Employing gate voltage tunable and geometry dependent plasmon resonances of graphene ribbons, we engineer dual graphene optical gratings that can be used to simultaneously achieve orders-of-magnitude enhancement of both the SHG and THG intensities.OCIS codes : 190.0190, 160.3918, 240.6680
IntroductionBecause of large optical field enhancements achievable in graphene via excitation of surface plasmons, this truly twodimensional (2D) physical system [1] provides a promising material platform for enhancing nonlinear optical interactions at the nanoscale [2][3][4]. In this paper, we demonstrate that by matching plasmon resonances in mutually interacting graphene gratings separated by a thin dielectric spacer, the second-harmonic (SH) and third-harmonic (TH) can be simultaneously enhanced by more than eight orders of magnitude as compared to that in a graphene sheet. Choosing which nonlinear optical effect is enhanced can be conveniently done by gate voltage tuning. To be more specific, employing the dependence of the resonance wavelength of localized plasmons of graphene ribbons on their width, we design a graphene bilayer grating in such a way that the resonance wavelength of the first-order localized plasmons in one grating is equal to half (for SH) and a third (for TH) of that of the first-order localized plasmons in an adjacent grating that is optically coupled to the first one. This finding is particularly relevant in the context of technological applications, as graphene plays an increasingly important role in optoelectronics, chiefly due to the remarkable tunability of its optical properties via chemical doping or electric gating. In addition, graphene structures support localized and propagating surface plasmons, whose excitation is accompanied by a significant enhancement of the optical near-field. This unique potential to control at deep-subwavelength the optical field has open up a broad array of technological applications, including optical modulation, sensing, and ultrafast active photonic devices [5,6].