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  • American Institute of Physics (AIP)  (12)
  • Blackwell Publishing Ltd  (1)
  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 3073-3080 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effects of the deposition parameters on configurations and stability of hydrogen (deuterium) in amorphous sputtered silicon a-Si:H have been analyzed using Fourier transformed infrared absorption spectroscopy, deuterium effusion experiments, and x-ray diffractometry. The ratio of monohydride bonds Si–H was calculated from the infrared absorption stretching mode spectrum. This ratio was increased when the substrate temperature was increased. The effusion results in a-Si:D, when deposited with a simple cathode, have shown the presence of clustered deuterium weak bonds in microvoids (400 °C deuterium effusion peak), beside isolated Si–D bonds embedded in the more compact tissue (650 °C deuterium effusion peak). The deconvolutions of the stretching mode infrared absorption spectrum of the as-grown sample and after isothermal annealing at 510 °C have allowed one to conclude that it is not possible to identify the low temperature and high temperature effusion peaks, respectively, with the decomposition of Si–H2 and Si–H centers. The effusion of the less stable hydrogen improved the amorphous structural relaxation. The ratio of monohydride bonds was increased by introducing a magnetron cathode in the deposition chamber. At the same time, the deuterium effusion spectrum was modified, showing a continuous deuterium effusion from 350 °C, instead of two well-defined effusion peaks. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 54 (1989), S. 1787-1789 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In+ -implanted CdTe and Cd0.23 Hg0.77 Te have been studied by resonant Raman scattering. Dipole-forbidden but defect-induced scattering by one longitudinal optical (LO) phonon as well as Fröhlich-induced two-LO phonon scattering is strongly affected by implantation of 350 keV In+ with doses ranging from 1011 to 5×1014 ions/cm2 . The intensity ratio of the one-LO and the two-LO phonon lines is found to be a measure of the implantation damage in CdTe and in the alloy Cd0.23 Hg0.77 Te. The observed implantation effects on resonant Raman scattering by LO phonons are due to a broadening and an energy shift of the corresponding resonances as demonstrated for the E0 +Δ0 gap resonance in CdTe.
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Films of Cu–In–Se alloys can be electrodeposited in a wide range of controlled composition. Annealing treatments under Se pressure transform these precursor films in large grain CuInSe2 films with improved electronic properties. These modifications are shown to depend on the Se pressure imposed during the treatment allowing a certain tailoring of the electronic properties of the films. The properties of electrodeposited/selenized films are presented as obtained from luminescence measurements, Hall effect, and photoelectrochemical characterization. An efficiency of 6.5% (total area, without antireflecting coating) is reported for the best CuInSe2/CdS/ZnO solar cell. An analysis of the device is also presented where limitations by interface recombination are shown to be the dominant loss mechanism. © 1996 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 73 (1998), S. 28-30 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Homoepitaxially grown nitrogen-doped ZnTe layers have been exposed to a hydrogen (deuterium) plasma. After hydrogen (deuterium) diffusion, an infrared absorption band appears at 3346 cm−1 (2489 cm−1). It is assigned to the vibrational stretching mode of the N–H (N–D) bond. It is also shown that the absence of such detectable bands in heteroepitaxially grown ZnTe/CdZnTe layers can be explained by thermal strains originating from the difference between the ZnTe and the CdZnTe thermal expansion coefficients. © 1998 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 1461-1466 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Atomic hydrogen has been introduced from a plasma source into InAs layers grown by molecular beam epitaxy on GaAs substrates. It is shown that hydrogen diffuses very fast into this material. The presence of hydrogen modifies the electronic transport properties, the near-band-edge luminescence spectra, and the far-infrared reflectivity spectra. The most striking effect is that, unlike other III-V compounds, the free-carrier density increases by one order of magnitude after hydrogenation. These phenomena are reversible and thermal annealing restores the original properties of the samples. Finally, models are proposed to explain the experimental results.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 1393-1397 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Nitrogen doped ZnSe layers grown by molecular beam epitaxy have been exposed to a hydrogen or deuterium plasma. Deuterium diffusion profiles have been measured by secondary ion mass spectroscopy. The main feature of these profiles is the presence of a plateau on which the H concentration closely matches the total N content of the layers. Electrical and photoluminescence studies of the layers, before and after hydrogen plasma exposure, show that both acceptor and donor N-related centers are passivated by hydrogen. These results demonstrate that in ZnSe:N hydrogen passivates the nitrogen acceptors and the related nitrogen donors. © 1999 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 88 (2000), S. 550-554 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Arsenic doped CdTe layers have been successfully exposed to a hydrogen or deuterium plasma to study the diffusion of these species and their interactions with arsenic. It is shown that hydrogen behaves similarly when unintentionally (during growth) or intentionally (plasma exposure) introduced. Infrared absorption measurements show that in both cases, identical As–H complexes are formed. The IR absorption line of deuterium–arsenic complexes has also been detected. The concentration of active arsenic acceptors decreases after intentional hydrogen or deuterium diffusion, as a consequence of the formation of these As–H or As–D complexes. But, the diffusion profiles of deuterium show that deuterium in the semiconductor binds also to other As-related centers which have not been identified unambiguously. © 2000 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 6454-6460 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have investigated the temperature dependence of the fundamental absorption edge of a series of Hg1−xCdxTe alloys (with composition x ranging from 0.5 to 1). Analyzing our data in the light of the three-dimensional theory of direct-allowed excitons, we find precise values for the fundamental Γ8-Γ6 interband transition energy in a temperature range extending from 0 to 300 K. All experimental results, including previous data for HgTe and mercury-rich Hg1−xCdxTe alloys, are well accounted for using a simple empirical formula: Eg (eV)=−0.303(1−x)+1.606x−0.132x(1−x)+[6.3(1−x) −3.25x −5.92x(1−x)]10−4T2/[11(1−x)+78.7x+T]. This expression, which is valid for all compositions 0≤x≤1 and temperatures 0≤T≤500 K, predicts an alloy composition such that the band-gap energy is temperature independent: We find x=0.505. Finally, it can be used for technological application purpose (far-infrared detection as well as optical-fiber communications performed at realistic values of the temperature) and gives accurate values for the temperature and composition dependence of the effective mass in the semiconducting range of alloys.
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  • 9
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Unintentionally doped ZnO layers grown epitaxially on a sapphire substrate have been exposed either to a hydrogen or deuterium plasma. Secondary ion mass spectroscopy measurements performed subsequently showed a rapid diffusion of hydrogen in these layers. Furthermore, the presence of hydrogen in the ZnO samples is found to be responsible for nearly a factor of 3 increase in the free electron concentration. This effect is attributed to the hydrogen passivation of compensating acceptor impurities present in the as-grown ZnO layers. © 2002 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 76 (2000), S. 1695-1697 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: ZnS layers were grown by metalorganic vapor phase epitaxy on GaAs substrates using diethylzinc, ditertiarybutyl sulphide, and triallylamine as organometallic sources. After postgrowth rapid thermal annealing, the ZnS layers showed p-type conductivity with hole concentrations up to 1018 cm−3. Photoluminescence measurements gave additional indications of the presence of electrically active nitrogen acceptors. In separate experiments, lithium was diffused from a LiH solid source into ZnS layers grown without the nitrogen precursor. High-conductivity p-type material was directly obtained with no need of thermal anneal. © 2000 American Institute of Physics.
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