C. A. Bauer
University of South Florida
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Featured researches published by C. A. Bauer.
Journal of Applied Physics | 2011
Nicholas Laurita; A. Chaturvedi; C. A. Bauer; Priyanga Jayathilaka; Alex Leary; Casey W. Miller; Manh-Huong Phan; Michael E. McHenry; Hariharan Srikanth
A 50 nm-thick Co film has been grown either on the free surface (surface roughness, ∼6 nm) or on the wheel-side surface (surface roughness, ∼147 nm) of Co84.55Fe4.45Zr7B4 amorphous ribbons. A comparative study of the giant magnetoimpedance (GMI) effect and its field sensitivity (η) in the uncoated and Co-coated ribbons is presented. We show that the presence of the Co coating layer enhances both the GMI ratio and η in the Co-coated ribbons. Larger values for GMI ratio and η are achieved in the sample with Co coated on the free ribbon surface. The enhancement of the GMI effect in the Co-coated ribbons originates mainly from the reduction in stray fields due to surface irregularities and the enhanced magnetic flux paths closure. These findings provide good guidance for tailoring GMI in surface-modified soft ferromagnetic ribbons for use in highly sensitive magnetic sensors.
Journal of Applied Physics | 2013
M. S. Lucas; Dustin D. Belyea; C. A. Bauer; N. Bryant; E. Michel; Zafer Turgut; S. O. Leontsev; John C. Horwath; S. L. Semiatin; Michael E. McHenry; Casey W. Miller
The equimolar alloy FeCoCrNi, a high-entropy alloy, forms in the face-centered-cubic crystal structure and has a ferromagnetic Curie temperature of 130 K. In this study, we explore the effects of Cr concentration, cold-rolling, and subsequent heat treatments on the magnetic properties of FeCoCrxNi alloys. Cr reductions result in an increase of the Curie temperature, and may be used to tune the TC over a very large temperature range. The magnetic entropy change for a change in applied field of 2T is ΔSm = −0.35 J/(kg K) for cold-rolled FeCoCrNi. Cold-rolling results in a broadening of ΔSm, where subsequent heat treatment at 1073 K sharpens the magnetic entropy curve. In all of the alloys, we find that upon heating (after cold-rolling) there is a re-entrant magnetic moment near 730 K. This feature is much less pronounced in the as-cast samples (without cold-rolling) and in the Cr-rich samples, and is no longer observed after annealing at 1073 K. Possible origins of this behavior are discussed.
Journal of Applied Physics | 2011
Brian J. Kirby; June W. Lau; D. V. Williams; C. A. Bauer; Casey W. Miller
Polarized neutron reflectometry was used to determine the depth profile of the magnetic moment per Gd atom, mGd, in a Gd(30 nm)/W(5 nm) multilayer. Despite sharp interfaces observed by transmission electron microscopy, mGd is systematically suppressed near the Gd-W interfaces. Because the peak magnetic entropy change is proportional to mGd2/3, this results in a reduction of the maximum achievable magnetocaloric effect in Gd-W heterostructures. By extension, our results suggest that creating materials with Gd-ferromagnet interfaces may increase the mGd relative to the bulk, leading to enhanced magnetocaloric properties.
Journal of Applied Physics | 2010
Priyanga Jayathilaka; C. A. Bauer; D. V. Williams; M. C. Monti; John T. Markert; Casey W. Miller
3000 A Fe3O4 (magnetite) thin films were simultaneously grown on (001) MgO single crystal substrates with and without 30 A buffer layers of Fe, Cr, Mo, and Nb. For all samples, the Verwey transition temperature (TV) occurs between 119 and 125 K, indicating good oxygen stoichiometry. We observe highly oriented (001) Fe3O4 with Mo and no buffer layer, reduced (001) texture with Nb and Fe, and polycrystalline growth with Cr. Mo, Cr, and unbuffered magnetite show typical magnetic behavior, whereas Nb and Fe buffers lead to anomalous magnetic properties that may be due to interfacial reactivity.
Applied Physics Letters | 2010
Alfred Lee; Priyanga Jayathilaka; C. A. Bauer; Mark C. Monti; John T. Markert; A. L. de Lozanne; Casey W. Miller
Magnetic force microscopy was performed on 300 nm thick magnetite films grown epitaxially on MgO (001) at temperatures ranging from well below to well above the Verwey transition temperature, TV. Frequency shift images were acquired at different locations on the sample as temperature was increased through the Verwey transition. The magnetic domain features are persistent at all temperatures, which indicates that the domains are pinned across the phase transition, probably due to antiphase boundaries. An enhancement of magnetic contrast below TV indicates the moments tilt out of the plane below TV, which is corroborated by superconducting quantum interference device magnetometry.
IEEE Transactions on Magnetics | 2010
Priyanga Jayathilaka; C. A. Bauer; D. V. Williams; Casey W. Miller
Thin films of Ni80Fe20, Fe3O4, as well as Ni80Fe20/Cr/Fe3O4 spin valves, have been grown with and without magnetic fields applied during the deposition, and their magnetotransport properties have been studied at room temperature. The applied field induces an anisotropy in both single layer films, which causes notable differences in their anisotropic magnetoresistance. In the spin valve system, the applied field enables the parallel and antiparallel states to be more well-defined, which reveals a possible giant magnetoresistance in the system. The origin of this signal is likely the interaction of electrons that have been polarized by spin-dependent reflection from the Cr/Fe3O4 interface with the Ni80Fe20 interface.
Bulletin of the American Physical Society | 2012
Dustin D. Belyea; C. A. Bauer; M. S. Lucas; J. Horwath; E. Michel; Casey W. Miller
Archive | 2011
C. A. Bauer
Bulletin of the American Physical Society | 2011
C. A. Bauer; Priyanga Jayathilaka; R.V. Rupani; Dustin D. Belyea; Casey W. Miller
Applied Physics Letters | 2011
Brian J. Kirby; June W. Lau; D. V. Williams; C. A. Bauer; Casey W. Miller