<p>Spin and valley polarizations (<i>P</i><sub><i>s</i></sub> and <i>P</i><sub><i>KK’</i></sub>) and tunneling magnetoresistance (TMR) are demonstrated in the ferromagnetic/barrier/normal/barrier/ferromagnetic WSe<sub>2</sub> junction, with the gate voltage and off-resonant circularly polarized light (CPL) applied to the two barrier regions. The minimum incident energy of non-zero spin- and valley-resolved conductance has been derived, which is consistent with numerical calculations and depends on the electric potential <i>U</i>, CPL intensity ΔΩ, exchange field<i> h</i>, and magnetization configuration: parallel (P) or antiparallel (AP). For the P (AP) configuration, the energy region with <i>P</i><sub><i>KK’</i></sub> = -1 or <i>P</i><sub><i>s</i></sub> = 1 is wider (narrower) and increases with ΔΩ. As <i>h</i> increases, the <i>P</i><sub><i>s</i></sub> = 1 (<i>P</i><sub><i>KK’</i></sub> = -1 or <i>P</i><sub><i>s</i></sub> = 1) plateau becomes wider (narrower) for the P (AP) configuration. As <i>U</i> increases, the energy region with <i>P</i><sub><i>KK’</i></sub> = -1 increases first and then moves parallel to the <i>E</i><sub><i>F</i></sub>-axis, and the energy region with <i>P</i><sub><i>s</i></sub> = 1 for the P configuration remains unchanged first and then decreases. The energy region for TMR = 1 increases rapidly with <i>h</i>, remains unchanged first and then decreases as <i>U</i> increases, and has little dependence on ΔΩ. When the helicity of the CPL reverses, the valley polarization will switch. This work sheds light on the design of spin-valley and TMR devices based on ferromagnetic WSe<sub>2</sub> double-barrier junctions.</p>

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Spin and valley dependent transport and tunneling magnetoresistance in irradiated ferromagnetic WSe2double barrier junctions

  • Ming Li,
  • Zheng-Yin Zhao,
  • Jia-Yi Sheng

摘要

Spin and valley polarizations (Ps and PKK’) and tunneling magnetoresistance (TMR) are demonstrated in the ferromagnetic/barrier/normal/barrier/ferromagnetic WSe2 junction, with the gate voltage and off-resonant circularly polarized light (CPL) applied to the two barrier regions. The minimum incident energy of non-zero spin- and valley-resolved conductance has been derived, which is consistent with numerical calculations and depends on the electric potential U, CPL intensity ΔΩ, exchange field h, and magnetization configuration: parallel (P) or antiparallel (AP). For the P (AP) configuration, the energy region with PKK’ = -1 or Ps = 1 is wider (narrower) and increases with ΔΩ. As h increases, the Ps = 1 (PKK’ = -1 or Ps = 1) plateau becomes wider (narrower) for the P (AP) configuration. As U increases, the energy region with PKK’ = -1 increases first and then moves parallel to the EF-axis, and the energy region with Ps = 1 for the P configuration remains unchanged first and then decreases. The energy region for TMR = 1 increases rapidly with h, remains unchanged first and then decreases as U increases, and has little dependence on ΔΩ. When the helicity of the CPL reverses, the valley polarization will switch. This work sheds light on the design of spin-valley and TMR devices based on ferromagnetic WSe2 double-barrier junctions.