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Dive into the research topics where W. Xia is active.

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Featured researches published by W. Xia.


Journal of Applied Physics | 1992

Solid phase epitaxy of stressed and stress‐relaxed Ge‐Si alloys

Q. Z. Hong; Jane G. Zhu; J. W. Mayer; W. Xia; S. S. Lau

Solid phase epitaxy of 3500‐A‐thick GexSi1−x (0.04≤x≤0.12) films on (100) Si substrates has been investigated. The thickness of regrown layers increased linearly with annealing time in the temperature range of 475–575 °C. The regrowth rates of stressed alloys were less than those of pure Si, while stress‐relaxed alloys have larger rates than Si. The difference in regrowth rates was explained by the activation‐strain tensor model (Aziz, Sabin, and Lu, to be published in Phys. Rev. B). The first element of the activation‐strain tensor obtained in this experiment was in excellent agreement with that deduced by Aziz et al. For low Ge concentrations (x<0.08), the recrystallized region was of good crystalline quality. However, threading dislocations were observed in a stressed Ge0.1Si0.9 alloy after complete recrystallization. During the regrowth at 550 °C, the Ge‐Si alloy first regrew coherently up to 300 A, above which threading dislocations started to nucleate. On the other hand, no dislocations were detecte...


Journal of Applied Physics | 1989

On the thermodynamical driving force during ion mixing of the Co-Si system

W. Xia; C.A. Hewett; M. Fernandes; S. S. Lau; D. B. Poker

The relative importance between the thermodynamical driving force and kinetics in thermal annealing and ion mixing in the thermally activated regime has not been clarified. To probe the role of the thermodynamical driving force in reactions between metals and silicon, the Co‐Si system was chosen for investigation. In general, three silicide phases are formed during thermal annealing of samples consisting of Co thin films deposited on Si substrates, i.e., Co2Si (the first phase to form with a heat of formation, ΔHf=−9 kcal/g atoms), CoSi (ΔHf=−12 kcal/g atoms), and CoSi2 (the last phase to form, with ΔHf=−8.2 kcal/g atoms). Previous experiments have shown that annealing a sample of Si/CoSi/Co converts CoSi into Co2Si instead of a continuous growth of CoSi. This type of reaction is apparently unrelated to the magnitude of the thermodynamical driving force since ΔHf of CoSi is significantly larger than those of Co2Si and CoSi2, but is kinetically restricted instead. Under ion mixing conditions the kinetic re...


Journal of Applied Physics | 1992

Ion mixing of III‐V compound semiconductor layered structures

W. Xia; S. A. Pappert; B. Zhu; A. R. Clawson; Paul K. L. Yu; S. S. Lau; D. B. Poker; C. W. White; S. A. Schwarz

Compositional disordering of III‐V compound superlattice structures has received considerable attention recently due to its potential application for photonic devices. The conventional method to induce compositional disorder in a layered structure is to implant a moderate dose of impurity ions (∼1015/cm2) into the structure at room temperature, followed by a high‐temperature annealing step (this process is referred to as IA here). Ion irradiation at room temperature alone does not cause any significant intermixing of layers. The subsequent high‐temperature annealing step tends to restrict device processing flexibility. Ion mixing (IM) is capable of enhancing compositional disordering of layers at a rate which increases exponentially with the ion irradiation temperature. As a processing technique to planarize devices, ion mixing appears to be an attractive technology. In this work, we investigate compositional disordering in the AlGaAs/GaAs and the InGaAs/InP systems using ion mixing. We found that the ion...


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1991

Ion mixing of semiconductor superlattices

W. Xia; S.N. Hsu; C.C. Han; S.A. Pappert; B. Zhu; C. Cozzolino; P.K.L. Yu; S. S. Lau; D.B. Poker; C.W. White; S.A. Schwarz

Abstract Compositional disordering of III–V compound superlattice structures has received considerable attention recently due to its potential application for photonic devices. The conventional method to induce compositional disorder is to implant a moderate dose of impurity ions (∼ 1015 cm−2) into the structure at room temperature, followed by a high-temperature annealing step (this process is referred to as IA here). Ion irradiation at room temperature alone does not cause any significant intermixing of layers. The subsequent high-temperature annealing step tends to restrict device processing flexibility. Ion mixing (IM) is capable of enhancing compositional disordering of layers at a rate which increases exponentially with the ion irradiation temperature. As a processing technique to planarize devices, ion mixing appears to be an attractive technology. In this work, we investigate compositional disordering in the AlGaAs/GaAs and the InGaAs/InP systems using ion mixing. We found that the ion mixing behavior of these two systems shows a thermally activated regime as well as an athermal regime, similar to that observed for metal-metal and metal-semiconductor systems. Ion mixing is observed to induce compositional disordering at significantly lower temperatures than that for the IA process. We have compared the two processes in terms of four parameters (1) irradiation temperature, (2) dose dependence, (3) annealing, and (4) electrically active ions. We found that the IM process is more efficient in utilizing the defects generated by ion irradiation to cause disordering. Both the physical mechanism of ion mixing and possible device implications will be discussed.


Applied Physics Letters | 1993

Photoelastic waveguides formed by interfacial reactions

L. S. Yu; Z. F. Guan; W. Xia; Q. Z. Liu; F. Deng; S. A. Pappert; Paul K. L. Yu; S. S. Lau; L. T. Florez; J. P. Harbison

The fabrication of low‐loss photoelastic waveguides in GaAs/AlGaAs layered structures by thin film reactions is investigated. The waveguides are formed by opening a narrow window stripe, a few microns wide, in an otherwise continuous Ni layer under tension deposited on a semiconductor structure. The local tensile stress induced by the Ni layer in the semiconductor causes the local refractive index to increase, thus providing the guiding mechanism. Annealing the sample at 250 °C for 1 h induced an interfacial reaction between the Ni film and the substrate to form Ni3GaAs. The formation of an interfacial compound stabilizes the stresses, making the stress state independent of the deposition system and technique. Single‐mode waveguide propagation losses as low as 1.4 dB/cm at 1.53 μm wavelength have been obtained on annealed waveguides. Further annealing up to 600 °C did not cause degradation in the optical confinement, thus indicating a thermally stable planar waveguide fabricated by this process. Other pho...


Journal of Applied Physics | 1992

Simultaneous disordering and isolation induced by ion mixing in InGaAs/InP superlattice structures

S. A. Pappert; W. Xia; B. Zhu; A. R. Clawson; Z. F. Guan; Paul K. L. Yu; S. S. Lau

The phenomenon of simultaneous compositional disordering and the formation of electrical resistive layers induced by oxygen implantation in InGaAs/InP superlattices has been investigated. The disordering characteristics have been studied as a function of implantation temperature and ion dose. It was found that implantation at elevated temperatures (referred to as the IM or ion mixing process) usually leads to much more efficient disordering compared to implantation at room temperature followed by annealing at the same elevated temperature (referred to as the implantation plus annealing process). Of particular interest is the observation that ion mixing at 550 °C with 1×1013 O+/cm2 leads to significantly more disordering than implantation with the same dose at room temperature followed by annealing at 550 °C for the same period of ion mixing time. In addition, the electrical resistance of the ion‐mixed layer at 550 °C increases 2600 times for the p‐type InGaAs/InP superlattice structure, whereas the sample...


Applied Physics Letters | 1992

Planar, low‐loss optical waveguides fabricated by solid‐phase regrowth

W. Xia; L. S. Yu; Z. F. Guan; S. A. Pappert; Paul K. L. Yu; S. S. Lau; S. A. Schwarz; M. A. A. Pudensi; L. T. Florez; J. P. Harbison

Planar, low‐loss AlGaAs/GaAs waveguides have been fabricated using the solid‐phase regrowth (SPR) process. Single‐mode waveguide with a propagation loss as low as 1.6 dB/cm have been obtained. This process requires only thin‐film deposition and low‐temperature short‐duration annealing (i.e., 650 °C for 30 s), thus making the SPR method a much simplified technique to induce compositional disordering. Simultaneous electrical isolation and compositional disordering are also demonstrated with the SPR process.


Applied Physics Letters | 1991

Compositional disordering by solid phase regrowth

W. Xia; C. C. Han; S. A. Pappert; S.N. Hsu; Z. F. Guan; Paul K. L. Yu; S. S. Lau

The principle of solid phase regrowth (SPR)has been used to induce compositional disordering in AlGaAs/GaAs superlattice structures in the temperature range of 400 °C (30 min)–650 °C (30 s) as compared to the conventional diffusion method in the temperature range of 600–850 °C for hours. The SPR process is simple to implement, requiring only thin‐film deposition and annealing. The crystal quality as well as the photoluminescence signals emerging from the disordered region generally improve with increasing processing temperature. The simplicity, the low process temperature, and the short process duration of the SPR technique are distinct advantages for optoelectronic applications, especially for self‐aligned devices.


Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1989

On the temperature dependence and the moving species during ion mixing

W. Xia; M. Fernandes; C.A. Hewett; S. S. Lau; D. B. Poker; J.P. Biersack

Abstract In this paper, we review the experimental observations of the temperature dependence and the moving species in ion mixing, emphasizing the metal-semiconductor systems. Ion mixing is the combined effect of two components. One component is temperature independent and is primarily due to events in the prompt regime; the other component is temperature dependent and has the characteristics of the associated thermal reactions. The moving species during ion mixing are influenced by collisional effects, either due to secondary recoils, or due to local hot spots, or both. The secondary recoil concept is consistent with experimental observations that the motion of the lighter element in a bilayer sample is enhanced. There is ample evidence that while the athermal regime is caused by particle-solid interactions, thermodynamical forces are important in deciding the magnitude of mixing. In the thermally activated regime, the ion induced reaction product should be influenced by the heats of formation of various compounds. We also indicate areas where satisfactory explanations are not available at present.


Journal of Applied Physics | 1994

Planar 1.3 and 1.55 μm InGaAs(P)/InP electroabsorption waveguide modulators using oxygen ion mixing and the photoelastic effect

S. A. Pappert; W. Xia; X. S. Jiang; Z. F. Guan; B. Zhu; Q. Z. Liu; L. S. Yu; A. R. Clawson; Paul K. L. Yu; S. S. Lau

Efficient 1.3 and 1.55 μm InP‐based electroabsorption waveguide modulators with planar device structures have been demonstrated. Elevated temperature oxygen ion implantation and/or the photoelastic effect induced by W metal stressor stripes deposited on the semiconductor surface have been used to produce these self‐aligned planar guided‐wave devices. The oxygen ion mixing process has been used to simultaneously achieve compositional disordering and electrical isolation of superlattice material while the photoelastic effect has been used to improve the lateral mode confinement. A 1.3 μm Franz–Keldysh modulator with a ≳10 dB extinction ratio at 2 V and a 1.55 μm device with a ≳10 dB extinction ratio at 7 V are reported. These single growth step planar processing techniques have also been used to fabricate relatively low‐loss (<4 dB/cm) double heterostructure InGaAs(P)/InP single‐mode optical waveguides which demonstrate their usefulness in developing InP‐based photonic integrated circuits.

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S. S. Lau

University of California

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Paul K. L. Yu

University of California

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S. A. Pappert

University of California

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Z. F. Guan

University of California

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B. Zhu

University of California

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D. B. Poker

Oak Ridge National Laboratory

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L. S. Yu

University of California

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A. R. Clawson

University of California

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C.A. Hewett

University of California

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M. Fernandes

University of California

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