2005Physical Review BRequires access

Ferromagnetic semiconducting behavior of Mn1−xCrxTe compounds

Yameng Li, Y. Q. Zhang, N. K. Sun, Qiang Zhang, Dunhai Li, Jinze Li, Z. D. Zhang

Open publisher page 37 citations

Abstract

The magnetic and electrical transport properties of ferromagnetic semiconductor ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$ ($x=0.04$, 0.08, and 0.14) compounds have been investigated. These compounds have ferromagnetic behavior with hysteresis loops showing a coercivity of $300--985\phantom{\rule{0.3em}{0ex}}\mathrm{Oe}$ at $5\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. The hysteresis loop is observed even at room temperature for ${\mathrm{Mn}}_{0.86}{\mathrm{Cr}}_{0.14}\mathrm{Te}$. The substitution of Cr for Mn leads to a change from an antiferromagnetic state of MnTe to a ferromagnetic (or ferrimagnetic) state of ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$. Moreover, the incorporation of Cr into the host antiferromagnetic semiconductor MnTe lattice is confirmed by the structural characterization, which proves further that the ferromagnetic properties are not a result of the secondary phase. The typical feature of the thermally activated conduction processes for semiconductors has been verified by electrical property measurement.

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What this paper is about

The magnetic and electrical transport properties of ferromagnetic semiconductor ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$ ($x=0.04$, 0.08, and 0.14) compounds have been investigated. These compounds have ferromagnetic behavior with hysteresis loops showing a coercivity of $300--985\phantom{\rule{0.3em}{0ex}}\mathrm{Oe}$ at $5\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. The hysteresis loop is observed even at room temperature for ${\mathrm{Mn}}_{0.86}{\mathrm{Cr}}_{0.14}\mathrm{Te}$. The substitution of Cr for Mn leads to a change from an antiferromagnetic state of MnTe to a ferromagnetic (or ferrimagnetic) state of ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$. Moreover, the incorporation of Cr into the host antiferromagnetic semiconductor MnTe lattice is confirmed by the structural characterization, which proves further that the ferromagnetic properties are not a result of the secondary phase. The typical feature of the thermally activated conduction processes for semiconductors has been verified by electrical property measurement.

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Available abstract

The magnetic and electrical transport properties of ferromagnetic semiconductor ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$ ($x=0.04$, 0.08, and 0.14) compounds have been investigated. These compounds have ferromagnetic behavior with hysteresis loops showing a coercivity of $300--985\phantom{\rule{0.3em}{0ex}}\mathrm{Oe}$ at $5\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. The hysteresis loop is observed even at room temperature for ${\mathrm{Mn}}_{0.86}{\mathrm{Cr}}_{0.14}\mathrm{Te}$. The substitution of Cr for Mn leads to a change from an antiferromagnetic state of MnTe to a ferromagnetic (or ferrimagnetic) state of ${\mathrm{Mn}}_{1\ensuremath{-}x}{\mathrm{Cr}}_{x}\mathrm{Te}$. Moreover, the incorporation of Cr into the host antiferromagnetic semiconductor MnTe lattice is confirmed by the structural characterization, which proves further that the ferromagnetic properties are not a result of the secondary phase. The typical feature of the thermally activated conduction processes for semiconductors has been verified by electrical property measurement.

Key concepts: Antiferromagnetism, Ferromagnetism, Condensed matter physics, Ferrimagnetism, Materials science, Magnetic semiconductor, Hysteresis, Magnetoresistance

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