Novel exciton systems in 2D TMD monolayers and heterobilayers

COFFEE_KLATCH · Invited

Abstract

In this talk, two exciton systems in transition metal dichalcogenides (TMDs) monolayer and heterobilayer will be discussed. In TMD monolayers, the strong e-h Coulomb exchange interaction splits the exciton and trion dispersions into two branches with zero and finite gap, respectively \footnote{H. Yu, G.-B. Liu, P. Gong, X. Xu, and W. Yao, Nat. Commun. \textbf{5}, 3876 (2014).} \footnote{H. Yu, X. Cui, X. Xu, and W. Yao, Natl Sci Rev \textbf{2}, 57 (2015).}. Each branch is a center-of-mass wave vector dependent coherent superposition of the two valleys, which leads to a valley-orbit coupling and possibly a trion valley Hall effect. The exchange interaction also eliminates the linear polarization of the negative trion PL emission \footnote{A. Jones, H. Yu, N. Ghimire, S. Wu, G. Aivazian, J. Ross, B. Zhao, J. Yan, D. Mandrus, D. Xiao, W. Yao, and X. Xu, Nature Nanotech. \textbf{8}, 634 (2013).}. In TMD heterobilayers with a type-II band alignment, the low energy exciton has an interlayer configuration with the e and h localized in opposite layers. Because of the inevitable twist or/and lattice mismatch between the two layers, the bright interlayer excitons are located at finite center-of-mass velocities with a six-fold degeneracy \footnote{H. Yu, Y. Wang, Q. Tong, X. Xu, and W. Yao, Phys. Rev. Lett. \textbf{115}, 187002 (2015).}. The corresponding photon emission is elliptically polarized, with the major axis locked to the direction of exciton velocity, and helicity determined by the valley indices of the e and h. Some experimental results on the interlayer excitons in the WSe$_2$-MoSe$_2$ heterobilayers will also be presented. The interlayer exciton exhibits a long lifetime as well as a long depolarization time, which facilitate the observation of a PL polarization ring pattern due to the valley dependent exciton-exciton interaction induced expansion \footnote{P. Rivera, K. L. Seyler, H. Yu, J. R. Schaibley, J. Yan, D. G. Mandrus, W. Yao, and X. Xu, to be published.}.

Authors

  • Hongyi Yu

    University of Hong Kong, Department of Physics and Center of Theoretical and Computational Physics, The University of Hong Kong, The Univ of Hong Kong