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Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
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Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
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Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass

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Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass
Journal Article

Spin-dependent resonant tunneling in CdTe/Cd.sub.1-xMn.sub.xTe nanostructures: effect of polaronic mass

2025
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Overview
Effect of polaronic mass on the resonant tunneling of electrons in CdTe/Cd.sub.1-xMn.sub.xTe double-barrier heterostructure is investigated. The well-known transfer matrix method is employed to calculate the barrier transparency. One can obtain a high degree of spin-polarization at a high concentration of Mn in the barrier region. The barrier transparency peak becomes narrow as the concentration of Mn increases from 10 to 20%. The effect of polaronic mass shifts the transparency peak to the lower value on the energy scale. One can obtain a high degree of spin-polarization at a high concentration of Mn in the barrier region. The account of the polaronic mass shifts the resonance energy of spin-polarization to the lower value and it enhances the spin-polarization. The spin-down electrons spend more time in the heterostructure than the spin-up electrons. The dwell time changes about 1000 times as the concentration of the barrier changes.
Publisher
Springer
Subject