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  • 1
    Publication Date: 2023-05-12
    Keywords: Conductivity, average; Depth, bottom/max; ELEVATION; Heat flow; LATITUDE; LONGITUDE; Method comment; Number; Number of conductivity measurements; Number of temperature data; Sample, optional label/labor no; Temperature gradient
    Type: Dataset
    Format: text/tab-separated-values, 49 data points
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 80 (1996), S. 5175-5182 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Co/Au multilayers have been prepared on glass substrates by electron-beam evaporation techniques. The perpendicular anisotropy is induced when the Co layer thickness is less than 12 A(ring) and its origin is discussed phenomenologically. In the perpendicular magnetic multilayers, large giant magnetoresistance appears and it consists of hysteretic and nonhysteretic components. The occurrence mechanism of these components has been discussed and it is suggested that the former arises from antiparallel spin alignment between adjacent Co layers due to the random wall position layer by layer, and the later is related to the granular-type giant magnetoresistance. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 365-372 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The structural phase and the magnetic anisotropy of Nd/Fe, Pr/Fe, and Gd/Fe multilayers have been examined using magnetization measurements and conversion electron Mössbauer spectrometry. With decreasing Fe layer thickness dFe, the structural phase of the Fe layer changes from bcc crystalline to amorphous at the critical thickness dFec of 17–20 A(ring) via an intermediate phase, which contains a paramagnetic phase in the Nd/Fe and Pr/Fe systems, but not in Gd/Fe. At just above dFec, Nd/Fe and Pr/Fe multilayers exhibit perpendicular anisotropy, which originates from the interface anisotropy due to the one ion anisotropy of Nd and Pr. However, Gd/Fe multilayers show in-plane magnetization because of the S-ionic Gd. Below dFec, the magnetization increases from nearly zero with decreasing dFe because of the exchange interaction between Fe and the rare earth (Nd,Pr,Gd). © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 6047-6049 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Co/Pt multilayers have been prepared by rf magnetron sputtering onto glass substrates with negative bias voltage. For 0-V bias, the film consists of the columns grown perpendicular to the substrate and the convex interfaces between layers. The column boundaries and the convex interfaces act as the pinning center for the domain wall motion resulting in the high perpendicular coercivity, Hc(⊥ ). In the −30-V biased multilayers, the columns are fine and close packed, and thereby the layer interfaces are smooth and sharp. So that Hc(⊥ ) is very small in these multilayers. Higher bias voltage of −70 V causes the obscure interfaces and decreases the anisotropy energy. In the Co/Pt multilayer deposited on 0 V-Pt underlayer, the coercivity Hc(⊥ ) increases with thickness of 0 V-Pt underlayer and reaches 4 kOe at 1000 A(ring) thickness. On the other hand, for −30 to −50-V Pt underlayer, the layer interfaces are smooth and sharp resulting in small Hc(⊥ ). Thus, Hc(⊥ ) is strongly affected by the film morphology such as the column boundaries or the layer interfaces.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 6209-6211 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Fe/DyFe multilayers were prepared by radio-frequency magnetron sputtering, where DyFe layers were amorphous and nonmagnetic at room temperature. When the Fe layer thickness dFe decreases, the crystallographic structure of the Fe layer changes from body-centered-cubic to amorphous at around 20 A(ring). At this critical thickness, the spontaneous magnetization and the Kerr rotation angle are nearly zero and the magnetization curve does not show hysteresis or saturation indicating its spin-glass-like or superparamagnetic nature. For dFe 〈 20 A(ring), the saturation magnetization and the Kerr rotation angle increase again due to the Fe-rich-DyFe amorphous alloy formed at the vicinity of the layer boundary with decreasing dFe. The perpendicular anisotropy increases with decreasing dFe because of the interfacial anisotropy Ks = 0.62 erg/cm2 in the crystalline region of dFe (approximately-greater-than) 20 A(ring).
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 57 (1985), S. 3204-3206 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Hall and ohmic resistivities of sputtered GdFe and CoCr films were measured at room temperature in the wide range of the film composition. It was suggested that the Hall effect is connected with the side-jump mechanism in both materials. Especially for ferrimagnetic GdFe films, the Hall effect was reasonably analyzed by assuming that the dominant contribution to the Hall effect is the Fe sublattice magnetic moment.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 57 (1985), S. 4034-4036 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Microstructure and temperature dependence of magnetic properties of Co-CoO films are studied. Columnar microstructure with chains of Co fine particles surrounded by CoO fine particles develops perpendicular to the film plane. Perpendicular anisotropy energy Ku takes a maximum value when the columnar diameter is minimum whose typical value is 1/20 of the film thickness. Change of magnetic domain structure with increasing Ku is studied. The perpendicular magnetization is restricted to the heterogeneous columnar microstructure. The perpendicular coercivity Hc decreases steeply with increasing temperature, that is associated probably with antiferromagnetic nature of CoO. Hc at room temperature increases after an annealing at 400–500 K.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 82 (1997), S. 4428-4434 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic properties and magnetoresistance (MR) are examined for the Fe/Au multilayers (MLs) prepared on glass substrates by electron-beam evaporation techniques as a function of the thicknesses of Fe and Au layers; dFe and dAu. For small dFe, the perpendicular magnetic anisotropy is induced, and in the films of dFe(approximate)5 Å, the stripe magnetic domain patterns are observed. In dFe≤3 Å, however, a superparamagnetic nature and a granular-type giant magnetoresistance (GMR) appear at room temperature. In a series of [Fe(3 Å)/Au(dAu)]40 MLs, the MR ratio increases with dAu and reaches the first peak at around 10 Å. On the other hand, at 14 K, the ferromagnetic component having a perpendicular anisotropy becomes dominant, and the GMR arises from the random wall alignment due to the antiferromagnetic coupling between the adjacent Fe layers, causing the first MR peak at dAu(approximate)10 Å. The layered structure is obscured and the superparamagnetic Fe grains are created by annealing at 300–350 °C, followed by the crystalline growth upon annealing at temperatures above 350 °C. These variations in the film morphology cause the changes in the saturation magnetization and the MR ratio. © 1997 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 82 (1997), S. 764-771 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Co–Ag granular films having various Co grain sizes are prepared by rf sputtering under various sputtering conditions. The Co grain sizes are derived from the magnetization curves by dividing them into ferromagnetic and superparamagnetic components. As the Co content decreases, the radii of the superparamagnetic Co grains, rg, decrease and the distances between the Co grains, tg, increase. The magnetoresistance is proportional to the volume density of superparamagnetic grains or related to krg3 exp(−tg/l) with k=3.8×102 μΩ/cm2 and l=20 Å, implying that the giant magnetoresistance is caused by the spin-dependent scattering in the inner part of the superparamagnetic Co grains as well as at the grain surfaces. Furthermore, it is found that the extraordinary Hall effect arises mainly from the side jump mechanism, and that significant perpendicular magnetic anisotropy appears in the Co composition range between 40 and 70 at %. © 1997 American Institute of Physics.
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  • 10
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magneto-optically active nanocomposite structures have been created by using ion implantation and thermal processing to form precipitated layers of ferromagnetic α-Fe or ferrimagnetic Fe3O4 that are embedded in the near-surface region of (100)-oriented yttrium stabilized ZrO2 (YSZ). When Fe-implanted YSZ is annealed at 1100 °C in Ar+4%H2, the redox conditions are sufficiently reducing so that metallic Fe is the stable phase. At lower temperatures the annealing conditions become less reducing and Fe3O4 becomes the stable phase. Transmission electron microscopy and x-ray diffraction studies established that each α-Fe or Fe3O4 particle is a single crystal that is crystallographically aligned with respect to the YSZ host. Magneto-optical effects due to both the α-Fe and Fe3O4 nanophase precipitates were found and characterized using magnetic circular dichroism. These magneto-optical effects have potential applications in integrated-optical devices. © 2000 American Institute of Physics.
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