Xufan Li1,Samuel Wyss2,Baichang Li3,Emanuil Yanev3,Yang Liu3,Yongwen Sun4,Zhiying Wang3,Matthew Strasbourg2,Raymond Unocic5,Yang Yang4,James Hone3,Nicholas Borys2,P. James Schuck3,Avetik Harutyunyan1
Honda Research Institute USA Inc.1,Montana State University2,Columbia University3,The Pennsylvania State University4,Oak Ridge National Laboratory5
Xufan Li1,Samuel Wyss2,Baichang Li3,Emanuil Yanev3,Yang Liu3,Yongwen Sun4,Zhiying Wang3,Matthew Strasbourg2,Raymond Unocic5,Yang Yang4,James Hone3,Nicholas Borys2,P. James Schuck3,Avetik Harutyunyan1
Honda Research Institute USA Inc.1,Montana State University2,Columbia University3,The Pennsylvania State University4,Oak Ridge National Laboratory5
Width confinement and effect of edge structure add new freedoms for exploring exotic properties for already rich atomically-thin materials. Unique properties have already been discovered in graphene nanoribbons with width less than 5 nm. However, for transition metal dichalcogenides (TMDs), the effects by width confinement and edge structure have only been predicted in theoretical calculation due to challenges in synthetic methods to obtain nanoribbons with width less than ~30 nm. We develop a synthetic strategy to directly grow TMD nanoribbons with controllable width (down to sub-10 nm) and layers (single or double layer), from the pre-deposited seed nanoparticles. Width-dependent Coulomb blockade oscillation in the electron transfer behavior in the nanoribbons suggests formation of quantum-dot-like electronic states due to width confinement. Furthermore, combination of width confinement with strain engineering through sharp bending generates highly localized states in TMD nanoribbons, which is responsible for high purity, deterministic single photon emissions. The TMD nanoribbons add a new family of materials to the reservoir for future quantum electronics and photonics. <br/><br/><b>References</b><br/>X. Li., et al. <i>ACS Nano</i><b> 14, </b>6570 (2020).<br/>X. Li., et al. <i>Sci. Adv.</i> 7 (50), eabk1892 (2021).