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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetostatic effect of a ferromagnetic particle array on an underlying two-dimensional superconducting Nb thin film was investigated in terms of flux penetration processes by means of high sensitive magnetometry. For bare Nb film, a large drop in magnetization due to a flux rearrangement appeared in the low field region below 2.5 mT. However, once magnetic particles were fabricated on the surface of the Nb film, the drop was not observed. In this configuration, the ferromagnetic particles seem to behave as flux guides for the external magnetic field, whereby the flux distribution inside the superconductor is well regulated. Furthermore, a periodical oscillation was observed in the hysteresis loops. This behavior is associated with a flux quantization in the regions where the superconductivity is suppressed by the stray field of the ferromagnetic particles. The local flux density distribution around the ferromagnetic particles was evaluated by using the London equation, and the magnetization curve of the Nb film with periodically modulated superconducting order parameter was calculated. © 1996 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 2634-2636 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Fine powders of SnO and Fe2O3 were thermally diffused into Y-Ba-Cu-O systems composed of YBa2Cu3O7−δ matrix with oriented c axes and Y2BaCuO5 precipitates. The magnetic hysteresis loops of the system were measured at 77 K as a function of an applied magnetic field direction defined as the angle between the field and the c axis. The amplitude of the magnetization hysteresis ΔM, which is proportional to the critical current density Jc, was increased by nonmagnetic impurities SnO. On the other hand, ΔM was decreased drastically by magnetic impurities Fe2O3 although the critical temperature Tc was hardly decreased. In all the samples, the angular variation of ΔM showed a maximum at θ=0° and a minimum around θ=90°. However a local maximum at θ=90°, which is due to the intrinsic pinning, was observed only in the sample with diffused SnO. The intrinsic pinning of the sample with diffused Fe2O3 was significantly suppressed and the two-dimensional pinning property apparently became more pronounced. © 1995 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5903-5903 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ni-Pd composite fine particle is an ideal system to study surface and interface magnetism because of its large surface area compared with the total volume. In this work, magnetic properties of Ni-Pd composite fine particles were studied in terms of the magnetic proximity effect and the effect of hydrogenation. The composite particle consists of Ni core and Pd shell. Five different particles with different Pd shell thicknesses, 50, 100, 150, 200, and 350 A(ring), were prepared. The average diameter of the Ni core is about 0.7 μm. The Curie temperatures of all the samples are lying around 630 K and are nearly equal to that of a bulk Ni. Unlike pure Ni, the samples exhibit a relatively large coercive force of a few hundred Oersted in the temperature range from 4.2 to 750 K. The magnetization of the Ni core is found to be somewhat lower than that of pure Ni. An enhanced interface anisotropy due to the Pd coating (∼−1.5×105 J/m3) seems to impede saturation. Before hydrogenation, there appears quite a large thermal hysteresis. On heating, the isofield magnetization exhibits ferromagnetic behavior with a rise of magnetic moment below 30 K, suggesting that there is induced magnetization in the Pd shell. The change in magnetization follows the Curie–Weiss law, which gives a Curie temperature of 22 K. However, the steep rise of magnetization is not observed in the cooling process. After hydrogenation, this ferromagnetic behavior completely vanishes. There is also observed no lattice expansion, but this isovolumetric constraint seems to have little change on the saturation hydrogen loading.
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  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic and structural properties of Ni fine particles coated with Pd were investigated in hydrogen atmospheres by means of in situ magnetometry and in situ x-ray diffractometry. The x-ray diffraction patterns in hydrogen atmospheres show that the width of the plateau in the Pd–H phase boundary (miscibility gap) narrows with decreasing Pd thickness, which is reminiscent of nano-crystalline Pd. At room temperature, the magnetization in hydrogen atmospheres shows a steep saturation and a small decrease in the residual magnetization, indicating that the interface magnetic anisotropy is reduced by the hydrogenation. © 1996 American Institute of Physics.
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  • 5
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetostatic effect of the micron-size ferromagnetic particle array on a two-dimensional superconductor was investigated. In the bare Nb film, a sharp drop in magnetization due to the flux rearrangement was observed, whereas this behavior was not observed for the Nb film with the ferromagnetic particles arranged on top. The difference in the magnetization curves may be attributed to the regulated flux penetration process by the ferromagnetic particle array. © 1996 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3479-3481 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic image effect in a superconducting magnet (SCM) distorts the distribution of the magnetic flux produced by the magnetized specimens, so that this effect must be taken in consideration for a precise measurement of magnetization. This effect depends on the intensity of magnetic fields, histories of the SCM magnet, and geometrical arrangements of the coil system. The magnetic flux distribution in a small SCM, into which a superconducting Pb tube shield is inserted, is measured for the purpose of comparison with the electromagnetic calculation. The image effect is also investigated experimentally using a high sensitive vibrating sample magnetometer and a 100 kOe SCM. The results calculated numerically are in good agreement with the experiments. In general, under the presence of the image effect, the susceptibility measured by a vibrating sample magnetometer tends to be overestimated, while magnetization tends to be rather underestimated. In a practical cryogenic system, however, the eddy current loss induced in the metallic wall around the specimens was found to play also an important role.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6735-6737 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Sm2Fe17N3−δ is a promising permanent magnet material but disproportionation above 650 °C means that only low-temperature processing can be considered. Sintering micron-size Sm2Fe17N3−δ powder with the soft, low-melting metals Zn, Bi, Sn, and Al has been investigated. Good results are obtained with zinc. A coercivity of 0.6 T and a maximum energy product of 84 kJ/m3 (10.5 MGOe) have been obtained. Zn7Fe3 is formed as a secondary phase.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4616-4618 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Amorphous melt-spun Pr2(Fe1−xCox)14B has been prepared to test the concept of magnetic-field-induced crystallite alignment. Crystallization temperatures (Tx) of alloys with x=0.5, 0.6, and 1.0 were determined to be 622, 646, and 507 °C, respectively. These temperatures are all lower than the Curie temperatures (Tc) of the crystallized 2:14:1 phase. The glasses were then heat treated at a temperature Tt(Tx〈Tt〈Tc), either in no field or in a magnetic field of 0.3 T applied parallel to the long edge of the ribbon. The degree of alignment was investigated by means of x-ray diffraction and magnetization measurements. A texture was found where the c axes tend to lie in the ribbon plane in zero field, which is slightly modified when a magnetic field is applied during the heat treatment.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4619-4621 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Both Nd15Fe77B8 and Sm(CoCu)5 sintered magnets have been reported to exhibit staircase hysteresis loops with giant Barkhausen jumps below about 10 K. The pattern is reproducible at a fixed temperature. Here the observation of heat pulses associated with the magnetization jumps in Nd15Fe77B8 magnets is reported. The origin of these Barkhausen jumps in sintered magnets is discussed as a two-stage trigger/propagation process. The first stage may be dominated by magnetization reversal in volumes of δ3, where δ is the domain-wall thickness, as in the magnetic after effect, whereas the second stage reflects thermally induced domain-wall motion facilitated by the small lattice specific heat below about 10 K.
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  • 10
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The body-centered cubic FeRh is known to exhibit a first-order phase transition from antiferromagnetic to ferromagnetic at about 400 K, accompanied by a volume expansion of about 1%. The time evolution of the magnetization M of ordered Fe0.5Rh0.5 and FeRh0.958Pt0.042 just below and above the transition temperature (T0) was measured as functions of temperature and magnetic field. Around T0, the magnetization increased logarithmically with time up to M*(=41 emu/g), the value of which indicates that the ferromagnetic grains occupy one third of the antiferromagnetic matrix. When M=M*, there appeared a jump in M. After that, M varies as M(t) =M∞[1−exp(−t/τ)], where τ is a relaxation time. It should be noted that the value of M* is independent of both temperatures and external magnetic fields. Microscopic observation and x-ray diffraction measurement showed that the ferromagnetic grains nucleated in the antiferromagnetic matrix began to grow with time just below T0. In this work, the time evolution of the phase transition was analyzed by considering the magnetic free energy, the elastic energy, and the strain energy at the surface of the grains. The above mentioned magnetic relaxation process is deeply related to the time evolution of the grain size.
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