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  • 1
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 80 (1996), S. 6349-6354 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: Shallow and deep centers were studied by means of temperature dependent Hall effect and photoluminescence (PL) measurements in two sets of undoped n-AlGaN samples grown by organometallic vapor phase epitaxy. The samples of these two series were grown under different conditions and had, as a result, electron concentrations differing by several orders of magnitude. The composition dependence of ionization energies of dominant donors in these two sets of samples is very different indicating that different types of centers are involved, but in both cases they are most probably related to some native defects. These defects behave as hydrogen-like donors for low Al compositions and become increasingly deeper with increasing Al content. The shallow-deep transition occurs at about x=0.2 in the low conductivity AlxGa1−xN series and at about x=0.5 for the high conductivity series. Several PL bands were detected in AlGaN and it is shown that the band at 3.05 eV is due to a radiative transition between deep donors in the upper part of the band gap and holes in the valence band or on shallow acceptors. For the yellow luminescence band at 2.25 eV it is demonstrated that this band consists of two overlapping bands and that the dominant band is due to a transition between the native donors and a carbon-related deep center. © 1996 American Institute of Physics.
    Materialart: Digitale Medien
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  • 2
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 5103-5106 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: Diffusion of boron, lithium, nitrogen, oxygen, and hydrogen into type IIa natural diamond was studied. The diffusion was performed in two steps. First, diffusion of Li and oxygen was performed in nitrogen atmosphere at 860 °C for one hour. The sample was then placed in a hot filament chemical vapor deposition (CVD) growth reactor and diffusion was performed for two hours in hydrogen atmosphere from a boron solid source placed on the surface of the sample. The condition of diffusion were those used routinely during CVD growth. After diffusion, the concentration of Li was of the order of 2×1016 cm−3 at the depth of 0.5 micrometer, and oxygen, nitrogen, and boron were found to be in the range (1–4)×1020 cm−3 at the same depth. The diffusion of hydrogen under conditions specific to CVD growth has also been studied for the first time and was found to be quite strong. © 1995 American Institute of Physics.
    Materialart: Digitale Medien
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  • 3
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 5625-5629 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: A method is proposed for the determination of the state of an impurity (donor, acceptor, or deep level) in semiconductor lattice. To demonstrate the method boron was diffused into type Ia natural diamond under a dc electric field. The concentration and diffusion profiles of boron were affected by the applied field. Boron diffuses as a negative ion since it is an acceptor shallow enough to be partially ionized at the temperature of diffusion. The drift velocity of boron ions at the temperature of diffusion was also estimated. The diffusion of lithium and oxygen from a Li2CO3 source in chemical vapor deposited diamond films was performed under bias at 1000 °C in an argon atmosphere. After diffusion, the concentrations of Li, O, and H in the diamond films were found to be around (3–4)×1019 cm−3. No dependence of these concentrations on the applied bias was observed. It was found that the diffusion of Li goes primarily through grain boundaries, which may explain why it does not depend on the applied voltage. Fluorine was present as an impurity in the dopant source. Its concentration in the films was around (1–2)×1017 cm−3 and did depend on the applied bias, indicating that fluorine may have formed a shallow level in the diamond band gap. © 1995 American Institute of Physics.
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  • 4
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: The effects of hydrogen treatment on electrical properties, luminescence spectra, and deep traps in InGaAlP and InGaP have been studied. It is shown that acceptors and donors (both shallow and deep) can be effectively passivated by hydrogen. The hydrogen is found not only to passivate the main electron and hole traps in our samples, but also to generate electron traps in n-InGaAlP and hole traps in p-InGaP. The influence of hydrogen treatment mode (direct plasma or a crossed-beams source in which the low-energy ion bombardment of the surface is effectively eliminated) on hydrogen concentration and hydrogen profiles in InGaAlP are discussed. © 1994 American Institute of Physics.
    Materialart: Digitale Medien
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  • 5
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 1968-1971 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: The redistribution of implanted atoms within GaAs/AlAs multilayer structures due to post-implantation furnace annealing is reported. The structures were grown using molecular-beam epitaxy on GaAs substrates and implanted with either hydrogen or beryllium ions. After furnace annealing at temperatures up to 700 °C, these samples were examined using secondary ion mass spectrometry. The measurements show that the hydrogen and the beryllium atoms redistribute with post-implantation annealing and that both species accumulate at the buffer layer-substrate interface. The concentration of atoms at this interface can exceed 1×1019 cm−3 and may be related to the crystal imperfections created during the inital stages of epitaxy. The significant redistribution of implanted ions may also alter the optoelectronics properties of multilayer semiconductor structures processed in this manner.
    Materialart: Digitale Medien
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  • 6
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 5121-5125 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: We implanted ions of 45 elements into HgCdTe, and into CdTe in some cases, at a variety of energies and fluences, and successfully measured the resulting depth distributions for 43 of them using oxygen and cesium primary ion beams and positive and negative secondary ion mass spectrometry (SIMS), respectively. Relative sensitivity factors for SIMS were determined for these elements in HgCdTe and CdTe using the known implantation fluences. The SIMS relative sensitivity factor is proportional to the inverse of the relative ion yield. We have plotted the results from oxygen SIMS and positive ions versus ionization potential (I), and from cesium SIMS and negative ions versus electron affinity (A) of the implanted elements. These data can be used to test models and theories about the dependence of positive and negative ion yield on I and A. Many of the data from oxygen SIMS for elements with ionization potential between 5 and 10 eV are consistent with the model of positive ion yield dependence on exp(−I), but some elements differ reproducibly and consistently from that model. Elements with ionization potential less than 5 eV and greater than 10 eV follow different dependencies. The data from Cs SIMS tend to fit the model of negative ion yield proportional to exp(+A), but no consistent single curve can be drawn through the data. The data for CdTe agree with those for HgCdTe within experimental error.
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  • 7
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 933-939 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: We report the results of a study of atom and acceptor depth profiles of unannealed and annealed Al implants into Si. We describe three regimes of Al redistribution during annealing, the characteristics of which depend on the density of the Al and associated defects. We also report as-implanted and annealed Al depth distributions, range parameters, and profile-shape factors for Al implanted into crystalline Si for energies from 20 to 600 keV and fluences from 3×1012 to 3×1016 cm−2.
    Materialart: Digitale Medien
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  • 8
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2797-2805 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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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  • 9
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 60 (1986), S. 2810-2813 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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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  • 10
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 59 (1986), S. 2597-2597 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Materialart: Digitale Medien
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