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  • 1
    Publication Date: 2020-02-12
    Keywords: 550 - Earth sciences
    Type: info:eu-repo/semantics/article
    Format: application/pdf
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 3679-3683 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effects of photoinduced hole doping on the electrical characteristics of grain boundary weak link junctions based on high Tc YBa2Cu3Oy thin films are investigated. Visible light illumination induces a substantial enhancement in the critical current Ic of approximately 20%–40% even at temperatures well below Tc. The Ic enhancement is accompanied by a clear decrease in the junction resistance RN which can be explained by the photoinduced hole doping of the degraded regions with oxygen deficiency and/or disorder near the grain boundary. It is also demonstrated that photoinduced hole doping provides a way of improving the IcRN product and also a way of controlling the Ic value in situ in these weak link junctions.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 5507-5509 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic measurements at various temperatures have been performed for loose powder and field-oriented samples of Gd1−xDyxCo4B with x=0, 0.05, and 0.1. The temperature dependences of spontaneous magnetization in these compounds are determined. It is found that a spin reorientation occurs at around T=162 K for Gd0.95Dy0.05Co4B and at around 225 K for Gd0.9Dy0.1Co4B. The temperature dependences of magnetic anisotropy constants, K1(Gd1−xDyxCo4B), of Gd1−xDyxCo4B with x=0 and 0.1 are determined. The anomalous temperature dependence of K1 (GdCo4B) is well explained by taking account of the Gd sublattice magnetic anisotropy due to the dipole–dipole interaction and the Co sublattice magnetic anisotropy similar to that in YCo4B. The temperature dependence of the Dy sublattice magnetic anisotropy constant, K1(Dy), has also been determined by making use of K1(GdCo4B) and K1(Gd0.9Dy0.1Co4B). © 1996 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6283-6285 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: X-ray diffraction and magnetization measurements have been performed for powdered and field-oriented samples of Gd1−xDyxCo4B with x=0, 0.05, 0.1, and 0.2. It has been found that Gd1−xDyxCo4B with x=0.2 has a planar magnetic anisotropy in the temperature region below room temperature; however, the samples with x=0.05 and x=0.1 have an axial magnetic anisotropy at room temperature and transform to a tilted state in the low-temperature region. By analyzing magnetization curves measured in a pulsed field up to 140 kOe at T=4 K and also in a static field up to 12 kOe at 78 K for the field-oriented samples with x=0.05 and x=0.1, approximate values of magnetic anisotropy constants of a Dy ion in Gd1−xDyxCo4B, K1(Dy) and K2(Dy), have been determined to be −2.1×10−14 erg/Dy and 1.3×10−14 erg/Dy, respectively. By comparing these values with those of DyCo5.2, it is found that K2(Dy) in the CeCo4B-type structure is enhanced in one order by the crystallographic change from the CaCu5- to the CeCo4B-type structure.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 1733-1739 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The optical parameters of NbN thin films reactively sputtered mainly at room temperature are investigated by in situ ellipsometry using a He-Ne laser source. Systematic correlations between the ellipsometric parameters and the film properties are observed. In particular, the Tc film shows an approximately linear relation with the parameter ψ over the wide range of 7–17 K. Optical reflectivity measurements are carried out in the wavelength range of 0.2–2.5 μm for these films. Each spectrum is well fitted by the curve calculated using the Drude model with a screened plasma frequency of 25 000–30 000 cm−1. The Tc film also shows a stronger correlation with the damping constant of plasma excitation than with the reflectivity. This is considered to be a universal degradation curve for this system, similar to those observed in high -Tc A15 compounds. The relation of Tc to ψ is found to be equivalent to this correlation.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 670-680 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Josephson tunnel junctions with Pb counterelectrodes have been fabricated using a CF4 plasma cleaning process on A15 Nb3X(X=Al,Ge) thin films prepared by magnetron sputtering. The effects of deposition conditions on junction quality as well as superconducting parameters (gap, dc Josephson current, and magnetic penetration depth) of the films have been investigated. The junction quality is largely influenced by film deposition conditions, especially by substrate temperature. Junctions with base electrodes which are deposited on oxidized silicon (for Nb3Al) or sapphire (for Nb3Ge) radiatively heated above approximately 700 °C show high-quality I–V curves, while lower temperatures lead to increases in the excess conductance and the width of the sum-gap structure. High-quality junctions with large sum gaps (up to 4.05 mV at 4.2 K for Nb3Al/Pb and 5.05 mV for Nb3Ge/Pb) can be prepared on such films. Furthermore, systematic relationships between the superconducting parameters and the energy gaps are observed, which indicate a good homogeneity of the films. In contrast, all junctions on higher-Tc films prepared by means of self-epitaxial deposition or using a molybdenum substrate holder exhibit apparent current rise at lower voltages, indicating the coexistence of low-Tc materials. Systematic correlation between the junction quality and the residual resistivity ratio shows that such an inhomogeneity extends to the bulk of the films. Radiatively heated samples with the A15 phase composition near the boundary of the film homogeneity range exhibit favorable properties for electric applications such as large energy gaps and small magnetic penetration depths (∼150 nm). However, junctions using these films persistently exhibit nonidealities, such as a slight amount of excess conductance with onset at the Pb gap and a broadened current rise at the sum-gap in their optimized I–V curves, similar to those reported in the coevaporated films.
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 71 (1997), S. 844-846 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ferromagnetic compound La3−3xCa1+3xMn3O10 with a triple perovskite structure can be successfully synthesized by using a thin-film growth method. Sputtered a-axis thin films with x=0.3 have been examined with respect to their magnetotransport properties. For the triple perovskite compound, we have observed the features, including the enhanced magnetoresistene (MR) effect and the characteristic low-temperature MR effect resulting from intragrain spin-polarized tunneling, which were reported for the double perovskite manganites. A comparison of the magnitude of these features in triple and double perovskite manganites suggests that the features are actually determined by the c-axis Mn–O bond configuration in a layered-perovskite ferromagnet. © 1997 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 70 (1997), S. 2303-2305 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Epitaxial thin-film and polycrystalline bulk samples of ferromagnetic La2−2xCa1+2xMn2O7 (x=0.3) with a layered perovskite structure have been examined with respect to their magnetotransport properties. In addition to a large magnetoresistance (MR) effect at temperatures around the metal–insulator transition, a-axis thin films exhibit unusual low-temperature MR behavior with apparent hysteresis in applied magnetic fields. The features in the bulk samples are a low-temperature MR effect without such hysteresis, and also an MR effect at high temperatures well above the metal–insulator transition temperature. The unique MR behavior depending on the sample form would reflect an anisotropic nature in the layered-perovskite ferromagnet with two-dimensional Mn-O networks. © 1997 American Institute of Physics.
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  • 9
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Epitaxial thin films of ordered double-perovskite Sr2FeMoO6−y are deposited on (001) SrTiO3 substrates by pulsed-laser deposition using a two step growth process. Selection of growth conditions is found to lead to either highly conductive metallic thin films (residual resistivity of about 1 μΩ cm) or semiconducting films. The metallic films show a positive magnetoresistance (MR) as high as 35%, while the semiconducting films show a negative MR of −3%, at a temperature of 5 K and a field of 8 T. © 1999 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 68 (1996), S. 3638-3640 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Bulk samples of La2−2xCa1+2xMn2O7 with the layered Sr3Ti2O7-type perovskite structure have been successfully synthesized and investigated with respect to their magnetic and electrical properties. It is found that La2−2xCa1+2xMn2O7 (x=0.25) is a metallic ferromagnet with a magnetic transition temperature Tc of 215 K. The large magnetoresistance (MR) effect with Δρ/ρ0 of ∼60% at 1.8 T was observed in a wide temperature range below a cusp temperature in resistivity of 96 K, which is well below the magnetic Tc. This behavior is quite different from that of the well-known double-exchange ferromagnets such as La1−xCaxMnO3, where large MR effects are restricted to a narrow temperature range around the ferromagnetic transition. The present result could be interpreted by using the double-exchange theory incorporating the anisotropy resulting from the two-dimensional Mn-O-Mn networks in La2−2xCa1+2xMn2O7. © 1996 American Institute of Physics.
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