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  • 2000-2004  (2)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 6297-6301 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A series of Permalloy films, of various shapes such as a square, a rectangle, a circle, and a rhombus, was made. The sample length to width ratio L/w varied from 1 (i.e., square) to 29 (i.e., rectangle). We studied how the planar Hall effect (PHE) signal was affected by adding a transverse field Hy along the easy-axis direction of the sample. It was found that in a certain range of Hy, the PHE sensitivity S might become inoperative, i.e., S changed linearly as a function of Hy from −Smax to +Smax (or vice versa), where Smax was the maximum sensitivity. This phenomenon is explained by considering the Zeeman-energy and the single-domain-rotation effects. In particular, for the square sample, the following data exist: (1) Smax is as high as 310 Ω/T at the film thickness t=500 Å, and (2) the inoperative range for Hy is the narrowest among all the samples. From this study, we conclude that the field of the Earth He—as long as its horizontal component is larger than 0.25 Oe—can be employed to stabilize the magnetic structure of a Permalloy element and to achieve the best PHE performance with Smax. © 2001 American Institute of Physics.
    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 87 (2000), S. 8640-8644 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this paper, we briefly described how to use the vector or biaxial vibrating sample magnetometer (VSM) to determine the angular dispersion of easy axis in a magnetically soft film. For each angle of rotation φ of the external field H, a pair of the Mx-hysteresis and My-hysteresis loops could be obtained. Then, we changed the φ setting from negative to positive, with φ=0° indicating the exact direction of the hard axis of the film. Note, the easy axis has been induced by a deposition field h during fabrication of the film. From the characteristics of the Mx-hysteresis and My-hysteresis loops, the condition |φ|〈φc≅1° defines the "in-center zone," and the condition |φ|〉φc defines the "off-center zone." The types of switching modes for the in-center and off-center zones, respectively, are different. Only the hysteresis behaviors in the latter zone are understood well for detailed explanations. Then, the normalized change ΔMy/MS due to the wall motions at the switching field |H|=HSW can be used to indicate the angular dispersion Δθ in the film. Co70Fe10Ni20 films were made with various deposition conditions in order to cause different degrees of dispersion in them. The result shows that it is possible to study the angular dispersion in a magnetically soft film via the vectorial VSM measurements. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
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