石墨烯
高次谐波产生
等离子体子
谐波
超短脉冲
光电子学
太赫兹辐射
二次谐波产生
物理
非谐性
非线性光学
电子
电磁场
材料科学
纳米技术
光学
激光器
凝聚态物理
量子力学
电压
作者
Joel D. Cox,Andrea Marini,F. Javier Garcı́a de Abajo
摘要
Abstract High-harmonic generation in condensed-matter systems is both a source of fundamental insight into quantum electron motion and a promising candidate to realize compact ultraviolet and ultrafast light sources. While graphene is anticipated to efficiently generate high-order harmonics due to its anharmonic charge-carrier dispersion, experiments performed on extended samples using THz illumination have revealed only a weak effect. The situation is further complicated by the enormous electromagnetic field intensities required by this highly nonperturbative nonlinear optical phenomenon. Here we argue that the large light intensity required for high-harmonic generation to occur can be reached by exploiting localized plasmons in doped graphene nanostructures. We demonstrate through rigorous time-domain simulations that the synergistic combination of strong plasmonic near-field enhancement and a pronounced intrinsic nonlinearity result in efficient broadband high-harmonic generation within a single material. Our results support the strong potential of nanostructured graphene as a robust, electrically tunable platform for high-harmonic generation.
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