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    Scalable Functionalization of Optical Fibers Using Atomically Thin Semiconductors
    (Weinheim : Wiley-VCH Verlag, 2020) Ngo G.Q.; George A.; Schock R.T.K.; Tuniz A.; Najafidehaghani E.; Gan Z.; Geib N.C.; Bucher T.; Knopf H.; Saravi S.; Neumann C.; Lühder T.; Schartner E.P.; Warren-Smith S.C.; Ebendorff-Heidepriem H.; Pertsch T.; Schmidt M.A.; Turchanin A.; Eilenberger F.
    Atomically thin transition metal dichalcogenides are highly promising for integrated optoelectronic and photonic systems due to their exciton-driven linear and nonlinear interactions with light. Integrating them into optical fibers yields novel opportunities in optical communication, remote sensing, and all-fiber optoelectronics. However, the scalable and reproducible deposition of high-quality monolayers on optical fibers is a challenge. Here, the chemical vapor deposition of monolayer MoS2 and WS2 crystals on the core of microstructured exposed-core optical fibers and their interaction with the fibers’ guided modes are reported. Two distinct application possibilities of 2D-functionalized waveguides to exemplify their potential are demonstrated. First, the excitonic 2D material photoluminescence is simultaneously excited and collected with the fiber modes, opening a novel route to remote sensing. Then it is shown that third-harmonic generation is modified by the highly localized nonlinear polarization of the monolayers, yielding a new avenue to tailor nonlinear optical processes in fibers. It is anticipated that the results may lead to significant advances in optical-fiber-based technologies. © 2020 The Authors. Published by Wiley-VCH GmbH
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    Terahertz radiative coupling and damping in multilayer graphene
    (Bristol : IOP, 2014) Bowlan, P.; Martinez-Moreno, E.; Reimann, K.; Woerner, M.; Elsaesser, T.
    The nonlinear interaction between intense terahertz (THz) pulses and epitaxial multilayer graphene is studied by field-resolved THz pump-probe spectroscopy. THz excitation results in a transient induced absorption with decay times of a few picoseconds, much faster than carrier recombination in single graphene layers. The decay times increase with decreasing temperature and increasing amplitude of the excitation. This behaviour originates from the predominant coupling of electrons to the electromagnetic field via the very strong interband dipole moment while scattering processes with phonons and impurities play a minor role. The nonlinear response at field amplitudes above 1 kV cm-1 is in the carrier-wave Rabi flopping regime with a pronounced coupling of the graphene layers via the radiation field. Theoretical calculations account for the experimental results.