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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Transmission electron microscopy and photoluminescence data are presented, before and after sample thermal annealing, on AlxGa1−xAs-GaAs quantum-well heterostructures with Se or Mg sheet doping in the barriers or in the quantum wells (QWs). The crystals are grown by metalorganic chemical vapor deposition and, in the active regions, have four GaAs wells and three Al0.2Ga0.8As barriers (or in one case five QWs and four barriers). The confining layer regions are bulk doped n type on the substrate side and p type on top (p-n). The sheet doping of the QW active region is obtained by deposition of Se from H2Se or Mg from bis(cyclopentadienyl) Mg in the middle of the layers (GaAs wells or Al0.2Ga0.8As barriers). The impurity sheet deposition (δ-Se or δ-Mg) is carried out in an arsine-rich atmosphere. Photoluminescence data on the as-grown crystals show that the energy ((h-dash-bar)ω) of the recombination radiation is not shifted by the sheet doping and that the samples behave as ordinary photopumped QWH lasers. Annealing the crystals in an As4 atmosphere (provided by excess As in a quartz ampoule) causes layer intermixing of the Se sheet-doped samples and very little disordering in the case of the Mg sheet-doped samples. Magnesium sheet doping leads to layer disordering only in the case of sample annealing with no excess As in the annealing ampoule. Disordering of both Se and Mg sheet-doped crystals occurs for Si3N4 capped but not for SiO2 capped samples.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Extensive data are presented on impurity-induced layer disordering (IILD) of AlxGa1−xAs-GaAs quantum-well heterostructures and superlattices that are Si implanted and annealed (Si+-IILD) at three different implant doses. We show that impurity activation is not critical to the layer disordering process and that Si diffusion from the implanted profile initiates Si+-IILD. When the implant dose is as high as φ≥5×1013/cm2 (nSi ≥2×1018/cm3), Si interstitial loops (Si-ILs) form by diffusion and agglomeration of the implanted Si atoms during the initial stages of annealing. If a source of Ga vacancies is provided (e.g., via an As overpressure or SiO2 encapsulation), the Si-ILs dissociate and supply Si atoms for diffusion and hence Si+-IILD during the latter stages of annealing. If a Si3N4 encapsulant is employed, however, fewer Si-ILs form and Si diffusion is inhibited. For an implantation dose as low as φ=1×1012/cm2 (nSi =3×1016/cm3), extensive Si+-IILD is realized via capless annealing and Si-ILs are not observed. It is significant for device applications that the layer-disordered material operates as a cw 77 K photopumped laser, which indicates that the layer averaging (IILD) does not damage the crystal.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: GaAs layers grown on misoriented silicon substrates are examined for defect reduction as a function of thermal annealing and degree of misorientation. These GaAs layers (3–4 μm) are grown by a two-step metalorganic chemical vapor deposition process on Si substrates misoriented 1°, 1.5°, 2°, 3°, 4°, and 6° from (100) toward [011]. Annealing takes place in an open tube furnace under an arsine ambient at 850 °C for one or two 30-min cycles. Double-crystal x-ray rocking measurements and plan-view and cross-section transmission electron microscopy are used to evaluate the resulting crystal quality. Prior to annealing, all cases exhibit approximately equal defect densities with the average size of the microtwins being a function of misorientation. There also exists an anisotropy in the microtwin variant distribution in the layers. After annealing, however, the defect density is found to be dependent on the misorientation. The 1° and 2° layers, which have smaller microtwins, exhibit a greater reduction in defect density after thermal cycling than the 4° and 6° layers. The annealed 4° and 6° layers instead exhibit larger microtwins on average than the as-grown layers. These data indicate that smaller microtwins are more likely to be annihilated through thermal cycling. In addition to the change in the microtwin structures, thermal cycling produces elongated dislocations in the 1° and 2° layers and dislocation tangles associated with the remaining microtwins in the 4° and 6° layers.
    Type of Medium: Electronic Resource
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  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Photoluminescence and absorption data are presented on AlxGa1−xAs-GaAs superlattices (SLs) disordered into bulk-crystal AlyGa1−yAs (0≤y≤x) by Si or Ge diffusion. The bulk-crystal AlyGa1−yAs produced by impurity-induced disordering (by Al-Ga interchange) is determined by transmission electron microscopy, absorption measurements, and photoluminescence to be homogeneous, with an alloy composition (y) that agrees with the average Al concentration of the SL. For low enough Al concentration (y≈0.23〈yc =0.44, the direct-indirect crossover), in absorption the Ge- or Si-disordered SL exhibits (4.2 and 77 K) the bulk-crystal exciton, which is characteristic of homogeneous alloy (AlyGa1−yAs). Stimulated emission (4.2 and 77 K) in bulk-crystal AlyGa1−yAs is observed ΔE≤50 meV below the band edge via photopumping for both Si- and Ge-disordered SLs of Al concentration yielding y∼0.23 and y∼0.39. Shallow hydrogenlike donor or acceptor states are characteristic of AlxGa1−xAs-GaAs SLs disordered with Ge or with Si. For the Si impurity (i.e., an AlxGa1−xAs-GaAs SL disordered with Si), however, much deeper states (transitions) are observed that saturate at higher photoexcitation levels. These states are attributed to nearest-neighbor or extended Si-Si pairs since similarly disordered AlxGa1−xAs-GaAs SLs doped with Ge do not exhibit deeper states.
    Type of Medium: Electronic Resource
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  • 5
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Data are presented showing that the Al-Ga interdiffusion coefficient (DAl-Ga) for an AlxGa1−xAs-GaAs quantum-well heterostructure, or a superlattice, is highly dependent upon the crystal encapsulation conditions. The activation energy for Al-Ga interdiffusion, and thus layer disordering, is smaller for dielectric-encapsulated samples (∼3.5 eV) than for the case of capless annealing (∼4.7 eV). The interdiffusion coefficient for Si3N4-capped samples is almost an order of magnitude smaller than for the case of either capless or SiO2-capped samples (800≤T≤875 °C). Besides the major influence of the type of encapsulant, the encapsulation geometry (stripes or capped stripes) is shown, because of strain effects, to be a major source of anisotropic Al-Ga interdiffusion.
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Short wavelength Alx'Ga1−x'As-AlxGa1−xAs (x'∼0.85, x∼0.22) quantum-well heterostructure (QWH) laser diodes (well size Lz ≈400 A(ring)) that operate continuously (cw) at 300 K are subjected to hydrostatic pressure ((approximately-less-than)12 kbar). The emission spectrum and the light intensity versus current (L-I) curves are monitored to determine the pressure dependence of the direct (Γ) band gap and the threshold current. The band gap exhibits a linear pressure dependence with a noticeable change in slope at ∼4.5 kbar, similar to previously reported results for AlxGa1−xAs-GaAs QWH diodes. The threshold current increases monotonically with pressure, reflecting the increasing loss of carriers to the X and L bands. The short-wavelength cw limit of the system, i.e., a gain-guided laser with a 400-A(ring) AlxGa1−xAs (x∼0.22) quantum well and no separate waveguide region, is determined to be ∼6980 A(ring).
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: High-pressure studies on high quality AlxGa1−xAs double heterostructure light emitting diodes (LEDs) grown by liquid phase epitaxy (LPE) are presented. The AlxGa1−xAs active region varies in composition from x∼0.25 to x∼0.53, i.e., through the important region of the direct-indirect crossover (x≡xc≈0.45). The pressure coefficient of the Γ conduction band is observed to decrease (∼1 meV/kbar for x∼0.25 to x∼0.53) with increasing Al concentration, which is in accord with alloy disorder and band-edge bowing. Indirect-gap (X) recombination radiation of significant intensity is observed and provides evidence for the high quality of the LPE diodes. High-pressure measurements, and the corresponding increase in energy of the direct band edge and decrease in the indirect band edge, show that the light emission is a strong function of the carrier distribution in the Γ and X conduction-band minima. Comparison LEDs fabricated from a crystal (x∼0.37) grown by metalorganic chemical vapor deposition exhibit nearly similar behavior as the LPE LEDs with application of pressure but with an order of magnitude lower light emission.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 55 (1989), S. 568-569 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ion-implanted In0.1Ga0.9As metal-semiconductor field-effect transistors (MESFETs) have been fabricated on 3 in. GaAs (100) substrates. The structure comprises an undoped InGaAs epitaxially layer grown directly on a GaAs (100) substrate by the metalorganic chemical vapor deposition (MOCVD) technique. Si+28 is ion implanted into the InGaAs layer to form an active channel layer. MESFETs with 100 μm gate width and 0.5 μm gate length are fabricated using standard process techniques. The best device shows a maximum transconductance of 426 mS/mm. From S-parameter measurements, the current-gain cutoff frequency ft is 37 GHz and the maximum available gain cutoff frequency fmax is 85 GHz. These results are comparable to InGaAs MESFETs grown by MBE.
    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. 2436-2438 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Data are presented on the long-term ((approximately-greater-than)8 yr) degradation of AlxGa1−xAs-AlAs -GaAs quantum well heterostructure material because of the instability of underlying (internal) AlAs layers. Material containing thicker (〉0.4 μm) AlAs "buried'' layers (confining layers) is found to be much less stable than material containing thinner ((approximately-less-than)200 A(ring)) AlAs layers. Hydrolysis of the AlAs layers because of cleaved edges and pinholes in the cap layers leads to the deterioration.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 56 (1990), S. 1995-1997 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In0.18Ga0.82As epitaxial layers having a thickness much greater than the established critical thickness of pseudomorphic layers have been grown on GaAs substrates. 0.25 μm gate metal-semiconductor field-effect transistors (MESFETs) are fabricated by silicon ion implantation into the epitaxial wafers. In spite of the large lattice mismatch and the high defect density, the devices show excellent device performance with a maximum extrinsic transconductance of 620 mS/mm and a current-gain cutoff frequency fT of 92.8 GHz. Furthermore, the Schottky gate characteristics of this device are shown to be comparable to those of GaAs MESFETs.
    Type of Medium: Electronic Resource
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