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- W2068235640 abstract "We report the energy-momentum dispersion $ensuremath{omega}$($mathcal{q}$) of a low-energy intraband $ensuremath{pi}$ plasmon arising from Dirac fermions in the conduction band of a single-layer graphene (SLG), not complicated by couplings with other excitations. For a wide range of $mathcal{q}$ (0.39 $ensuremath{leqslant}mathcal{q}/{k}_{F}ensuremath{leqslant}$ 2.36), where ${k}_{F}$ $=$ 0.061 $AA{}{}^{ensuremath{-}1}$ is the Fermi wave vector, the intraband plasmon survives through the interband single-particle excitation (SPE) region, and linearly disperses beyond the Landau damping ${q}_{c}$ $=$ 0.90 ${k}_{F}$ asymptotically approaching the boundary of the interband SPE without ever entering the intraband SPE. Such a unique feature is completely distinct from the plasmon of either a multilayer graphene or a normal two-dimensional electron gas, and hence demonstrates another intrinsic nature of Dirac fermions in SLG." @default.
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- W2068235640 date "2011-04-18" @default.
- W2068235640 modified "2023-10-06" @default.
- W2068235640 title "Observation of intrinsic intraband<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mi>π</mml:mi></mml:mrow></mml:math>-plasmon excitation of a single-layer graphene" @default.
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- W2068235640 doi "https://doi.org/10.1103/physrevb.83.161403" @default.
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