TY - JOUR
T1 - Defect dynamics in 2-D MoS2 probed by using machine learning, atomistic simulations, and high-resolution microscopy
AU - Patra, Tarak K.
AU - Zhang, Fu
AU - Schulman, Daniel S.
AU - Chan, Henry
AU - Cherukara, Mathew J.
AU - Terrones, Mauricio
AU - Das, Saptarshi
AU - Narayanan, Badri
AU - Sankaranarayanan, Subramanian K.R.S.
N1 - Funding Information:
This work was supported by Argonne LDRD-2017-012-N0. Use of the Center for Nanoscale Materials and the resources of the Argonne Leadership Computing Facility was also supported by the U.S. Department of Energy (DOE), Office of Science, Office of Basic Science, under Contract No. DE-AC02-06CH11357. This research used resources of the National Energy Research Scientific Computing Center, a DOE office of science user facility supported by the Office of Science of the US Department of Energy under Contract No. DE-AC02-05CH11231. An award of computer time was provided by the Innovative and Novel Computational Impact on Theory and Experiment (INCITE) program. This research used resources of the Argonne Leadership Computational Facility, which is a DOE Office of Science user facility supported under Contract No. DE-AC02-06CH11357. T.K.P. thanks Prof. David Simmons, University of Akron, for providing the GA code, which is modified and used for this work. D.S.S. and S.D. acknowledge support from the Air Force Office of Scientific Research (AFOSR) through the Young Investigator Program with Grant No. FA9550-17-1-0018. F. Z. and M. T. acknowledge the NSF-IUCRC Center for Atomically Thin Multifunctional Coatings 275 (ATOMIC), under award #1540018.
Funding Information:
This work was supported by Argonne LDRD-2017-012-N0. Use of the Center for Nanoscale Materials and the resources of the Argonne Leadership Computing Facility was also supported by the U.S. Department of Energy (DOE), Office of Science, Office of Basic Science under Contract No. DE-AC02-06CH11357. This research used resources of the National Energy Research Scientific Computing Center, a DOE office of science user facility supported by the Office of Science of the US Department of Energy under Contract No. DE-AC02-05CH11231. An award of computer time was provided by the Innovative and Novel Computational Impact on Theory and Experiment (INCITE) program. This research used resources of the Argonne Leadership Computational Facility which is a DOE Office of Science user facility supported under Contract No. DE-AC02-06CH11357. T.K.P. thanks Prof. David Simmons, University of Akron, for providing the GA code, which is modified and used for this work. D.S.S. and S.D. acknowledge support from the Air Force Office of Scientific Research (AFOSR) through the Young Investigator Program with Grant No. FA9550-17-1-0018. F. Z. and M. T. acknowledge the NSF-IUCRC Center for Atomically Thin Multifunctional Coatings 275 (ATOMIC), under award #1540018.
Publisher Copyright:
© 2018 American Chemical Society.
PY - 2018/8/28
Y1 - 2018/8/28
N2 - Structural defects govern various physical, chemical, and optoelectronic properties of two-dimensional transition-metal dichalcogenides (TMDs). A fundamental understanding of the spatial distribution and dynamics of defects in these low-dimensional systems is critical for advances in nanotechnology. However, such understanding has remained elusive primarily due to the inaccessibility of (a) necessary time scales via standard atomistic simulations and (b) required spatiotemporal resolution in experiments. Here, we take advantage of supervised machine learning, in situ high-resolution transmission electron microscopy (HRTEM) and molecular dynamics (MD) simulations to overcome these limitations. We combine genetic algorithms (GA) with MD to investigate the extended structure of point defects, their dynamical evolution, and their role in inducing the phase transition between the semiconducting (2H) and metallic (1T) phase in monolayer MoS2. GA-based structural optimization is used to identify the long-range structure of randomly distributed point defects (sulfur vacancies) for various defect densities. Regardless of the density, we find that organization of sulfur vacancies into extended lines is the most energetically favorable. HRTEM validates these findings and suggests a phase transformation from the 2H-to-1T phase that is localized near these extended defects when exposed to high electron beam doses. MD simulations elucidate the molecular mechanism driving the onset of the 2H to 1T transformation and indicate that finite amounts of 1T phase can be retained by increasing the defect concentration and temperature. This work significantly advances the current understanding of defect structure/evolution and structural transitions in 2D TMDs, which is crucial for designing nanoscale devices with desired functionality.
AB - Structural defects govern various physical, chemical, and optoelectronic properties of two-dimensional transition-metal dichalcogenides (TMDs). A fundamental understanding of the spatial distribution and dynamics of defects in these low-dimensional systems is critical for advances in nanotechnology. However, such understanding has remained elusive primarily due to the inaccessibility of (a) necessary time scales via standard atomistic simulations and (b) required spatiotemporal resolution in experiments. Here, we take advantage of supervised machine learning, in situ high-resolution transmission electron microscopy (HRTEM) and molecular dynamics (MD) simulations to overcome these limitations. We combine genetic algorithms (GA) with MD to investigate the extended structure of point defects, their dynamical evolution, and their role in inducing the phase transition between the semiconducting (2H) and metallic (1T) phase in monolayer MoS2. GA-based structural optimization is used to identify the long-range structure of randomly distributed point defects (sulfur vacancies) for various defect densities. Regardless of the density, we find that organization of sulfur vacancies into extended lines is the most energetically favorable. HRTEM validates these findings and suggests a phase transformation from the 2H-to-1T phase that is localized near these extended defects when exposed to high electron beam doses. MD simulations elucidate the molecular mechanism driving the onset of the 2H to 1T transformation and indicate that finite amounts of 1T phase can be retained by increasing the defect concentration and temperature. This work significantly advances the current understanding of defect structure/evolution and structural transitions in 2D TMDs, which is crucial for designing nanoscale devices with desired functionality.
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U2 - 10.1021/acsnano.8b02844
DO - 10.1021/acsnano.8b02844
M3 - Article
C2 - 30074765
AN - SCOPUS:85052305834
SN - 1936-0851
VL - 12
SP - 8006
EP - 8016
JO - ACS Nano
JF - ACS Nano
IS - 8
ER -