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Magnetic properties of the layered III-VI diluted magnetic semiconductor Ga1−x Fe x Te
Magnetic properties of single crystalline Ga1−x Fe x Te (x = 0.05) have been measured. GaTe and related layered III-VI semiconductors exhibit a rich collection of important properties for THz generation and detection. The magnetization versus field for an x = 0.05 sample deviates from the linear res...
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Published in: | AIP advances 2016-05, Vol.6 (5) |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Magnetic properties of single crystalline Ga1−x
Fe
x
Te (x = 0.05) have been measured. GaTe and related layered III-VI semiconductors exhibit a rich collection of important properties for THz generation and detection. The magnetization versus field for an x = 0.05 sample deviates from the linear response seen previously in Ga1−x
Mn
x
Se and Ga1−x
Mn
x
S and reaches a maximum of 0.68 emu/g at 2 K in 7 T. The magnetization of Ga1−x
Fe
x
Te saturates rapidly even at room temperature where the magnetization reaches 50% of saturation in a field of only 0.2 T. In 0.1 T at temperatures between 50 and 400 K, the magnetization drops to a roughly constant 0.22 emu/g. In 0 T, the magnetization drops to zero with no hysteresis present. The data is consistent with Van-Vleck paramagnetism combined with a pronounced crystalline anisotropy, which is similar to that observed for Ga1−x
Fe
x
Se. Neither the broad thermal hysteresis observed from 100-300 K in In1−x
Mn
x
Se nor the spin-glass behavior observed around 10.9 K in Ga1−x
Mn
x
S are observed in Ga1−x
Fe
x
Te. Single crystal x-ray diffraction data yield a rhombohedral space group bearing hexagonal axes, namely R3c. The unit cell dimensions were a = 5.01 Å, b = 5.01 Å, and c = 17.02 Å, with α = 90°, β = 90°, and γ = 120° giving a unit cell volume of 369 Å3. |
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ISSN: | 2158-3226 2158-3226 |
DOI: | 10.1063/1.4945335 |