AVS 60th International Symposium and Exhibition | |
Graphene and Other 2D Materials Focus Topic | Thursday Sessions |
Session GR+EM+NS+SS+TF-ThA |
Session: | Beyond Graphene: Other 2D Electronic Materials and their Heterostructures |
Presenter: | T.F. Heinz, Columbia University |
Correspondent: | Click to Email |
Inspired by the fascinating properties and application potential of graphene, interest within the community has extended to a broader class of stable, atomically thin materials. In this paper, we will discuss recent advances in the study of atomically thin layers of MoS2 as representatives of the class transition metal dichalcogenides. Although the structure of the monolayer of MoS2 is similar to that of graphene, the A and B sublattice are occupied either by Mo atoms or by a pair of S atoms, rather than just by C atoms. This difference in symmetry allows MoS2 to be a semiconductor with a significant band gap. Through characterization of the optical properties of the material as a function of thickness, we show that quantum confinement effects lead to a crossover in MoS2 from an indirect gap semiconductor in the bulk to a direct gap semiconductor at monolayer thickness.
As expected for lower-dimensional materials, excitonic effects are very strong in monolayer MoS2. This allows for the existence of charged exciton with binding energies sufficient to produce stable states even at room temperature. Another distinctive feature of this material is the possibility of creating long-lived valley polarization in which one of the two inequivalent, but energetically degenerate K and K’ valleys is populated in preference to the other. We demonstrate how this can be achieved using optical excitation with circularly polarized radiation and monitored through the retention of the polarization in fluorescence emission. The pronounced change in symmetry from the non-centrosymmetric monolayer to the centrosymmetric bilayer has also been examined through its influence on the production of valley polarization and of optical second-harmonic radiation.