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• W2016145831 abstract "The real and imaginary parts of magnetic permeability at the three frequencies 100 Hz, 1 kHz and 10 kHz and magnetic moment in magnetic field H = 0.05 T in the Sm <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>X</sub> Mn <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>1-X</sub> S(0.1 ≤ × ≤ 0.25) solid solutions at the temperatures 5 K-300 K were measured. Magnetization curves were measured in the range of fields - 9 T <; H <; 9 T at the temperatures T = 5 K, 50 K. Non-linear behavior of the magnetization versus field, residual magnetic moment, logarithmic dependence of imaginary parts of the magnetic permeability maximum on frequency and sharp drop of Im(μ) at T <; 40 K for compound Sm <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>0.25</sub> Mn <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>0.75</sub> S were found. The electrical resistivity of the Sm <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>X</sub> Mn <sub xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>1-X</sub> S(0.15 <; x <; 0.25) solid solution in the range of temperatures 80 K-300 K were measured. Minimum and maximum in the temperature dependence of the resistivity were found respectively at T = 220 K for X = 0.15 and at T = 100 K for X = 0.2 compounds. This behavior is explained a result of the mobility edge movement and the disorder of the deformation and spin density fluctuations with short-range order." @default.
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• W2016145831 date "2011-10-01" @default.
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• W2016145831 title "Nonuniform Magnetic States and Electrical Properties of ${rm Sm}_{rm X}{rm Mn}_{1-{rm X}}{rm S}$ Solid Solutions" @default.
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• W2016145831 doi "https://doi.org/10.1109/tmag.2011.2160715" @default.
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