Optical pump-terahertz probe spectroscopy has been used to investigate ultrafast photo-induced charge carrier transport in epitaxial graphene nanoribbons. The picosecond THz photoconductivity first increases with an increasing pump fluence and then it saturates at high fluences. This behavior is due to an interplay between contributions of the directly photoexcited carriers and the secondary carriers, which are equilibrium conduction band carriers strongly heated by the carrier-carrier scattering process after the photoexcitation. This phenomenon leads to a non-monotonic variation of the carrier mobility and plasmonic resonance frequency as a function of the pump fluence and, at higher fluences, to a balance between a decreasing carrier scattering time and an increasing Drude weight. In addition, a weak carrier localization occurring at low pump fluences is progressively lifted as a result of increasing initial carrier temperature.
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Singh et al. (2024) studied this question.
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