2011
DOI: 10.1103/physrevb.84.024428
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Theory and simulation of spin transport in antiferromagnetic semiconductors: Application to MnTe

Abstract: In this paper we study the parallel spin current in an antiferromagnetic semiconductor thin film where we take into account the interaction between itinerant spins and lattice spins. The spin model is an anisotropic Heisenberg model. Here we use the Boltzmann equation with numerical data on cluster distribution obtained by Monte Carlo simulations and cluster-construction algorithms. We study the cases of degenerate and nondegenerate semiconductors. The spin resistivity in both cases is shown to depend on the t… Show more

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Cited by 21 publications
(22 citation statements)
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“…The values we used to obtain that agreement are A = 1 and the Heisenberg critical exponents ν = 0.707, z = 1.97 [23]. In the temperature regions below T < 140 K and above T N the MC result is also in excellent agreement with experiment, unlike in our previous work [18] using the Boltzmann equation.…”
Section: Frustrated Systemssupporting
confidence: 59%
“…The values we used to obtain that agreement are A = 1 and the Heisenberg critical exponents ν = 0.707, z = 1.97 [23]. In the temperature regions below T < 140 K and above T N the MC result is also in excellent agreement with experiment, unlike in our previous work [18] using the Boltzmann equation.…”
Section: Frustrated Systemssupporting
confidence: 59%
“…6 We have shown by MC simulations that this is true, however the form of the rounded peak depends on the crystal structure and other interaction parameters. 10,11 Experimentally, there has been a large number of works dealing with the spin resistivity in different magnetic compounds. 12,13,14,15,16,17,18,19,20,21,22 These experiments show the existence of an anomaly of ρ at the magnetic phase transition.…”
Section: Introductionmentioning
confidence: 99%
“…In order to study the effects of MI-MI exchange interactions on the behavior of surface conductivity, we consider magnetic clusters as scattering centers and suppose that Dirac electrons interact with these centers rather than single impurities 23,24 . By defining the parameter ξ as the mean size of magnetic clusters, we model the interaction of a Dirac electron located at r with a cluster centered at R as:…”
Section: Our Modelmentioning
confidence: 99%
“…23,24 to explain the temperature dependence of magneto-resistance of magnetic semiconductors. The clusters' mean size (CMS) and the number of clusters with mean sizes (CN) depend on temperature, they increase by increasing temperature, pass through a maximum at a critical temperature, and decrease toward zero at high temperatures 23,24 . We model the scattering of massless Dirac electrons off magnetic clusters with a potential, exponentially decaying with the electron-cluster separation distance rescaled by the CMS.…”
Section: Introductionmentioning
confidence: 99%