Abstract
Non-volatile resistive switching, also known as memristor1 effect, where an electric field switches the resistance states of a two-terminal device, has emerged as an important concept in the development of high-density information storage, computing and reconfigurable systems2–9. The past decade has witnessed substantial advances in non-volatile resistive switching materials such as metal oxides and solid electrolytes. It was long believed that leakage currents would prevent the observation of this phenomenon for nanometre-thin insulating layers. However, the recent discovery of non-volatile resistive switching in two-dimensional monolayers of transition metal dichalcogenide10,11 and hexagonal boron nitride12 sandwich structures (also known as atomristors) has refuted this belief and added a new materials dimension owing to the benefits of size scaling10,13. Here we elucidate the origin of the switching mechanism in atomic sheets using monolayer MoS2 as a model system. Atomistic imaging and spectroscopy reveal that metal substitution into a sulfur vacancy results in a non-volatile change in the resistance, which is corroborated by computational studies of defect structures and electronic states. These findings provide an atomistic understanding of non-volatile switching and open a new direction in precision defect engineering, down to a single defect, towards achieving the smallest memristor for applications in ultra-dense memory, neuromorphic computing and radio-frequency communication systems2,3,11.
Original language | English |
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Pages (from-to) | 58-62 |
Number of pages | 5 |
Journal | Nature Nanotechnology |
Volume | 16 |
Issue number | 1 |
DOIs | |
State | Published - Jan 2021 |
Funding
This work was supported in part by the Presidential Early Career Award for Scientists and Engineers (PECASE) through the Army Research Office (W911NF-16-1-0277), and a National Science Foundation grant (ECCS-1809017). S.M.H. acknowledges support from a US S&T Cooperation Program. The facilities of the Center for Dynamics and Control of Materials: an NSF Materials Research Science and Engineering Center (MRSEC) was used for materials characterization. A portion of this research, including STM, transport measurements and STM simulations, was conducted at the Center for Nanophase Materials Sciences at Oak Ridge National Laboratory, which is a US Department of Energy User Facility. We thank W. R. Hendren and R. M. Bowman for their help with the metal film deposition.