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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 6212-6214 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on the magnetic properties of Er/Mo multilayers and compare to our earlier work on Dy80Ni20/Mo multilayers. The magnetic order in these multilayers is not collinear and most likely is speromagnetic, much like a spin glass. Magnetic fields as high as 55 kOe do not saturate the magnetization. Both the interface anisotropy Ks and the bulk anisotropy are determined. We find a qualitative correlation between Ks and the single ion anisotropy (calculated from the bulk anisotropy) with Dy multilayers where the single ion anisotropy is larger having a larger value of Ks than Er multilayers.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 5292-5294 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Dy80Ni20/Mo multilayers have been prepared by sputtering and the effects of the interface on the magnetic anisotropy of these materials are reported. A large interface anisotropy is found but it is somewhat smaller than that estimated from a point-charge model assuming a sharp interface.
    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 87 (2000), S. 6137-6139 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Thin amorphous Dy50Fe50/A layers are prepared by sputtering to understand the influence of the spacer layer A on magnetic properties in the DyFe thickness regime where size effects are also important. The spacer layer A in this work is either Ti or Ca and we compare to our earlier work involving a spacer layer of Mo. The Dy50Fe50 layer is amorphous and Mössbauer spectroscopy indicates that two types of Fe site are present. Finite size effects manifest themselves below a size of 10 nm in a reduction of magnetic ordering temperature TC and coercivity HC. For equal values of d, the reduction of TC and HC is larger for the system with a Ti or Mo spacer layer as compared to the Ca spacer layer. We argue that both size and the structure of the interface are important in lowering HC and TC. The temperature dependence of coercivity is also studied and suggests that magnetic reversal via domain wall movement occurs in our thinnest films. © 2000 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 85 (1999), S. 4322-4324 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Elemental rare-earths R (Gd, Dy, Tb) are prepared in layer and particle form to look at the effects of geometry (layers or particles) and size (layer thickness or particle diameter) on their magnetism. All of the rare-earth systems show a maximum in coercivity (measured at 4.5 K) at about 10 nm (average particle diameter or layer thickness). Magnetic ordering temperature is reduced significantly compared to the bulk when size is reduced below 10 nm for both the layer and the particle geometry. Geometry has a significant effect on the maximum coercivity with particles tending to have larger coercivity than layers. © 1999 American Institute of Physics.
    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 76 (1994), S. 6174-6176 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on finite size effects and evidence for quantum mesoscopic tunneling (QMT) in thin isolated rare-earth layers prepared in the form of R/Mo multilayers where R represents Tb, Dy, or Dy50Co50. The magnetic transition temperature Tc decreases with decreasing magnetic layer thickness and is discussed within a finite size scaling theory. Evidence for QMT is found in magnetic relaxation measurements in these systems with a sharp crossover to a temperature-independent magnetic relaxation regime at low temperatures. The Tb system has a crossover temperature T0 of 20 K, the largest value reported so far for this crossover.
    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 75 (1994), S. 5643-5643 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on the magnetic properties of Dy(t A(ring))/Mo(d A(ring)), DyCo(t A(ring))/Mo(d A(ring)), and Gd(t A(ring))/Mo(d A(ring)) multilayers where d=180 A(ring) and t ranges from 10 to 3000 A(ring). We find a decrease in Tc with decreasing t, with the most rapid decrease occurring for the Gd system where the anisotropy is the weakest. We have looked at the time dependence of magnetization in the anisotropic systems (Dy based). At long times (5×104 s) the magnetization shows a stretched exponential dependence on time as is found in other magnetically disordered systems. We have also looked at the rate of magnetic relaxation at short times (〈1000 s) and find that it becomes independent of temperature below a temperature in the range 3–6 K depending on the magnetic layer thickness t. We shall consider the possibility of macroscopic quantum tunneling here and estimate the temperature, T*, below which a system is expected to cross over from thermally activated to quantum tunneling.1,2 We shall also compare our results to previous work on Dy/Cu.3
    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 79 (1996), S. 5299-5301 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Tb nanoscale particles are prepared in a matrix of Ti by sputtering. A range of samples are made with average particle diameter ranging from 1.5 to 21 nm. The magnetic transition temperature is depressed for smaller particles due to finite size effects. The coercivity at 4.5 K shows a maximum of 22 kOe at approximately 7 nm being a factor of 2.4 larger than a thick film of Tb. We compare the coercivity of our particle samples to multilayers of the form Tb/Mo and find larger coercivity in the particle systems due to the more confined geometry of the particles. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 9 (1997), S. 376-391 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Advective nonsolenoidal ((bold del)⋅v≠0) flow driven by diffusion-induced density changes in strictly zero gravity is studied in a two-dimensional rectangular box. Our model, which is more general than the Oberbeck–Boussinesq model, is a precursor for the study of fluid flow that occurs due to density changes during isothermal interdiffusion in a binary liquid under the influence of stochastic microgravity (g-jitter). We consider perturbation expansions of mass fraction (w) of the second chemical component of a binary solution, pressure (p), velocity (v), and chemical flux (j) with respect to a small parameter α [=ρ0∂(1/ρ)/∂w], where ρ is the density and ρ0 is its value for some average composition. The total barycentric velocity field is given by the sum of an average flow, having a nonzero divergence, and a solenoidal flow derived from a pseudo-stream-function. At first order in α, we obtain a fourth order partial differential equation for this pseudo-stream-function. We solve this equation analytically in a quasi-steady-state approximation for an infinitely long diffusion couple by using transform techniques. We also solve it numerically for the full time-dependent problem for a finite domain. We conclude that such nonsolenoidal flows will dominate for sufficiently small gravity, for which the Oberbeck–Boussinesq approximation will certainly not be valid. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of natural products 47 (1984), S. 835-838 
    ISSN: 1520-6025
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of natural products 50 (1987), S. 89-101 
    ISSN: 1520-6025
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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