ti(10 nm)/Au-Sn(1.5–2.2 μm) system was heat treated at 350 °C for durations of 5 s–5 min, simulating a bonding cycle, and the metallurgical interactions were analyzed. Some diffusion of the Ti was observed, but the W layer remained intact. Thus, due to the absence of interaction between the Sn or Au and the W barrier layer, the Au:Sn ratio was kept uniform for long duration heating ((approximately-greater-than)2 min). The Au-Sn solder tends to "ball up'' in local spots leading to the formation of local voids in the continuous solder layer over the W. In the case of the CVDD/Ti (100 nm)/Cr(200 nm)/AuSn(1.5–2.2 μm) structure a minimum interaction between the Au-Sn solder and the barrier was observed through a heating cycle at 350 °C for 5 min. This heat treatment, however, led to solder surface roughness in the order of about 5000 A(ring) between bump peak and valley, but the Au:Sn composition remained in the eutectic ratio of 70:30 at. %. Both soldering metallurgical systems gave a potential good bonding of InP laser diodes to CVDD heat sinks.
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