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Galvanomagnetic properties and magnetic domain structure of epitaxial MnAs films on GaAs(001)

Epitaxial MnAs films on GaAs(001) in the thickness range 20–200 nm were studied. Using ordinary and extraordinary Hall effect data to determine the field required for perpendicular saturation and saturation magnetizations reported elsewhere, we determined the shape anisotropy constant in the basal p...

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Published in:Journal of applied physics 1996-04, Vol.79 (8), p.4967-4969
Main Authors: Park, M. C., Park, Y., Shin, T., Rothberg, G. M., Tanaka, M., Harbison, J. P.
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Language:English
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cited_by cdi_FETCH-LOGICAL-c291t-22b60cdca0f304afec63067c1af05a6fcbf977d1e6658659f1931a59b58a375a3
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container_end_page 4969
container_issue 8
container_start_page 4967
container_title Journal of applied physics
container_volume 79
creator Park, M. C.
Park, Y.
Shin, T.
Rothberg, G. M.
Tanaka, M.
Harbison, J. P.
description Epitaxial MnAs films on GaAs(001) in the thickness range 20–200 nm were studied. Using ordinary and extraordinary Hall effect data to determine the field required for perpendicular saturation and saturation magnetizations reported elsewhere, we determined the shape anisotropy constant in the basal plane of the hexagonal structure to be 3.7(0.6)×105 erg/cm3 and the surface anisotropy constant to be −1.3(0.4) erg/cm2. The negative sign indicates thin enough films will be perpendicularly magnetized. By magnetic force microscopy of a 100 nm film we found stripe domains with 180° Bloch walls, thereby avoiding the hard c axis. The widths of the domains and the walls are 4.0(0.3) μm and 95(6) nm, respectively. In magnetoresistance, we observed behavior similar to other ferromagnets, namely peaks centered around the positive and negative coercive fields, and at fields beyond the coercive field a linear dependence on magnetic field. The electrical resistance showed rapid increase with temperature beginning about 5° below the Curie temperature (40 °C) caused by the change in crystal structure from hexagonal to orthorhombic. The resistivities are, respectively, 300(24) and 375(30) μΩ cm. Comparison with bulk values indicates the large lower temperature value is partly due to the presence of some orthorhombic phase observed in x-ray studies.
doi_str_mv 10.1063/1.361605
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C. ; Park, Y. ; Shin, T. ; Rothberg, G. M. ; Tanaka, M. ; Harbison, J. P.</creator><creatorcontrib>Park, M. C. ; Park, Y. ; Shin, T. ; Rothberg, G. M. ; Tanaka, M. ; Harbison, J. P.</creatorcontrib><description>Epitaxial MnAs films on GaAs(001) in the thickness range 20–200 nm were studied. Using ordinary and extraordinary Hall effect data to determine the field required for perpendicular saturation and saturation magnetizations reported elsewhere, we determined the shape anisotropy constant in the basal plane of the hexagonal structure to be 3.7(0.6)×105 erg/cm3 and the surface anisotropy constant to be −1.3(0.4) erg/cm2. The negative sign indicates thin enough films will be perpendicularly magnetized. By magnetic force microscopy of a 100 nm film we found stripe domains with 180° Bloch walls, thereby avoiding the hard c axis. The widths of the domains and the walls are 4.0(0.3) μm and 95(6) nm, respectively. In magnetoresistance, we observed behavior similar to other ferromagnets, namely peaks centered around the positive and negative coercive fields, and at fields beyond the coercive field a linear dependence on magnetic field. The electrical resistance showed rapid increase with temperature beginning about 5° below the Curie temperature (40 °C) caused by the change in crystal structure from hexagonal to orthorhombic. The resistivities are, respectively, 300(24) and 375(30) μΩ cm. 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title Galvanomagnetic properties and magnetic domain structure of epitaxial MnAs films on GaAs(001)
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