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    Opposite behavior of ultrafast dynamics of exciton shift and linewidth broadening in bilayer ReS2

    Sangwan Sim1,*, Ho-Seung Shin2,*, Doeon Lee3, Jekwan Lee4, Myungjun Cha4, Kyusang Lee3,5, and Hyunyong Choi4,†

    • 1Division of Electrical Engineering, Hanyang University, Ansan 15588, Korea
    • 2School of Electrical and Electronic Engineering, Yonsei University, Seoul 03722, Korea
    • 3Department of Electrical and Computer Engineering, University of Virginia, Charlottesville, Virginia 22903, USA
    • 4Department of Physics and Astronomy, Institute of Applied Physics, Seoul National University, Seoul 08826, Korea
    • 5Departments of Materials Science and Engineering, University of Virginia, Charlottesville, Virginia 22903, USA

    • *These authors contributed equally to this work.
    • †Corresponding author: hy.choi@snu.ac.kr

    Phys. Rev. B 103, 014309 – Published 21 January, 2021

    DOI: https://doi.org/10.1103/PhysRevB.103.014309

    Abstract

    The optical and optoelectronic properties of two-dimensional (2D) semiconductors are dominated by excitons, which usually appear as well-defined peaks in the spectral domain. Thus, detailed behaviors of excitons can be understood by tracking transient changes of the fundamental spectral observables, i.e., the resonance energy and the spectral linewidth. Rhenium disulfide (ReS2) is a 2D semiconductor that has recently attracted attention due to its excellent exciton properties, such as light-polarization selectivity and anisotropic coherent effects. However, an understanding of exciton dynamics and spectral behavior of excitons in ReS2 is lacking. Here, we used time- and spectrally resolved pump-probe spectroscopy to investigate ultrafast exciton dynamics in bilayer ReS2. Upon photoexcitation, the exciton resonance undergoes linewidth broadening and redshift, but they exhibit different dynamics, and an opposite pump fluence dependence on the approximately hundreds of picoseconds timescale. This is because the spectral broadening and the red-shift both have different origins (the exciton-carrier scattering and exciton-exciton attractive interaction, respectively) and different decay mechanisms (the trapping of carriers and exciton-exciton annihilation, respectively). On a longer timescale of ∼100 ps, both the spectral broadening and the redshift are well explained by the indirect recombination of carriers and lattice heating. This work provides in-depth insight into exciton dynamics in 2D rhenium dichalcogenides.

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