TY - JOUR
T1 - Electrical Control of Circular Photogalvanic Spin-Valley Photocurrent in a Monolayer Semiconductor
AU - Liu, Lei
AU - Lenferink, Erik J.
AU - Wei, Guohua
AU - Stanev, Teodor K.
AU - Speiser, Nathaniel
AU - Stern, Nathaniel P.
N1 - Funding Information:
This work was supported by the Office of Naval Research under Grant no. N00014-16-1-3055 (L.L.), the U.S. Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering under Award no. DESC0012130 (E.J.L., G.W.), and the National Science Foundation MRSEC program under grant No. DMR-1720139 (T.K.S.) at the Materials Research Center of Northwestern University. This work utilized Northwestern University Micro/Nano Fabrication Facility (NUFAB) and the EPIC facility of Northwestern University’s NUANCE Center, which have received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-1542205); the MRSEC program (NSF DMR-1720139) at the Materials Research Center; the International Institute for Nanotechnology (IIN); the Keck Foundation; and the State of Illinois.
Publisher Copyright:
© 2018 American Chemical Society.
PY - 2019/1/23
Y1 - 2019/1/23
N2 - In a monolayer transition metal dichalcogenide (TMDC) that lacks structural inversion symmetry, spin degeneracy is lifted by strong spin-orbit coupling, and a distinctive spin-valley locking allows for the creation of valley-locked spin-polarized carriers with a circularly polarized optical excitation. When excited carriers also have net in-plane momentum, spin-polarized photocurrents can be generated at ambient temperature without magnetic fields or materials. The behavior of these spin-polarized photocurrents in monolayer TMDC remains largely unexplored. In this work, we demonstrate the tuning of spin-valley photocurrent generated from the circularly polarized photogalvanic effect in monolayer MoS 2 , including magnitude and polarization degree, by purely electric means at room temperature. The magnitude of spin-polarized photocurrent can be modulated up to 45 times larger, and the polarization degree of the total photocurrent can be tuned significantly (here from 0.5 to 16.6%) by gate control. Combined with the atomic thickness and wafer-scale growth capabilities of monolayer TMDC, the efficient electrical tuning of spin-valley photocurrent suggests a pathway to achieve spin-logic processing by local gate architectures in monolayer opto-spintronic devices.
AB - In a monolayer transition metal dichalcogenide (TMDC) that lacks structural inversion symmetry, spin degeneracy is lifted by strong spin-orbit coupling, and a distinctive spin-valley locking allows for the creation of valley-locked spin-polarized carriers with a circularly polarized optical excitation. When excited carriers also have net in-plane momentum, spin-polarized photocurrents can be generated at ambient temperature without magnetic fields or materials. The behavior of these spin-polarized photocurrents in monolayer TMDC remains largely unexplored. In this work, we demonstrate the tuning of spin-valley photocurrent generated from the circularly polarized photogalvanic effect in monolayer MoS 2 , including magnitude and polarization degree, by purely electric means at room temperature. The magnitude of spin-polarized photocurrent can be modulated up to 45 times larger, and the polarization degree of the total photocurrent can be tuned significantly (here from 0.5 to 16.6%) by gate control. Combined with the atomic thickness and wafer-scale growth capabilities of monolayer TMDC, the efficient electrical tuning of spin-valley photocurrent suggests a pathway to achieve spin-logic processing by local gate architectures in monolayer opto-spintronic devices.
KW - circular photogalvanic effect
KW - electrostatic screening
KW - gate control
KW - monolayer transition metal dichalcogenide
KW - spin-valley photocurrent
UR - http://www.scopus.com/inward/record.url?scp=85060489140&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85060489140&partnerID=8YFLogxK
U2 - 10.1021/acsami.8b17476
DO - 10.1021/acsami.8b17476
M3 - Article
C2 - 30582322
AN - SCOPUS:85060489140
VL - 11
SP - 3334
EP - 3341
JO - ACS applied materials & interfaces
JF - ACS applied materials & interfaces
SN - 1944-8244
IS - 3
ER -