The fast carrier relaxation time, high carrier mobility and electrostatic tunability make graphene a prospective ideal material for electronics and optoelectronics. However, its low optical absorption is a big obstacle. Moreover, for using graphene in the large area optoelectronic devices, any scheme for enhancing the light-matter interaction in graphene should be polarization and incident angle-independent.
Here, we demonstrate a novel design of an optical cavity-coupled hexagonal nanohole and nanodisk array to excite Dirac plasmon. We compare the Dirac plasmon lifetimes of the graphene nanohole and nanodisk arrays and their role in the enhanced light-matter interaction. Coupling the patterned graphene to an optical cavity creates a temporal and spatial overlap between the graphene plasmon and cavity modes. This complex geometry gives rise to an unprecedented polarization independent light absorption of 60% on nanohole and 90% on nanodisk arrays in low carrier mobility CVD-grown monolayer graphene in the 8-12 um atmospheric transparent infrared imaging band. Electrostatically doping of the patterned graphene tune the surface plasmon resonance wavelength up to 2.5 um by applying a small gate voltage (4V). We show theoretically, and also for the first time the experimental results of the enhanced light absorption for the non-normal incidence. While the light absorption up to 40° (incident angle) is almost constant, the trend of the angular optical response for s- and p-polarized light are different which is validated by our analytical coupled-dipole approximation modeling. This electronically tunable wide angle extraordinary light absorption paves the path towards new generation of graphene-based optoelectronics devices.
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