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  • American Institute of Physics (AIP)  (5,187)
  • American Association for the Advancement of Science  (3,274)
  • Nature Publishing Group (NPG)
  • 2010-2014
  • 1985-1989  (8,461)
  • 1986  (8,461)
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  • 2010-2014
  • 1985-1989  (8,461)
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  • 1
    Electronic Resource
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3007-3014 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The design and performance of a magnetic susceptometer for thin films and surfaces is described. The device uses a 14-MHz resonant circuit driven by a tunnel diode oscillator with a superconducting meander line as the inductive element. Magnetic properties of thin films deposited near the line in ultrahigh vacuum at low temperature affect the inductance of the meander line and thus the frequency. The device can detect a susceptibility change equal to that of a change in Fe thickness of 0.03 atomic layers. The minimum detectable change in the diamagnetism of superconducting Pb corresponds to a thickness difference of 10−3 A(ring). The effect of 10−6 atomic layers of Fe can be detected by its depairing effect on a superconducting Pb film. The oscillator circuit including the film being studied is analyzed and the oscillation frequency calculated so that the effect of the various circuit elements can be determined. Suggestions for extending this technique are given.
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  • 2
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3018-3027 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The gas-phase etch products of silicon and XeF2 have been studied as a function of doping and XeF2 flux using molecular beam mass-phase spectrometry. In this experiment the product flux, not the incident reactant beam, is modulated, providing direct information on product identity and velocity, and indirect information on surface reaction kinetics. The data show that although the product ion distributions exhibit little change over the range of experimental conditions used, the neutral products from which the ions are formed vary significantly. More SiF4 desorbs from n-type than p-type silicon at constant flux. The balance of the products mainly consists of Si2F6 and SiF3, the relative amounts of which are flux dependent. These species have not been identified previously as etch products. Average product translational temperatures have also been determined, providing important information on surface interactions during etching. The stable molecules SiF4, Si2F6, and reflected (unreacted) XeF2 all have translational temperatures of approximately 270 K. The free radical SiF3 is much colder, having a temperature of about 200 K. Although etching of the two types of silicon is qualitatively similar, a quantitative comparison reveals intrinsic differences in their reactivity which are not attributable to field effects. The possible origin of these differences is discussed.
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  • 3
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3040-3044 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Optical third harmonic generation measurements by transmission have been performed on thin films of polysilane deposited by a spinning technique with a thickness varying between 0.15 and 0.45 μm. The films have a good optical quality and support large laser power (∼200 MW/cm2 at 1.064 μm). They are transparent in visible and near infrared. The measured average value of cubic susceptibility 〈χ(3)xxxx (−3ω; ω,ω,ω)〉 is equal to (1.5±0.1)×10−12 esu at 1.064 μm. The technique used for the third harmonic generation measurements allows determination of both modulus and phase of χ(3). It is argued that the large value of χ(3) is due to a three-photon resonance at 1.064 μm.
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  • 4
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3045-3055 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Concepts from the theory of interacting continua are employed to develop constitutive relations for liquid and/or gas saturated elastic porous media. The model is formulated by defining intrinsic stress tensors and densities in terms of the partial stress tensors, partial densities, and actual volume fractions occupied by each component. It is assumed that the constitutive law for each component as a single continuum relates intrinsic pressure to intrinsic deformation. Relative motion between the constituents is allowed through simple Darcy-type expressions. The governing equations together with the constitutive relations are used to investigate the propagation of both harmonic and transient pulses. In general three modes of wave propagation exist. In the case of a transient pulse, these modes lead to a three-wave structure. Laplace transform techniques are used to derive closed-form solutions for transient loading for two limiting values of viscous coupling (i.e., weak viscous coupling, strong viscous coupling). Strong viscous coupling results in the coalescence of the three wave fronts into a single front. Solutions for the general case of transient loading are obtained by numerical inversion of the Laplace transforms.
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  • 5
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3035-3039 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The TlBr-TlI (thallium bromoiodide) crystal and its fiber preparation method were studied in order to develop a high power CO2 laser beam fiber. As a result of this study, the most preferable composition for the fiber was determined to be 42 wt. % TlBr. The fiber (0.5 mm in diameter and 1.5 m in length) at that composition had the following excellent characteristics: (1) a high output power of 138 W (70 kW/cm2), (2) a high total transmissivity of more than 93%/1.5 m, and (3) a bending radius of ultimate 3.5 cm.
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  • 6
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3028-3034 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using standard multilayer and effective medium models, we determine microstructures that optimize the near-IR-visible normal-incidence optical transmittance of electrically conducting metal films intended for use as semitransparent contacts for semiconductor devices such as photodetectors or photoelectrochemical converters. Various conditions are considered, including unpolarized and linearly polarized light and electrical conduction both parallel and perpendicular to the surface. For linearly polarized light, the optimum microstructure consists of parallel metal lines of nominally square cross section oriented perpendicular to the polarization vector of the incident light, regardless of the direction of electrical conduction. The line separation and cross-sectional dimensions must both be small compared to the wavelength λ. For unpolarized radiation, the optimum microstructure depends on the direction of electrical conduction. For conduction parallel to the surface, the optimum microstructure again consists of parallel lines with the lines oriented perpendicular to the residual linear polarization, if any, of the incident flux. For conduction perpendicular to the surface, the optimum microstructure consists of cylindrical metal posts of dimension small compared to λ. Expressions are derived that allow the thicknesses and refractive indices of protective antireflection coatings to be calculated to first order in the thicknesses of the metal films. The more general case of antireflection coatings for anisotropic structures is briefly discussed.
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  • 7
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3068-3071 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Neutron time-of-flight techniques have been used to diagnose fuel ion temperatures of inertial confinement fusion plasmas. A new technique for making this measurement using an array of "single-hit'' detectors operating in single-particle counting mode is described. This technique has some potential advantages over previous methods (faster timing, better energy resolution, good sensitivity) and can possibly be further developed to allow detailed measurements of neutron energy spectra to give other diagnostic information, such as fuel areal density (〈ρR〉).
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  • 8
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3056-3067 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The confinement properties of a low-β (average) potassium plasma produced by contact ionization in a spindle cusp magnetic field were investigated. In this configuration, ne≈108–1010 cm−3, Te≈Ti≈0.2 eV, and the ions are weakly magnetized. Electron and ion densities, space potentials, and plasma flow velocities were measured in the ring and point cusps. The leak width of the escaping plasma was measured over a wide range of magnetic field strengths and neutral pressures. The dependence of the leak width on neutral pressure and magnetic field strength is accounted for by a simple model in which the plasma streams out of the cusps along the magnetic field lines while diffusing across the magnetic field due to the combined effects of neutral-particle collisions and Bohm diffusion. Measurements of broadband plasma noise suggest the presence of ion acoustic wave turbulence.
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  • 9
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3081-3087 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An equivalent circuit model is presented for a planar rf plasma reactor. The physical properties of the plasma sheath adjacent to the electrodes are incorporated in the model. The sheath capacitances and the conduction currents through the sheaths are time varying and have a highly nonlinear dependence on the potentials across the plasma sheaths. The model shows that the waveforms of the voltage differences across the sheaths are highly nonsinusoidal and agree with reported measurements.
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  • 10
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1532-1534 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An electrostatic energy analyzer with a deflection angle of 90° and a resolving power of about 4% up to 200 keV was used to analyze the distribution from a cluster ion source. The experiments were carried out with cluster-ion beams of nitrogen extracted from a specially designed cluster ionizer for controlling the cluster sizes. It is shown that the cluster size as large as ∼105 atoms/cluster is measurable with this energy analyzer.
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  • 11
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1535-1537 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report highly sensitive planar, interdigitated Ga0.47In0.54As photoconductive detectors prepared by trichloride vapor-phase epitaxy. The devices exhibit dc gains as high as 104 at 1.3 μm. For a bit rate of 500 Mbit/s a sensitivity of P¯=−35.4 dBm has been measured at 1.55 μm. With devices having unity gain quantum efficiencies of η=33% we obtain ηP¯=−40 dBm matching the highest sensitivity measured with a p-i-n photodetector at similar bit rates. The devices show responsivities in excess of 3000 A/W and detectivities ranging between 1012 and 1013 cm Hz1/2 W−1. These values represent the highest performance that has ever been achieved with photoconductors in this wavelength range.
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  • 12
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1538-1539 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A method for the direct writing of metal features from a metal film supported on an optically transparent substrate using a single pulse from a high-energy excimer laser (193 nm) is presented. The technique eliminates the need for gas-phase precursors in many cases and is an inherently clean process. Results of copper depositions onto silicon substrates are shown to exemplify the technique and a mechanism for the process is proposed.
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  • 13
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1540-1542 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Hydrogenated amorphous carbon films (a-C:H) have been formed by the electron beam decomposition of 100% acetylene (C2H2). The optical and electrical properties of the films depend on the substrate temperature (Ts). Insulating, translucent, and hard films were obtained at Ts≤250 °C. Only sp3C–H and sp3C–H2 stretch were observed by infrared absorption spectroscopy. The a-C:H films deposited at 250 °C were doped by incorporation of B2H6 during growth, and the doping effects of B in the films formed on indium-tin-oxide/glass substrates were investigated. The photo- and dark conductivities strongly dependend on the B doping level.
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  • 14
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1542-1544 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: High sensitivity, high-energy resolution, and the capability to obtain data in situ make ellipsometry a useful tool for addressing a number of problems in thin-film deposition processes. Dielectric functions ε˜=ε1−i ε2 of glow-discharge-produced microcrystalline silicon films (μc-Si) are determined by using spectroscopic ellipsometry (SE). ε2 spectra present a shoulder near 4.2 eV which corresponds to the E2 optical transition observed in crystalline silicon. This peak is not observed in amorphous silicon spectra. c-Si is described as a mixture of amorphous phase, microcrystallites, and voids. The choice of the microcrystalline reference phase is discussed in particular by comparing the microcrystallite volume fraction determined from SE and x-ray measurements. Strong variations in the nature of the material are observed during growth: the density deficiency and the surface roughness both increase as functions of film thickness up to 0.4–0.5 μm.
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  • 15
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3192-3195 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The analysis of Czochralski-silicon annealed in the range 500–800 °C is performed using infrared transmission, electron paramagnetic resonance and admittance spectroscopy measurements. It is shown that the experimental data and especially, new original data obtained with the pulsed admittance spectroscopy technique are consistent with a new model. The "new donors'' effect would in fact be the result of the inversion layer around silica precipitates. This model is demonstrated taking in account the known properties of the Si/SiO2 interface (between precipitates and the silicon crystal). The electrical conduction is shown to be a percolation process through an inhomogeneously conducting material.
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  • 16
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3204-3210 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An emerging new class of superconductor-semiconductor devices requires Ohmic superconducting contacts which do not diffuse deeply into a semiconductor. We developed a contact to GaAs based on ∼150 A(ring) of AuGe covered with ∼2000 A(ring) of Nb annealed in reducing atmosphere at 390–420 °C for 1–5 s. The resulting contact has linear I-V characteristics at all temperatures down to 4.2 K, resistivity of ∼2×10−6 Ω cm2 (∼0.1 Ω mm), and superconducting transition temperature Tc (approximately-greater-than)8 K. Secondary ion mass spectroscopy (SIMS) and transmission electron microscopy (TEM) studies revealed very shallow penetration of the active dopant Ge into GaAs; the upper limit for the thickness of the doped layer with Ge concentration over 1017 cm−3 is estimated as 200–300 A(ring). Gold, a nonactive dopant (deep level) drops to below 1018 cm−3 within the same distance, with the possible tail extending further. Morphology and uniformity of a contact, as revealed in TEM and optical microscopy, is good, owing to the Nb overlayer which prevents AuGe from "balling up'' upon melting. These contacts can be used in low-temperature devices and conventional devices based on GaAs.
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  • 17
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1019-1024 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Thin films of an iron–tellurium alloy were prepared by rf sputtering and characterized by means of x-ray diffraction and Mössbauer spectroscopy. In an immiscible range in equilibrium composition, tellurium atoms were incorporated into iron, distorting the lattice to some extent. Beyond 14 at. % of Te, an amorphous structure appeared. Judging from the metastable superstructures formed at higher substrate temperatures and the covalent nature in the bonding, the kinetic hindrance against the redistribution of the elements due to the local atomic forces during rapid quenching plays a critical role in the formation of amorphous structure in this alloy. In addition, beyond some intermetallic range around 60 at. % Te, an amorphous phase also exists in the tellurium-rich region. The thermal stability was examined by a differential scanning calorimetry; the electrical resistivity is also discussed.
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  • 18
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1038-1041 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using a new model relating dislocation charge to Fermi level, we have simulated the differential capacitance resulting from the inclined dislocations accompanying the misfit dislocations in epitaxial InGaAs/InP samples. The result is a quadratic dependence of charge upon mismatch which is in quantitative agreement with experiments of Macrander et al. for a misfit dislocation segment length equal to about nine times the dislocation spacing.
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  • 19
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1042-1045 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The field-dependent capture-emission process has been studied for double Poole–Frenkel well traps compared with that of single Poole–Frenkel well trap. The emission rate increases with increasing field strength for a single trap. However, for a double trap, it increases to a maximum then decreases with further increasing field due to the barrier lowering and interstate interactions between these two wells. Experimental capacitance deep-level transient spectroscopic data of GaAs samples grown by molecular-beam epitaxy show that when there is a delay in the capacitance transient then there always appear two levels, namely, 0.4 and 0.5 eV. In addition, for both levels, the emission rate increases first to a maximum and then decreases with increasing electric field.
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  • 20
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1059-1064 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Data on ac and dc field dependence of the conductivity of semi-insulating GaAs crystals are reported. The existence of long-range potential fluctuations in these samples has been previously reported. Field-enhanced conductivity results from the decrease of the maximum depth of the wells due to barrier lowering, up to a critical field at which the effect of potential fluctuations disappears. The transient behavior is also discussed.
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  • 21
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1071-1073 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetoresistance skewness effect (change of the principal directions of electrical resistivity) appears when a magnetic field of arbitrary direction is applied on the examined material. This effect is useful for the magnetoresistance coefficients determination. A complete investigation of the skewness effect requires additional experimental facilities, such as the rotation of the sample and the contact system, which in some cases are impossible or very difficult to obtain. In this work the importance of the (110) and (111) planes of cubic crystals for such measurements is shown. For this purpose the elements of the resistivity tensor in the systems of reference, used in these planes, are correlated with those in the basic system of the (001) plane.
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  • 22
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1104-1113 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A construction method for determining the domain structure in ideally soft-ferromagnetic cylindrical objects with plane-parallel top and bottom surfaces of arbitrary shape is presented. The self-consistent theory is confined to two-dimensional solenoidal dipole distributions in which the dipoles are parallel to the top and bottom surfaces. It is proved that the basic domain structure is uniquely defined in simply connected objects, while an extra criterion has to be added in order to guarantee the uniqueness in the multiply connected ones. The treatment is based on differential geometrical principles. The object edge is partitioned into segments, in which each segment is situated in between two adjacent edge points where the radii of curvature of convex edge segments are locally minimal. To each edge segment, a region is attributed, in which M is uniquely specified by the course of M along that edge segment. In the cross section of regions corresponding to different edge segments, domain walls provide an adequate separation of the dipole distribution imposed by these segments. The extremities of these domain walls are found in the singular points of the evolute corresponding to the extremities of the edge segments and in the points where a number of walls meet. It is proved that the basic domain structure is the locus of centers of all circles inside the object that touch the object edge at at least two points. A number of experimentally observed basic structures are given, and the relevance of the definition of basic structures in multiply connected objects is examined. OFF
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  • 23
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1135-1138 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report electrolyte electroreflectance studies of the ternary semimagnetic semiconductor Hg1−xMnxTe for compositions below x=0.2. The dependence of E1 and E1+Δ1 transition energies on the composition was determined on the basis of the low field approximation. The present results are compared and discussed in relation to experimental data obtained previously and the theoretical predictions reported in the literature.
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  • 24
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    Journal of Applied Physics 60 (1986), S. 3303-3308 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An overdamped plasmon-LO phonon coupled mode in undoped GaP crystals has been observed under high excitation condition. We have studied the relaxation process of the coupled mode in the time range of nonoseconds using a time-resolved Raman scattering technique at 81 K. The decay time of photocreated free carriers has been estimated from line-shape fitting of the coupled mode in the time-resolved Raman spectra. The decay time obtained from the Raman study has been compared with the value obtained from luminescence measurements. The plasmon hybridized with the LO phonon is found to be a gaslike electron-hole plasma.
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  • 25
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3323-3326 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: The oxidation of TaSi2 and Ta2Si surfaces prepared under ultrahigh vacuum conditions has been studied by x-ray photoemission spectroscopy. For both silicides, Si and Ta oxides comprise the native oxide formed at room temperature. Annealing at 550 °C induces a solid state reaction within the native oxide. Ta2O5 is partially decomposed, and the liberated oxygen bonds to Si. This reaction and the influence of the silicide stoichiometry are discussed.
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  • 26
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    Journal of Applied Physics 60 (1986), S. 1189-1205 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: A series of experimental measurements of the yield of O3 in nuclear-induced O2 and O2-SF6 discharges are reported. The discharges were created by bombardment with energetic particles from the 10B(n,α)7Li reaction. Continuous irradiation at dose rates of 1015–1017 eV cm−3 s−1 and pulsed irradiation (∼10 ms FWHM) at a peak dose rate of ∼1020 eV cm−3 s−1 were conducted. At the lower dose rates, the addition of SF6 generally increased the ozone yield due to the slowing of ozone destruction by negative oxygen and ozone ions. In contrast, at the high dose rates, the ozone concentration decreased due to SF6 suppression of atomic oxygen formation by ion–ion recombination. A numerical model was developed and tested against experimental conditions. This model indicates that the steady-state ozone concentration was limited by the reaction O−3+O3→2O2+O−2 with a rate coefficient of ∼1×10−12 cm3 s−1. In addition to dose rate effects, pressure and temperature effects on ozone production are discussed and methods for increasing the ozone yield are suggested.
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  • 27
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1212-1214 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The primary ion beam column of a combined secondary ion/sputtered neutral mass spectrometer is used for in situ ion implantation of precise amounts of a given species superimposed as an internal standard upon its residual concentration. Subsequent depth profile analysis is done in the instrument after switching to another primary projectile. It is shown that concentrations can be determined with an accuracy of 4% from the known in situ implanted fluence by comparing the original and the added amounts. In this way, the helium concentration in a silicon sample (produced by external implantation) and the interfacial oxygen concentration between an amorphous and crystalline Si layer are determined quantitatively.
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  • 28
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    Journal of Applied Physics 60 (1986), S. 3376-3378 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: A new process—simultaneous implantation and diffusion annealing—has been developed for the formation of pn junctions in compound semiconductors. It combines implantation and diffusion, by using doped SiO2 spin-on films simultaneously as a surface protection during activation of the implants and as a diffusion source. Only a single annealing step is necessary, which is very important for a careful heat treatment of existing semiconductor structures. Examples are presented for GaInAs. The n level formed by Si implantation varies from 1×1017 cm−3 to 6×1018 cm−3, with an increasing dose. The p level is adjusted to about 1×1019 cm−3 by the amount of Zn salt in the spin-on solution. The position of the pn junction is shifted by the annealing step.
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  • 29
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    Journal of Applied Physics 60 (1986), S. 3384-3384 
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  • 30
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2655-2658 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: A statistical consideration based upon a theory of microscopic molecular kinetics is developed to describe the time-dependent fracture process for oriented polymers. The interrelation between the macroscopic fracture strength and the microscopic behaviors is formulated with the aid of a double Fourier series expansion. The microscopic behavior in the vicinity of a point is expressed in the form of a spherical function which can be expanded into a series of symmetric tensorial terms. Subsequently, the fracture strength of polymers is evaluated in terms of both time and molecular orientation. By taking account of the individual values of the directional fraction of integrity, the time to fracture and the most probable direction of fracture within any volume element in a medium are predicted.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3381-3383 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: Multiple magnetic films composed of alternating magnetic and nonmagnetic layers may have a layered domain structure when there is no exchange coupling through the nonmagnetic layers. As demonstrated for an Fe-Cu multilayer thin film, this structure can be made visible in Schlieren images using a particular variant of Foucault–Lorentz transmission electron microscopy.
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  • 32
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2651-2654 
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    Topics: Physics
    Notes: Acoustic emission (AE) has been coupled with slow crack propagation experiments in polystyrene to probe the mechanisms of damage and fracture. The single AE active mechanism recorded during slow crack growth is probably caused by failure of the craze fibrils in the craze zone at the propagating crack tip. The AE event rate and the AE energy release rate varied linearly with the crack speed indicating that the AE depends only upon the amount of fracture surface created independent of the crack speed. Since the duration of the AE was less than 1% of the total time of the experiment, it is concluded that crack propagation is discontinuous even at the highest crack speeds investigated.
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  • 33
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2708-2712 
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    Topics: Physics
    Notes: A confocal interference microscope incorporating an electro-optic phase modulator has been used to make simultaneous measurements of the inphase and quadrature components of the confocal signal as a reflecting surface is scanned axially, the so-called V(z) response. Comparison with previously published theoretical predictions is seen to be favorable.
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  • 34
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 973-979 
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    Topics: Physics
    Notes: Deep level transient spectroscopy of p–n junctions, Schottky barriers, or metal-oxide-semiconductor (MOS) capacitors is widely used to obtain the concentrations of defects and their profiles in semiconductors. The use of this technique for profiling presents several difficulties, some of which have not been taken into account in the works previously published. The aim of this paper is to describe the exact analysis which should be performed to obtain correct profiles. The analysis is tested on a constant defect profile, induced by electron irradiation in n-GaAs, in order to illustrate the effect of each correction. It is then applied to defect profiling of a silicon MOS capacitor and on the EL2 defect in annealed GaAs.
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  • 35
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 991-1001 
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    Topics: Physics
    Notes: The metallurgical examination of solid-state reaction between nickel thin films and single-crystal GaAs substrates and the resultant electrical properties of the contacts are reported. Annealing at 100–300 °C in forming gas led to formation of a metastable hexagonal phase Ni2GaAs which was stabilized due to its epitaxial growth on (001) and (111) GaAs substrates, as follows: (101¯1)Ni2GaAs(parallel)(001)GaAs and (0001)Ni2GaAs(parallel)(111)GaAs. Nickel atoms were found to be the dominant diffusing species during the ternary phase growth. Ni2GaAs is stable on (111)GaAs up to at least 600 °C, compared to 350 °C on (001)GaAs. The larger stability on (111) is explained by the better epitaxial match found in this case. Reaction on (001)GaAs in the temperature range of 350–550 °C resulted in decomposition of Ni2GaAs by NiAs precipitation. After annealing at 600 °C the reacted film was composed of two phases: NiGa and NiAs. The electrical properties of the contacts were correlated to the phase interfacing the substrate. The Ni2GaAs formed rectifying contact with a barrier height of 0.84 eV, whereas when NiGa and NiAs were at the interface an ohmic behavior was observed.
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  • 36
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2717-2720 
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    Topics: Physics
    Notes: The operating rotational-vibrational transition lines are observed in a pulsed transversely excited atmospheric pressure CO2 laser with a separated intracavity CO2 gas absorber. The laser operates a dominant 10.6-μm P-20 and P-18 line in a low pressure of CO2 cell and a single-line operation of P-20 line at more high pressure. In a high pressure, the laser does not operate the 10.6-μm P-20 and P-18, but it operates the single-line operation of 10.6-μm R-14, R-18, P-22, and 9.4-μm R-12, and in multiline oscillation, of various combinations of these lines and 10.6-μm R-16, according to the temperature of this gas absorber. The results are attributed to the absorbing mechanism of the CO2 gas.
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  • 37
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2739-2753 
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    Topics: Physics
    Notes: A model of cw argon ion lasers excited by low-energy (50–200 eV) direct current electron beams at current densities between 1 and 50 A/cm2 has been developed. The electron energy distribution in the electron-beam-created plasma is calculated by numerically solving the Boltzmann equation for electrons. Optical gains, powers, and laser efficiences were computed for the 4765-, 4880-, 4965-, and 4658-A(ring) Ar ii transitions for a wide range of discharge conditions. Laser efficiencies comparable to those of a conventional Ar ii laser (∼3×10−4) are predicted for these laser transitions when electron beam excitation is used.
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  • 38
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2766-2770 
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    Notes: A prototype of a new class of thyratrons having a linear geometry is described and measurements of excited state densities in the thyratron plasma using hook method spectroscopy are presented. The linear thyratron is conceptually scalable to high currents by lengthening it in the axial dimension without changing any other critical scaling dimension (such as the cathode-control grid distance). The prototype linear thyratron is a tetrode having a 3 cm×10 cm slotted dispenser cathode with an effective area of 80 cm2. The thyratron has separately switched 25 kV and 10 kA, with a maximum dI/dt of 1.3×1011 A s−1. Using helium as the working gas, maximum excited state densities of 6×1012 cm−3 were measured for the 23P state.
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  • 39
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2778-2782 
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    Notes: The potential of ferroelectric liquid crystals for application as pyroelectric infrared detectors is examined. The liquid crystals studied belong to a family of biphenyl and phenylbenzoate esters. It is found that even within this first liquid-crystal family examined, the materials figure of merit compares well with ferroelectric solid materials commonly used for infrared detection and imaging. Because they permit very simple and flexible device design, liquid crystals are attractive candidates for these applications. However, for low-frequency applications, attention must be paid to the reduction of thermal loading by the cell walls.
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  • 40
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2788-2796 
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    Notes: The conductivity enhancement in polydiacetylene (PDA) crystals due to chemical doping and ion implantation was measured and analyzed in relation to their spin concentration and photocurrent decay based on the structural and optical information obtained through infrared and visible reflectivity spectra. A conductivity jump was observed upon slight increase of the spin concentration at low doping levels of chemically doped PDAs, suggesting the formation of spinless carriers in chemically doped PDAs, as in trans-polyacetylene and poly(p-phenylene). In contrast, in ion-implanted samples, a great difference in the magnitudes (by more than five orders of magnitude) was observed between the conductivity enhancement for two PDAs having different side chain species. Furthermore, the photocurrent decay time measurements reveal different distributions of implantation-induced trap levels between ion-implanted poly [2,4-hexadiyne-1,6-diol-bis-(p-toluene sulfonate)] (PTS) and poly[2,4-hexadiyne-1,6-di(N-carbazolyl)] (DCH). A conduction mechanism which could explain the significant difference in conductivity enhancement between PTS and DCH is suggested. Because the enhanced conductivity by ion-implanted PTS showed no orientational effect associated with the polymer chain direction, a conductive path and network formation by the implantation-induced defects is more plausible for the conduction mechanism than carrier introduction into the backbone chain band from side chain defect levels.
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  • 41
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 534-537 
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    Topics: Physics
    Notes: The effect of device parameters on static and dynamic properties of inhomogeneously current-injected bistable semiconductor lasers has been analyzed. It is shown that in addition to the fraction of current injection region in the cavity, the device parameters, such as dopant concentration in active layer, facet reflectivity, and cavity length, affect the hysteresis width and threshold current. The mechanism of transition between lasing and nonlasing states is discussed, in which a new interpretation is given about the bias dependence of switch-on delay time and the driving condition for switching off is clarified. The carrier increasing rates due to the bias current and dopant concentration in the active layer are dominant factors for the switching on and switching off, respectively.
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    Journal of Applied Physics 60 (1986), S. 559-562 
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    Notes: A new physical explanation for the operation of the Orbitron maser is presented. The Orbitron experimental results are shown to be in agreement with the prediction of the theory of amplification by stimulated emission of bremsstrahlung.
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    Journal of Applied Physics 60 (1986), S. 2797-2805 
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    Notes: We have measured implanted and annealed depth distributions for the two elements adjacent to Si, Al, an acceptor in Si, and P, a donor in Si, using secondary ion mass spectrometry for the atom depth distributions and differential capacitance-voltage profiling for the acceptor or donor depth distributions. Ions of Al or P were implanted into Si amorphized by Si implantation, into crystalline Si in a random orientation, and channeled into the three principal low index directions of the Si lattice, 〈100〉, 〈110〉, and 〈111〉. The ion energies were 25, 50, 75, 100, 150, 200, 300, 400, or 600 keV and the ion influences were 3×1013, 3×1014, and 3×1015 cm−2 for the atom depth distributions, and 1.5×1012 cm−2 for the acceptor and donor profiles. Pearson IV fitting was used to obtain the values of the first four moments of the random depth distributions, the projected range Rp or μ, the range straggle ΔRp or standard deviation σ, the skewness γ1, and the kurtosis β2. For the channeling orientations, the maximum channeling range or the depth of the channeled peak are plotted versus ion energy, and values of the energy exponent p are determined. The random ranges Rp and profiles are compared for amorphized and crystalline Si and compared with range calculations; the profiles in amorphized Si are modified Gaussians as predicted by theory, with no channeling tails, and the profiles in crystalline Si have significant channeling tails that are not easily fit to a modified Gaussian. The different channeling profiles for Al and P are illustrated and explained in terms of their different electronic stopping and ion size. The effects of 30-min furnace annealing at 550 and 800 °C are shown for implanted Al profiles; significant redistribution occurred, and in a manner that depends on Al atom density and whether the Si is amorphous or crystalline. Furnace annealing at 875 and 925 °C or rapid radiant annealing at 900 °C caused no redistribution of P profiles implanted at room temperature.
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  • 44
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2810-2813 
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    Notes: High and low densities of 300-keV Ag atoms were implanted into (100) and (111) crystalline and self-amorphized Si, and annealed at temperatures from 100 to 900 °C and for various times. Silver depth distributions were profiled using secondary ion mass spectrometry. Regrowth locations and rates of the various damaged regions were measured with good sensitivity via the Ag profiles, which resulted from the retention of Ag atoms by defect complexes and their release upon annihilation of the defect complexes during annealing. The following results were obtained for (100) Si: regrowth toward the surface of the 0.3-μm-thick amorphized layer beginning at about 450 °C, up to 650 °C, with a regrowth rate of (18±2) A(ring)/°C or 5.2 A(ring)/min at 530 °C; regrowth of the amorphous-crystalline interface region at 850 °C at a rate of (8±1) A(ring)/min. The presence of 2×1019 cm−3 Ag atoms retards the regrowth rate of (100) Si by a factor of 2. Two separate, but closely spaced regions of residual damage in the amorphous–crystalline interface region were revealed. Regrowth of (111) Si occurs uniformily in depth throughout the amorphized region, consistent with the growth of polycrystalline or microtwinned Si in this region as seen by transmission electron microscopy.
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    Journal of Applied Physics 60 (1986), S. 2823-2830 
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    Notes: Nucleation kinetics and spatial distribution of spherulitic clusters can be determined from growth rate and cluster size measures. This method presented here was applied to the nucleation of disk-shaped PtSi clusters which grow in solid phase on nitridized Si substrates. It shows that the nucleation occurs in three modes corresponding to three kinetic regimes. A first nucleation phenomenon occurs at the beginning of the annealing on low-density (∼102 cm−2) preferred sites which are not randomly distributed in the plane and probably linked to defects. Then a steady state of nucleation on preferred sites, which are randomly distributed with a density of about 104 cm−2, is observed. A third phenomenon of nucleation is distinguished by a nucleation rate which exponentially increases with time. This "avalanche state'' is linked to the presence of microclusters, the density of which can reach 107 cm−2. It depends on temperature and on the ratio of platinum layer thickness to silicon nitride thickness.
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  • 46
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2924-2931 
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    Notes: A previously developed model for the angular dispersion of Raman scattering power from the surface of absorbing centrosymmetric cubic materials is extended to absorbing materials of the zinc blende type. Independent expressions have been obtained which give the scattered power due to the longitudinal and transverse long-wavelength optical phonons as a function of external scattering geometry parameters; from these calculations, it has been found that the ratio of the scattered powers shows significant dependence on the angles of incidence and detection. These results provide a quantitative method in assessing the effects of choosing an approximate rather than the exact backward scattering geometry. Experimental results obtained from GaAs are in very good agreement with the predictions of the model. Examples of physical situations are given where angular dispersion corrections become necessary.
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    Journal of Applied Physics 60 (1986), S. 2944-2948 
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    Notes: The absorption and scattering (reflection plus transmission) energy spectra of normally incident 24.8-MeV electrons on C, Al, Cu, and Pb foils have been calculated using an updated version of the relativistic Monte Carlo electron/photon transport code sandyl. The theoretical results are compared with recent experimental data and good agreement is found.
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  • 48
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    Journal of Applied Physics 60 (1986), S. 639-642 
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    Notes: Trap levels in ∼2-μm In0.2Ga0.8As (94 A(ring))/GaAs(25 A(ring)) strained-layer superlattices, suitable for optical waveguides, have been identified and characterized by deep-level transient spectroscopy and optical deep-level transient spectroscopy measurements. Several dominant electron and hole traps with concentrations ∼1014 cm−3, and thermal ionization energies ΔET varying from 0.20 to 0.75 eV have been detected. Except a 0.20-eV electron trap, which might be present in the In0.2Ga0.8As well regions, all the other traps have characteristics similar to those identified in molecular-beam epitaxial GaAs. Of these, a 0.42-eV hole trap is believed to originate from Cu impurities and the others are probably related to native defects. Upon Si implantation and halogen lamp annealing, new deep centers are created. These are electron traps with ΔET=0.81 eV and hole traps with ΔET=0.46 eV. Traps occurring at room temperature may present limitations for optical devices.
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    Journal of Applied Physics 60 (1986), S. 650-656 
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    Notes: Decreasing device dimensions will cause an increasing internal field strength in a semiconductor device. The average carrier energy is different from the thermal equilibrium value 3/2 kT. Modification of current transport is considered on different levels of approximation. In a local approximation we derive a field-dependent carrier mobility and temperature from a more general self-consistent formulation. Numerical estimation of hot-electron effects are given for a realistic n-channel metal-oxide-semiconductor field-effect transistor of various channel lengths. It is shown that both high-field and field-gradient effects will contribute.
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    Journal of Applied Physics 60 (1986), S. 673-676 
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    Notes: We calculated the shift of Fermi energy EF with temperature, using a model density of states for hydrogenated amorphous silicon (a-Si:H) similar to that of deep level transient spectroscopy results, by a numerical method. The conductivity σ was calculated from the calculated EF as a function of temperature. It was found that some features of anomalous transport phenomena of n-type a-Si:H such as kinks or the continuous bending of log σ vs 1/T curves and the Meyer–Neldel-type preexponential factors can be explained, at least in part, by the statistical shift alone.
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    Journal of Applied Physics 60 (1986), S. 677-680 
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    Notes: Both secondary ion mass spectrometry and transmission electron microscopy have been used to characterize Au–Ni–Ge and Au–Ag–Ge ohmic contacts to modulation-doped GaAs/AlGaAs heterostructures. The time periods for alloying the contact were kept to a minimum (〈25 s) in order to obtain controlled diffusion of Ge into the semiconductor. Structural analysis shows that a stable alloy contact is formed after 3 s of alloying at temperatures above the Au–Ge melting point. There were no major structural or compositional changes observed with longer alloying times. The Ge-rich region has a tendency to regrow epitaxially on the GaAs after alloying, as shown by high-resolution electron microscopy.
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    Journal of Applied Physics 60 (1986), S. 2205-2217 
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    Notes: A study is made of the scatter of low-frequency electric and magnetic dipole fields from a perfectly conducting sphere coated with a thin and lossy dielectric and immersed in an infinite and lossy medium. Infinite series solutions are obtained for the incident and scattered electric and magnetic fields. The solutions are evaluated numerically for various coating parameters and orthogonally oriented transmitter-receiver systems traveling along linear paths beneath the coated sphere. Results are compared with those obtained for the scatter of dipole fields from an uncoated sphere and used to determine the extent to which the scatter of low-frequency electric and magnetic dipole fields may be used to detect such objects and to obtain information about the nature of the coating.
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    Journal of Applied Physics 60 (1986), S. 2250-2255 
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    Notes: The problem of heating a homogeneous slab of material induced by time-dependent laser irradiance is studied. An exact solution for the temperature distribution of the slab is obtained using the Fourier series expansion technique. The temperatures for the front and rear surfaces are also obtained. The case of time-independent laser irradiance is considered. The exact expressions for the thermal penetration depth and the critical time required to initiate melting (i.e., damage) are recovered and compared with the published data for this special case.
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    Journal of Applied Physics 60 (1986), S. 2238-2249 
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    Notes: The composite resonator consists of a uniform thin layer etched in a small well-defined region of a semiconductor wafer to form a diaphragm, upon which is deposited a thin piezoelectric film along with the electrodes to form a resonant region directly on the wafer. Although the composite resonator, which operates in an essentially thickness-extensional mode, can be constructed to employ energy trapping, almost all existing experimental work in the literature is for the case when trapping is not present. All previous analytical work expressly ignores radiation into the bulk semiconductor except one treatment, which unrealistically ignores the junction between the etched diaphragm and the bulk semiconductor. In this work an analysis of the composite resonator driven into essentially thickness-extensional vibrations by the application of a voltage to strip electrodes is performed. The analysis includes all radiating plate waves in the thick portion of the semiconductor. The solution consists of a sum of terms satisfying all differential equations and boundary conditions on major surfaces exactly and uses the appropriate variational principle of linear piezoelectricity to satisfy the remaining conditions approximately. For the case of the aluminum–nitride film on gallium arsenide the Q is calculated for both the configuration in which the film ends at the edges of the electrodes and in which it continues to the edges of the etched diaphragm when trapping is not present and for the latter configuration when trapping is present. The calculations show that when trapping is not present the Q is a very rapidly varying function of the ratio of the composite resonator thickness to the wafer thickness and that the range of variation is very large, i.e., between one and two orders of magnitude. The calculations also reveal that when trapping is present the Q is always much larger and its range of variation much smaller than when trapping is not present.
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    Journal of Applied Physics 60 (1986), S. 2316-2320 
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    Notes: Alloys of Ga1−xAlxAs were implanted with As and Be ions at room temperature, and the implant damage was studied as a function of the depth from the surface by Raman scattering. The arsenic implant led to the amorphization of the AlAs and GaAs constituents of the mixed crystal. The Be implant, on the other hand, amorphized the AlAs constituent only while damaging the GaAs.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2351-2356 
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    Notes: The deposition kinetics of hydrogenated amorphous silicon (a-Si:H) from a SiH4 glow-discharge plasma have been investigated by examining the diffusion of SiH3 monoradicals in the discharge-free space within a triode reactor. This experiment suggests that the SiH3 radicals are responsible for about 37% of the total deposition rate of a-Si:H in a conventional SiH4 glow-discharge process. The contribution of other radicals and atoms to the deposition rate is also discussed through the analysis of reaction-rate constants.
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    Journal of Applied Physics 60 (1986), S. 2372-2376 
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    Notes: Experimental evidence indicates that coherent multilayer structures (strained superlattices) can be grown in a damage-free state when the thickness of the layer is less than a critical value. The resistance of such structures to subsequent damage by dislocation or crack injection is examined in the present study. The structures are determined to exhibit damage resistance that decreases as either the layer thickness or the coherency strains increase.
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    Journal of Applied Physics 60 (1986), S. 2218-2225 
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    Notes: Three separate variations of a vibrational energy nonequilibrium flow of a supersonic expansion of a CO2-N2-H2O mixture through a gasdynamic laser nozzle are examined to demonstrate the relative importance of the error induced by neglecting various kinetic effects and anharmonicity. The significance of each important collisional relaxation mechanism is specifically demonstrated by comparing the error induced due to neglecting each effect, with the variation in the predicted inversion obtained by using three different sets of empirical relaxation time equations. Since the net effect of each relaxation mechanism is to drive the system towards equilibrium, thus decreasing the inversion, it is suggested that the application of the parallel mixture rule in a kinetic model to include different relaxation paths is incorrect. Two kinetic models are solved by first assuming the molecules to be harmonic oscillators and then using the Morse oscillator model to demonstrate the significance of anharmonicity. The influence of the reservoir temperature in establishing the significance of each kinetic effect on the inversion and small-signal gain is calculated.
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    Journal of Applied Physics 60 (1986), S. 2256-2259 
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    Notes: The thickness of the molten layer and the rate of melting induced by constant laser irradiance in a solid slab is studied. The study is carried out for time intervals less than or equal to the transit time, defined as the time taken for the temperature of the rear surface to change from ambient. The integral form of the heat conduction equation with the boundary condition at the interfacial surface between the liquid and solid phases together with a suggested model for the melting process is used to obtain an exact solution for the considered problem. Computations for a slab of aluminum of thickness 3×10−4 m subjected to laser irradiance of value q0=1014 W/m2 are carried out. It is found that the rate of melting after a certain delay time attains a constant value.
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    Journal of Applied Physics 60 (1986), S. 2266-2271 
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    Topics: Physics
    Notes: This paper discusses digital image processing techniques suitable for use with the velocity interferometric records obtained from shock-wave experiments using ORVIS (optically recorded velocity interferometer system). An ORVIS system is capable of measuring shock events with subnanosecond time resolution, the data consisting of fringe motion (proportional to the impacted material velocity) recorded with a streak camera. Two image processing methods are described which permit the determination of accurate velocity-time data from the records. The first, based on global analysis of the records, requires no operator intervention during reduction of the data, but breaks down when records show very rapid acceleration of the target under observation. The second, based on a thinning algorithm, can be used to treat rapid acceleration data and data in which the fringes are less than ideal. It requires operator intervention in some cases. The two techniques are shown to agree well when applied to the same data.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2285-2295 
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    Topics: Physics
    Notes: This paper presents self-consistent steady-state solutions of the space charge, transmitted current, and return currents in diodes with electron injection from the cathode and unlimited field emission of electrons and ions from both electrodes. Time-dependent particle simulations of the diode operation confirm the analytical results and show how these steady states are reached. The results are applicable to thermionic diodes and to photodiodes.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2304-2309 
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    Topics: Physics
    Notes: This paper describes some numerical calculations for the temperature fields associated with laser melting and subsequent recrystallization of a thin silicon film on a conductive (glass) substrate. Particular attention has been paid to the change in the material properties with temperature and to the change in reflectivity which occurs when the silicon undergoes a phase change. Thin film optics have also been incorporated into the solution. Physical arguments and experimental observations suggest the possibility of the coexistence of liquid and solid phases. Here an attempt has been made to simulate this process numerically by using a scheme based on the enthalpy formulation. The numerical algorithm given allows the representation of regions where both the liquid and solid phases coexist. This method of solution has not been applied to cases where the reflectivity changes are considered in the "slush'' formation. This is the first numerical simulation to include this effect.
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  • 63
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2321-2326 
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    Topics: Physics
    Notes: Photo-induced dry etching of silicon with chlorine is studied by measuring mass spectra and time-of-flight (TOF) distributions of the particles desorbed from a chlorinated target during irradiation with 308- and 248-nm photons. The detected masses are Si, SiCl, SiCl2, and SiCl3. The measured TOF spectra can be fitted with Maxwell–Boltzmann-like distributions. The temperatures obtained by these fits depend on laser power and chlorine pressure. A higher laser power or gas pressure results in a higher temperature. Activation energies for desorbing Cl, SiCl, and SiCl2 are obtained. Possible mechanisms to explain the results will be discussed. Etching of rough silicon is much more efficient than the etching of polished silicon. The maximum etch rate obtained is 30 A(ring) per laser pulse. No difference is found between p- and n-type silicon.
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  • 64
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2327-2342 
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    Topics: Physics
    Notes: Three-dimensional linear equations of motion for small vibrations superposed on thermal deformations induced by steady, uniform temperature change in quartz are obtained. The material properties of quartz, such as the elastic stiffnesses and thermal expansion coefficients, are assumed temperature dependent and expressible by third-degree polynomials in temperature change. From the solutions of third-order perturbations of these equations for the thickness resonances of infinite quartz plates, six values of the effective third temperature derivatives of elastic stiffnesses C˜(3)pq are calculated by the use of the measured temperature coefficients of frequency by Bechmann, Ballato, and Lukaszek [Proc. IRE 50, 1812 (1962)] for various doubly rotated cuts and the values of the first temperature derivatives C(1)pq and the effective second temperature derivatives C˜(2)pq obtained in a previous study. An infinite system of two-dimensional equations of motion is derived by Mindlin's method of power-series expansion for crystal plates subject to a steady, uniform temperature change. Four equations, governing the coupled thickness-shear, thickness-twist, thickness-stretch, and flexural vibrations, are extracted from the infinite set and employed to study the frequency-temperature behavior of thickness vibrations of finite SC-cut quartz plates with a pair of free edges. Changes in the thickness-shear resonance frequencies as a function of temperature are predicted and plotted for various values of orientation angles θ and φ, and length-to-thickness ratio a/b. Effects on the frequency-temperature behavior of the plates due to changes in the values of θ, φ, and a/b are observed and discussed.
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  • 65
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 4090-4094 
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    Topics: Physics
    Notes: Use is made of the T-matrix method to examine the effect of surface profile modeling errors in studying the scalar scattering responses of impenetrable, periodic surfaces. It is shown that even small errors can alter the maximum surface slope significantly, thereby taxing the resources of numerical procedures and severely limiting their scopes of applicability. However, it is possible that the power diffraction coefficients are not very different when calculations are made with and without these errors. Possible implications for using such methods in order to understand the scattering behavior of fractal surfaces are discussed.
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  • 66
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    Journal of Applied Physics 60 (1986), S. 2386-2395 
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    Notes: We report here computer calculations of current-voltage characteristics, impedance, and noise in space-charge-limited (SCL) flow in SiC crystals composed of layered polytypes. The results are compared with previously reported experimental data [Part I of the same title, J. Appl. Phys. 58, 1562 (1985) and Part II of the same title, J. Appl. Phys. 58, 1571 (1985)], and are found to give excellent agreement. In contrast to the analytical computations reported previously, the diffusion term is not neglected. It is shown to play an important role at low and moderate bias voltage. Also, these computations show clearly that while many types of traps are present, ranging from 63 to 367 meV below the conduction band, at a given temperature only one trap determines the I-V characteristics. On the contrary, in the impedance and in the generation-recombination noise spectra, many traps show up simultaneously and must be taken into account. In general, the main features of the analytical theory developed by Van Vliet et al. are confirmed.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2401-2405 
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    Notes: The short-circuit current in a polycrystalline semiconductor may be distorted by the local defects or by the local interface defects (variation of the effective recombination velocity at the grain boundary). These defects can be determined from the steady-state electron-beam-induced current. The expression for the contrast coefficient C for the above defects are given. In the analysis, the generation of the excess carriers is assumed to be uniform in a sphere tangent to the semiconductor surface. The p-n junction is placed on the surface of the semiconductor.
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    Journal of Applied Physics 60 (1986), S. 2419-2421 
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    Notes: Electrical conduction data from undoped low-pressure chemically vapor deposited polycrystalline silicon thin films at room temperature and above are presented. The physical mechanisms pertinent to general current-voltage characteristics are experimentally interrogated from three different viewpoints. In the nonlinear current-voltage region, the sheet resistance Rs is shown to vary drastically depending on the device aspect ratio for given applied electrical field E¯. The nonscalability of Rs with respect to E¯, the temperature behavior of Rs, and the photoconductivity data indicate that the nonlinear current-voltage behavior cannot be attributed to field-enhanced conductivity. Other possible mechanisms responsible for observed nonlinearity are discussed.
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    Journal of Applied Physics 60 (1986), S. 2445-2452 
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    Notes: Electrical and microstructural changes of coevaporated V75Si25 alloy thin films have been studied as a function of temperature from room temperature to 830 °C. In situ resistivity measurements, hot-stage transmission electron microscopy, Rutherford backscattering spectroscopy and the Seeman–Bohlin glancing angle incidence x-ray diffraction technique were applied. Upon heat treatment at a heating rate of 8 °C/min, a sharp decrease in resistivity occurs at ∼670 °C which results from an amorphous to crystalline phase transformation. The crystallized phase was identified as V3Si. The mechanism of transformation is random nucleation at a rapidly decreasing rate and a fast quasi-isotropic growth. The kinetics of crystallization have been studied by utilizing electrical resistivity measurements during isothermal heat treatment. Six different temperatures between 570 °C and 630 °C were adopted. The apparent activation energy (∼3.6 eV) obtained from isothermal measurements was found to be in agreement with that obtained from nonisothermal treatments at varying rates of heating. The distinct change of the Avrami mode parameter from 4 to 2 at a constant value of t/τ during the process of crystallization is not immediately understood.
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    Journal of Applied Physics 60 (1986), S. 2050-2057 
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    Notes: Interface properties of plasma-enhanced chemical-vapor-deposited dielectric SiON on GaAs systems pretreated by NH3 plasma were studied. The effects of the process parameters in the NH3 plasma pretreatment, such as total pressure, radio-frequency power, substrate temperature, NH3 flow rate and pretreatment time, were investigated by the measurements of Auger electron spectroscopy, Raman spectroscopy, current-voltage, and capacitance-voltage characteristics. The transient region width and the surface strain field, surface leakage current, hysteresis, and degree of Fermi-level pinning evidently related to interface properties, are increased with increasing total pressure, decreased with increasing radio-frequency power, substrate temperature, and pretreatment time, and independent of NH3 flow rate. The physical and electrical properties of SiON/GaAs interface have been significantly improved under an optimum NH3 plasma pretreatment condition. The correlation of these parameters in pretreatment process with the interface properties including interdiffusion, surface strain field, surface leakage current, hysteresis, and Fermi-level pinning are discussed.
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    Journal of Applied Physics 60 (1986), S. 2103-2105 
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    Notes: A silicon-on-insulator structure was formed by implanting 2×1018 oxygen ions cm−2 into crystalline silicon at 150 keV. A systematic investigation of the effect of annealing temperature was carried out by annealing for 6 h at temperatures of 1150, 1200, 1250, and 1295 °C. The microstructure and oxygen-concentration profile were investigated by using cross-sectional transmission-electron microscopy and Auger analysis. Changes were observed to occur throughout this annealing-temperature regime. After the highest annealing temperature, a single-crystal top silicon-layer of 150 nm with 4×109 dislocations cm−2 and no oxide precipitates was obtained. The 500 nm of buried oxide has very sharp interfaces, and contains crystalline-silicon inclusions near the interface with the substrate silicon.
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    Journal of Applied Physics 60 (1986), S. 2133-2136 
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    Notes: In this paper, experimental results of bias- and light-dependent spectral response measurements of CuInSe2/Cd(Zn)S thin-film solar cell and its consequences are discussed. The dc measurements are analyzed in light of new data and their consistency with chopped light measurements are reiterated. Experimental evidence also suggests that, at least in some cells, at high forward bias, reversal of photocurrent occurs. Present models for the bias- and light-dependent collection factor are also reviewed.
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    Journal of Applied Physics 60 (1986), S. 2149-2153 
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    Notes: Successful operation of a p-n-p AlGaAs heterojunction bipolar transistor at temperatures up to 800 K (527 °C) has been achieved. The device was fabricated from molecular-beam epitaxy grown material and features an Al0.45Ga0.55As emitter and Al0.25Ga0.75As base and collector regions. At room temperature a common emitter current gain of 12 is obtained, which reduces to ∼3 at 800 K. Weak emission of light is seen from the base region with λ=7170 A(ring) at 300 K, in agreement with the expected band gap for Al0.25Ga0.75As of 1.74 eV.
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    Journal of Applied Physics 60 (1986), S. 2154-2161 
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    Notes: A threshold voltage sensitivity analysis of high electron mobility transistors (HEMTs) based on a self-consistent model for the electron distribution is presented. The calculated sensitivity values are related to experimentally obtained uniformity data on 2-in. wafers grown by molecular-beam epitaxy (MBE). The effect of doping concentration, compensation, and thickness of the doped and undoped (Al,Ga)As layers and the mole fraction are considered. Enhancement mode transistors are generally found to be less sensitive than transistors of depletion type. The analysis brings out that the most important design parameters to control are the thickness of the doped (Al,Ga)As layer and its doping concentration (compensation). Changes in the Al mole fraction are found to have a negligible influence. The effects of varying growth conditions are estimated and possible ways of improving the threshold uniformity are discussed.
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    Journal of Applied Physics 60 (1986), S. 2177-2179 
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    Notes: Contrary to recent predictions, it has been observed that the addition of small quantities of hydrogen, ethanol, and benzene to nitrogen reduce the output power of a nitrogen laser. N,N-dimethylaniline enhances the output power of the laser by 25%. A Penning ionization process is proposed as a mechanism for quenching the B 3Πg state of nitrogen.
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    Journal of Applied Physics 60 (1986), S. 2182-2184 
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    Notes: Experimental values are reported for parameters employed in the theory of film deposition from organic vapors by irradiation with charged particles. Direct evidence is given for the known assumption that for ion-beam-induced deposition the activation cross section is much larger than for electron-beam-induced deposition. It is shown that this cross section is a complex quantity presumably including energy transfer within the macromolecules and excitation by secondary particles. The other parameters were found to be consistent with their simple interpretations in the theory as the lifetime of an activated state and area per polymerization center.
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    Journal of Applied Physics 60 (1986), S. 2184-2186 
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    Notes: A thermal conversion mechanism of semi-insulating GaAs with a SiOxNy cap was studied. Both SiO- and SiN-rich cap films exhibit n-type conductivity after thermal annealing, and a newly discovered level Ec−0.91 eV is present in these converted samples found by deep-level transient spectroscopy measurements. This conversion phenomenon may be attributed to Ga out-diffusion through the cap layer during thermal annealing.
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    Journal of Applied Physics 60 (1986), S. 2189-2191 
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    Notes: It is shown that a formula recently given for the ratio of emission to capture coefficient of a trap, en/cn=Nc exp(−ΔG/kT), holds with only minor modifications also for traps which can capture several electrons. Auger effects and impact ionization can also readily be included.
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    Journal of Applied Physics 60 (1986), S. 1560-1564 
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    Notes: A revised fringe equation is proposed for the hook method in anomalous dispersion for the case of thick plate compensation. The derivation is based on the equality of transit times through the interferometer arms, which results in a revised expression for the optical path difference of the plate. As a result, an apparent fringe order inconsistency in the traditional derivation is resolved, and the interpretation of the hook constant is clarified.
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    Journal of Applied Physics 60 (1986), S. 1569-1576 
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    Notes: A trapped distribution of low-energy electrons was used to alleviate spherical aberration in a solenoidal magnetic lens. The space-charge-correction method has potential application to the focusing of heavy, negatively charged particles such as H− ions. In the geometry investigated, the field contributions from trapped electrons cancel net electric fields along magnetic flux surfaces. The lens magnetic fields therefore define equipotential surfaces. Experimental results were obtained using a 10-keV electron beam as a nondestructive probe in a solenoid lens with 65-G peak field. Annular distributions of trapped electrons were achieved that were stable against the diochotron instability. Deflections of the probe beam were consistent with theoretical predictions. The peak focused current density of the 10-keV beam was improved twentyfold with the addition of trapped electrons in the lens.
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    Journal of Applied Physics 60 (1986), S. 1584-1590 
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    Notes: A calculation is presented of spontaneous radiation emitted by an electron beam passing through a continuously rotating quadrupole magnetic undulator. It is shown that radiation spectrum emitted in forward direction of beam propagation has four peaks, corresponding to four betatron frequencies. Utilizing the Madey theorem, a stimulated emission is calculated and presented as gain versus frequency curves, for different values of the quadrupole magnetic field. A free-electron laser operating at two or three radiation frequencies with a quadrupole magnetic wiggler is suggested.
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    Journal of Applied Physics 60 (1986), S. 1269-1273 
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    Notes: Simple analytic models have been developed to describe the current density and magnetic field profiles in a cylindrically symmetric plasma carrying a z-directional current. Solutions are obtained for time varying boundary magnetic fields characteristic of imploding liner and gas puff plasma implosions. The cylindrical models are compared with previously developed planar solutions. Applications to electromagnetically imploded plasma shells show a small variation in the magnetic field profiles at early times and large radius. These variations become more pronounced as the implosion moves to smaller radius. In general, the effects of cylindrical geometry become significant only when the outer radius reaches the same order as the magnetic field gradient scale length.
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    Journal of Applied Physics 60 (1986), S. 1295-1299 
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    Notes: A negative potential well is found in front of a positively biased electron collecting plate in a low temperature laboratory plasma. The well parameters are governed by the Child–Langmuir condition and a necessary condition for the existence of such potential wells is the presence of an ion pumping mechanism which removes trapped ions from the wells. Here ion pumping was provided by the presence of negative electrically floating ceramic on the back of the plate.
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    Journal of Applied Physics 60 (1986), S. 1310-1312 
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    Notes: The edge shift at the threshold in the L2,3 soft x-ray emissions spectra of Al and Mg in the γ-phase Al–Mg alloy was measured with a 2-m grazing incidence spectrometer of high resolution under ultrahigh vacuum (UHV). The work function of metallic Al, Mg, and Al–Mg alloy were measured by ultraviolet photoemission spectroscopy in UHV (5×10−10 Torr). The measured work function has shown that charge transfer from Mg to Al takes place on alloying and that the edge shift of the L2,3 soft x-ray emission spectrum in Al–Mg alloy is caused by such a charge transfer.
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    Journal of Applied Physics 60 (1986), S. 1306-1309 
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    Notes: A real-time pulsed nuclear magnetic resonance measurement system controlled by a microcomputer has been constructed. The real-time measurements of the spin-spin relaxation time T2, the spin-lattice relaxation time in the rotating frame T1ρ, and the spin-lattice relaxation time T1 become possible by the use of this system. It is applicable to the studies of nonequilibrium phenomena in polymers such as crystallization, phase separation, gelation, polymerization, etc. It is also applicable to wider fields such as biological reaction and chemical reaction. The application of this system to polymer crystallization is presented as an example.
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    Journal of Applied Physics 60 (1986), S. 1322-1324 
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    Notes: Profiles of Bi, Xe, Sn, Kr, Ga, Fe, K, Ar, P, Na, and F implanted into the AZ111 photoresist are compared with recent theoretical predictions. With the exception of the noble gases and F, the experimental results are well fitted by the Biersack–Haggmark [Nucl. Instrum. Methods 174, 257 (1980)] Monte Carlo calculations. For the noble gases we obtain ranges up to a factor of 2 shorter than the above predictions. Fluor changes the profile as function of energy, being nearly Gaussian at 30 keV and distributing according to the calculated ionization at 70 keV.
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    Journal of Applied Physics 60 (1986), S. 1336-1341 
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    Notes: Different amounts of 100-keV iron ions have been implanted into high-resistivity p-type FZ-silicon samples. The implantation damage, recovery of damage during various annealing periods and temperatures, movement of iron atoms under annealing and oxidation, and the kinds of defects created after implantation, annealing, or oxidation are all investigated by channeling and backscattering measurements. We have found that the critical fluence of 100-keV iron implanted into silicon at room temperature is ∼2.5×1014 Fe/cm2, and that iron atoms are gettered by silicon oxidation. In this supersaturated region iron atoms diffuse slightly towards bulk silicon during high-temperature annealing (≥1100 °C) but not at all during low-temperature annealing (≤1000 °C) in dry nitrogen ambient.
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    Journal of Applied Physics 60 (1986), S. 1364-1368 
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    Notes: Computer simulations of the intrinsic (400) reflecting power of In1−xGaxAs layers having graded compositions are presented. We find that multiple x-ray peaks can result from a linearly graded region which implies that an interpretation which ascribes individual peaks to sublayers having a constant lattice parameter may not always be correct. We find that, in general, the simulations are asymmetric and that they have a full width at half maximum less than ∼100 arcsec. We have simulated an actual rocking curve of a single In1−xGaxAs1−yPy layer grown on a (100) InP substrate by vapor-phase epitaxy which exhibited multiple peaks, and we find that a good fit is possible if the layer had a graded lattice parameter. Comparing dynamical to kinematical simulations for a 3-μm-thick linearly graded layer, we find that most of the features resulting from the grading can be explained using kinematical theory. However, only the dynamical simulations can properly account for the reflecting power in the vicinity of the substrate peak and for the lack of fine structure which is observed in the absence of a discontinuity in Bragg spacing at the layer/substrate interface.
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    Journal of Applied Physics 60 (1986), S. 1352-1358 
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    Notes: The time-resolved reflectivity technique is shown to be able to characterize interface structure during solid-phase epitaxy in GaAs. A detailed study of interface structure during regrowth and recrystallization kinetics is made for different implanted impurities and implantation parameters in GaAs. It is shown that the interface roughens on a macroscopic scale during the regrowth process and that this evolution has an intrinsic character in the implanted material. Activation energy is shown to be independent of implantation conditions. Substitutional impurity implantation does not produce variations in regrowth kinetics whereas argon implantation drastically decreases the growth rate. Results are interpreted in terms of interface roughening due to nonrelaxing atomic configurations in the disordered phase. The evolution of the interface has been related to an increase of disorder in the regrown layers.
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    Journal of Applied Physics 60 (1986), S. 3845-3849 
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    Notes: The irradiation of a KrF laser (248 nm) into the interelectrode space affects the electric flashover characteristics there. The results obtained show that negative oxygen ions dominate formation of the interelectrode arc in air. A laser beam is introduced parallel to the interelectrode axis and the equipment is arranged to prevent the occurrence of photoelectric effects on the electrode surfaces. The time separation between laser firing and application of the interelectrode voltage is varied from 10 ns to 10 ms. The interelectrode spacing is set in the range 2–12 cm. The arc formation time and the flashover probability are measured. The initial ion number density is estimated experimentally to be on the order of 1011 cm−3 throughout the channel.
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    Journal of Applied Physics 60 (1986), S. 3836-3839 
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    Notes: An extensive range of solid solubility was found in the LiNb3O8-TiO2 system. The solid-solution phase has the undistorted rutile structure for 0.40≤x≤1.0 in (Li0.25Nb0.75O2)1−x (TiO2)x. A member of this series, with x≈0.58, is proposed to be the intermediate phase formed during Ti indiffusion in LiNbO3 during optical waveguide formation, rather than Ti0.65Nb0.35O2 as was previously postulated. This assignment agrees with the experimental results of previous studies of Ti indiffusion into LiNbO3 single crystals, and is consistent with a Ti diffusion mechanism based on defect chemistry studies. The preparation and structural characterization of the LiNb3O8-TiO2 solid-solution phase is discussed.
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  • 92
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3886-3894 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Si and Ge layers have been grown on CaF2/Si(111) by molecular-beam epitaxy. Both Ge and Si grow as islands, and both the island size and the spacing between nucleation sites are considerably larger for Ge (∼300 nm) than for Si (∼100 nm). In addition, Ge and Si layers are found to be a mixture of type-A (aligned with the underlying CaF2) and type-B (rotated 180° about the surface normal with respect to the underlying CaF2) regions. The crystalline quality and surface morphology of the Ge layers are much better than those of the Si layers. This is thought to be due to the larger island size of the Ge deposits and to a greater ease of movement of the boundaries between type-A and type-B regions in Ge. Hall measurements show electron mobilities of up to 664 cm2/V s in Si layers and hole mobilities of 234 cm2/V s for Ge layers. Finally, the use of a GexSi1−x-Si superlattice, when grown on a GexSi1−x buffer layer which is lattice matched to the CaF2 at the growth temperature, is shown to improve Si heteroepitaxy.
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  • 93
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3910-3915 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Grain boundaries (GB's) can induce electrostatic potential barriers due to trapping of majority carriers into defect states at the interface. The as-grown electrical activity of GB's in silicon is related with the density of decorated dislocations in the interface plane. Heat treatments actuate as-grown electrically active and inactive boundaries. The measured transverse conductance is reduced due to the presence of a potential barrier. The density of these generated states is determined by duration and temperature of the treatment. We explain this actuation by impurity-related formation of trap states at the interface. The annealing-temperature dependence of the density of trap states is independent of the atomistic structure of the interface. We observe strong impurity gettering of GB's. Hydrogen incorporation in plasma discharge can repassivate as-grown electrically active and the heat-actuated GB's. The majority-carrier transport properties of silicon GB's are thus determined by impurities instead of the atomistic interface structure.
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  • 94
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3895-3899 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: For visible-light-emitting laser diodes, InGaAsP double heterostructures have been grown on GaAs substrates using liquid-phase epitaxy. As the growth temperature is as high as about 780 °C, a large amount of phosphorus evaporates from the solutions for the cladding layers during the growth process. The phosphorus vapor disturbs the solution composition for the active layer, so that very thin and uniform active layers cannot be obtained. By using In-P-Sn solution and supplying the phosphorus partial pressure around the graphite boat, the influence of phosphorus vapor ambient for InGaAsP (λPL=805 nm) growth is confirmed. When the phosphorus partial pressure increases, the surface of epitaxial layer becomes rough and the substrate is partly etched back. From x-ray diffraction and photoluminescence spectral measurements, the composition of the grown layer is also found to be changed. As a result of increasing the flow rate of H2 gas in order to protect the solution for the active layer from phosphorus contamination, the double heterostructure wafers with the high-quality active layer can be obtained reproducibly. Thus, pulsed lasing operation at room temperature has been achieved. The lasing wavelength is 816 nm and the threshold current density is ∼4.6 kA/cm2.
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  • 95
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3954-3958 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect on negative resistance of a small aluminum concentration in the outer GaAs layers of a GaAs-Ga1−xAlxAs double-barrier tunneling structure is calculated. The aluminum concentration can be chosen so that the alloy conduction-band minimum is slightly below the energy of the resonant tunneling level of the GaAs central well region. Less voltage is then needed to raise the incoming electrons into the resonant energy level. The decreased voltage across the structure has several beneficial effects. The electron transmission coefficient through the barriers on resonance increases, the total applied voltage across the device is reduced, and the current through parasitic parallel resistances is reduced. Significant improvements in peak-to-valley ratios are predicted, the improvement being dependent on the parameters of the structure.
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  • 96
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 3967-3977 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analysis of the frequency dependence of superconductor-insulator-normal (SIN) and superconductor-insulator-superconductor (SIS) quasiparticle mixers is presented. Power-law expressions for conversion loss and mixer shot-noise temperature for the double-sideband SIN mixer are derived from the Tucker theory for the case of a source conductance which is small compared to the conductance of the junction. For an ideal SIN tunnel junction at T=0 the mixer conversion efficiency is shown to decrease approximately linearly with frequency up to f=Δ/h. From f=Δ/h to 2Δ/h the conversion efficiency remains approximately constant, while above f=2Δ/h it rolls off as the inverse square of the frequency. Expressions for the shot-noise contribution to the mixer noise temperature are also derived. At frequencies up to f=Δ/h the noise temperature rises as the square root of the frequency. From f=Δ/h to f=2Δ/h the noise temperature of the mixer increases linearly with frequency, whereas above f=2Δ/h it rises as the cube of the frequency. Conversion efficiency and noise temperature are also calculated numerically for the SIN mixer. Good agreement is found between the frequency dependencies calculated analytically in the limit of small local oscillator power and the numerical calculations for optimal pumping. The frequency dependence of the nonideal SIS junction is also analyzed, and shown to yield similar results, with the characteristic frequencies Δ/h and 2Δ/h for a SIN mixer transformed into 2Δ/h and 4Δ/h, respectively. Expressions also are derived for the saturation power as a function of frequency.
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  • 97
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 4007-4011 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report for the first time an attempt to melt and recrystallize macroscopic (10–20 μm deep) silicon mechanical damage that originates from wafer modifications such as slicing and lapping. Recrystallized surfaces appear mirror shiny, with significantly improved surface smoothness, as compared to the grossly coarse texture of the original damaged surfaces. The crystallinity also appears good. Across the recrystallized layer was observed some indication of impurity migration caused by segregation in the melt. Recrystallized layers contained far fewer defects than the bulk underneath, sometimes evolving to denuded-zone-like layers. This aspect can be particularly useful in the practical use of this technique for wafer modifications.
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  • 98
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 4015-4021 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: To calculate the head field distribution first we pursue the Poisson integral approach3 using Fourier series method retaining up to 200 terms in the series. The parameters related to the rational approximation to the field equation for both ring heads and pole-keeper heads have been obtained and tabulated. The idea of the Poisson integral is then extended, denoted as Poisson integral II, to enable us to calculate the head fields both within and without the head gap regions. The first Poisson integral II involves eight parameters and enables us to calculate head fields in reasonably good agreement with the direct Fourier series calculations. The second Poisson integral II involves a self-consistent calculation, which is reducible to the rational field equations with five parameters and is highly capable of producing head field distribution anywhere with great accuracy at low spacings. Results of a comparison with a finite element method calculation are excellent.
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  • 99
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 4030-4032 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It has been found that CuInSe2 polycrystalline material suitable for photoelectrochemical cells can be produced from low grade In, Se, and Cu. Low-energy electron diffraction (LEED) measurements on these samples show that well ordered (112) surfaces can be produced after 35 min Ar ion bombardment at ∼8 μA cm−2, 600 eV, followed by 30 min anneal at temperatures as low as 320 °C. Extra LEED spots are visible at some energies, indicating a clean surface but with possible nonstoichiometric areas. No effects of oxygen are observed at exposures up to 326×103 L.
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  • 100
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 1434-1439 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A model is presented for the potential barrier height at grain boundaries in polycrystalline semiconductors, which takes into account a curved grain boundary under equilibrium and nonequilibrium conditions, assuming flat quasi-Fermi levels. An analytical method to calculate the reduction of the potential barrier due to the grain curvature, without using the depletion approximation, is developed and applied to compute the barrier lowering as a function of the bulk doping concentration, interface state density, and the grain radius in silicon. The barrier height can vary along a grain boundary, due to different local curvatures, being lowest at corners of grains.
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