- Open Access
Fast two-dimensional long-wavelength plasmons in atomically thin
Phys. Rev. Research 8, 023072 – Published 24 April, 2026
DOI: https://doi.org/10.1103/hr7f-kgdg
Abstract
Plasmons are bosonic wavelike charge oscillations in solids and the plasmon group velocity (), the first derivative of momentum ()-dependent dispersions, depicts the many-body electron motions of critical electronic importance. The profound characteristics of in either three-dimensional (3D) or two-dimensional (2D) electron systems are nonetheless short of quantitative scrutiny. Using -resolved electron energy loss spectroscopy, we tackle the -dependent of π and π + σ plasmons in 3D-bulk and 2D-monolayer (ML) semiconductors, with the 2D being the model transition-metal dichalcogenide (TMD) for emergent atomically thin electronics. along with the underlining electronic parameters of the charge density, effective mass, and screening length in 2D for the plasmon dispersions is quantitatively elaborated. 2D is further compared to those evaluated from metallic ML-TMD and graphene, and the scaling over the single-particle Fermi velocity () unveils a function generally obeyed by the semiconducting and metallic TMD and graphene of distinctly different massive and relativistic characters, respectively. Beyond the pertinent critical (on the order of ) where one observes , electric-field lines connecting the oscillating 2D charges would turn from vacuum into the atomically thin matters, concomitant with the increasing plasmon damping and reducing (). Long-wavelength 2D plasmons below the critical characterize the field lines largely in vacuum and are persistent and fast (), with high-speed application merits. Conversely, 3D plasmons in bulk never exceed .
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