Realization of valley-spin polarized current via parametric pump in monolayer

Monolayer ${\mathrm{MoS}}_2$ is a typical valleytronic material with valley-spin locked valence bands. We numerically investigate the valley-spin polarized current in monolayer ${\mathrm{MoS}}_2$ via adiabatic electron pumping. By introducing an exchange field to break the energy degeneracy of monol...

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Published in:New Journal of Physics
Main Authors: Kai-Tong Wang, Hui Wang, Fuming Xu, Yunjin Yu, Yadong Wei
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/acb22e
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author Kai-Tong Wang
Hui Wang
Fuming Xu
Yunjin Yu
Yadong Wei
author_facet Kai-Tong Wang
Hui Wang
Fuming Xu
Yunjin Yu
Yadong Wei
author_sort Kai-Tong Wang
collection DOAJ
container_title New Journal of Physics
description Monolayer ${\mathrm{MoS}}_2$ is a typical valleytronic material with valley-spin locked valence bands. We numerically investigate the valley-spin polarized current in monolayer ${\mathrm{MoS}}_2$ via adiabatic electron pumping. By introducing an exchange field to break the energy degeneracy of monolayer ${\mathrm{MoS}}_2$ , the top of its valence bands is valley-spin polarized and tunable by the exchange field. A device with spin-up polarized left lead, spin-down polarized right lead, and untuned central region is constructed through applying different exchange fields in the corresponding regions. Then, equal amount of pumped currents with opposite valley-spin polarization are simultaneously generated in the left and right leads when periodically varying two pumping potentials. Numerical results show that the phase difference between the pumping potentials can change the direction and hence polarization of the pumped currents. It is found that the pumped current exhibits resonant behavior in the valley-spin locked energy window, which depends strongly on the system size and is enhanced to resonant current peaks at certain system lengths. More importantly, the pumped current periodically oscillates as a function of the system length, which is closely related to the oscillation of transmission. The effects of other system parameters, such as the pumping amplitude and the static potential, are also thoroughly discussed.
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spelling doaj-art-be83b4f2ce8b499fbbea697d6bc55bda2025-08-19T22:01:42ZengIOP PublishingNew Journal of Physics1367-26302023-01-0125101301910.1088/1367-2630/acb22eRealization of valley-spin polarized current via parametric pump in monolayerKai-Tong Wang0Hui Wang1Fuming Xu2Yunjin Yu3Yadong Wei4College of Physics and Optoelectronic Engineering, Shenzhen University , Shenzhen 518060, People’s Republic of China; School of Physics and Engineering, Henan University of Science and Technology , Luoyang 471023, People’s Republic of ChinaSchool of Physics and Engineering, Henan University of Science and Technology , Luoyang 471023, People’s Republic of ChinaCollege of Physics and Optoelectronic Engineering, Shenzhen University , Shenzhen 518060, People’s Republic of ChinaCollege of Physics and Optoelectronic Engineering, Shenzhen University , Shenzhen 518060, People’s Republic of ChinaCollege of Physics and Optoelectronic Engineering, Shenzhen University , Shenzhen 518060, People’s Republic of ChinaMonolayer ${\mathrm{MoS}}_2$ is a typical valleytronic material with valley-spin locked valence bands. We numerically investigate the valley-spin polarized current in monolayer ${\mathrm{MoS}}_2$ via adiabatic electron pumping. By introducing an exchange field to break the energy degeneracy of monolayer ${\mathrm{MoS}}_2$ , the top of its valence bands is valley-spin polarized and tunable by the exchange field. A device with spin-up polarized left lead, spin-down polarized right lead, and untuned central region is constructed through applying different exchange fields in the corresponding regions. Then, equal amount of pumped currents with opposite valley-spin polarization are simultaneously generated in the left and right leads when periodically varying two pumping potentials. Numerical results show that the phase difference between the pumping potentials can change the direction and hence polarization of the pumped currents. It is found that the pumped current exhibits resonant behavior in the valley-spin locked energy window, which depends strongly on the system size and is enhanced to resonant current peaks at certain system lengths. More importantly, the pumped current periodically oscillates as a function of the system length, which is closely related to the oscillation of transmission. The effects of other system parameters, such as the pumping amplitude and the static potential, are also thoroughly discussed.https://doi.org/10.1088/1367-2630/acb22evalleytronicsmonolayer MoS2parametric pumpvalley-spin polarization
spellingShingle Kai-Tong Wang
Hui Wang
Fuming Xu
Yunjin Yu
Yadong Wei
Realization of valley-spin polarized current via parametric pump in monolayer
valleytronics
monolayer MoS2
parametric pump
valley-spin polarization
title Realization of valley-spin polarized current via parametric pump in monolayer
title_full Realization of valley-spin polarized current via parametric pump in monolayer
title_fullStr Realization of valley-spin polarized current via parametric pump in monolayer
title_full_unstemmed Realization of valley-spin polarized current via parametric pump in monolayer
title_short Realization of valley-spin polarized current via parametric pump in monolayer
title_sort realization of valley spin polarized current via parametric pump in monolayer
topic valleytronics
monolayer MoS2
parametric pump
valley-spin polarization
url https://doi.org/10.1088/1367-2630/acb22e
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AT fumingxu realizationofvalleyspinpolarizedcurrentviaparametricpumpinmonolayer
AT yunjinyu realizationofvalleyspinpolarizedcurrentviaparametricpumpinmonolayer
AT yadongwei realizationofvalleyspinpolarizedcurrentviaparametricpumpinmonolayer