Abstract
Grain boundaries in monolayer transition metal dichalcogenides have unique atomic defect structures and band dispersion relations that depend on the inter-domain misorientation angle. Here, we explore misorientation angle-dependent electrical transport at grain boundaries in monolayer MoS2 by correlating the atomic defect structures of measured devices analysed with transmission electron microscopy and first-principles calculations. Transmission electron microscopy indicates that grain boundaries are primarily composed of 5–7 dislocation cores with periodicity and additional complex defects formed at high angles, obeying the classical low-angle theory for angles <22°. The inter-domain mobility is minimized for angles <9° and increases nonlinearly by two orders of magnitude before saturating at ∼16 cm2 V−1 s−1 around misorientation angle≈20°. This trend is explained via grain-boundary electrostatic barriers estimated from density functional calculations and experimental tunnelling barrier heights, which are ≈0.5 eV at low angles and ≈0.15 eV at high angles (≥20°).
Highlights
Grain boundaries in monolayer transition metal dichalcogenides have unique atomic defect structures and band dispersion relations that depend on the inter-domain misorientation angle
On using density functional theory (DFT) to calculate the a-dependent local grain boundaries (GBs) band structures, equilibrium electrostatic GB barriers were found to be correlated with experimentally determined barriers, which gives a clear understanding of the underlying mobility dependences
To suppress interaction with oxygen-related functional groups, further device fabrication was performed in a glove box (H2O, O2o1 p.p.m.) and only acetone solvent was used during the electron-beam lithography procedures to minimize additional GB functionalization
Summary
Grain boundaries in monolayer transition metal dichalcogenides have unique atomic defect structures and band dispersion relations that depend on the inter-domain misorientation angle. The inter-domain mobility is minimized for angles o9° and increases nonlinearly by two orders of magnitude before saturating at B16 cm[2] V À 1 s À 1 around misorientation angleE20° This trend is explained via grain-boundary electrostatic barriers estimated from density functional calculations and experimental tunnelling barrier heights, which are E0.5 eV at low angles and E0.15 eV at high angles (Z20°). Experimental assessment of MoS2 GB transport is still under debate in the literature[6,7,8,9,10,11] due to a large device-to-device performance variation, poor single-domain carrier mobility, and, most importantly, lack of correlation between transport properties and GB atomic structures We overcome these difficulties by directly correlating four-probe transport measurements across single GBs with both high-resolution transmission electron microscopy (TEM) imaging of the measured devices and first-principles calculations. On using DFT to calculate the a-dependent local GB band structures, equilibrium electrostatic GB barriers were found to be correlated with experimentally determined barriers, which gives a clear understanding of the underlying mobility dependences
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