816
Phonon and Defect Induced Transparencies in the Mid-Infrared Spectrum of Grafted Single Layer Graphene

Thursday, 1 June 2017: 08:40
Churchill A1 (Hilton New Orleans Riverside)
F. Lapointe (Université de Montréal, National Research Council Canada), B. Rousseau, M. Nguyen, V. Aymong (Université de Montréal, Regroupement Québécois sur les Matériaux de Pointe), M. Biron (École Polytechnique de Montréal, Regroupement Québécois sur les Matériaux de Pointe), É. Gaufrès (Université de Montréal, Regroupement Québécois sur les Matériaux de Pointe), P. Desjardins (École Polytechnique de Montréal, Regroupement Québécois sur les Matériaux de Pointe), M. Côté, and R. Martel (Université de Montréal, Regroupement Québécois sur les Matériaux de Pointe)
The Drude-like response of graphene in the terahertz and infrared region of the spectrum has made it attractive for optoelectronic applications in this range, because the response can be controlled by gating and doping. [1] Graphene infrared response can further be tailored for photonics and plasmonics, as the patterned material harbors low energy plasmon modes. [2] However, the infrared spectrum of pristine single layer graphene (SLG) is monotonous; in contrast to Raman, there are no infrared-active phonon modes, while bilayer graphene displays a Fano resonance in the infrared at ~1600 cm-1. [3]

In a first time, we show experimentally that grafting SLG with halogenophenyl moieties induces optical transparencies at two specific energies: 1250 and 1600 cm-1 [4], in close similarity to the bands that can also be observed in carbon nanotubes as Fano resonances. [5] Unlike bands caused by the absorption of light by vibrational modes, these antiresonances show a decrease of the absorbance, an optical transparency effect. Moreover, we show that the amplitude of the transparencies can be modulated by changing the charge carrier density through doping, and by the defect density through controlled grafting.  

In as second time, we will present a theory based on quantum mechanics to calculate the optical conductivity of grafted SLG. [4] The model puts into play phonon modes with momenta different from Γ that can be addressed through scattering on defects. Numerical simulations reproduce the experimental data with good agreement. The theory also captures the dependence of the signal on charge carrier density and defect density.  

Our findings bring a new understanding for the physics behind the infrared activity of nanostructures, while opening new capabilities for tailoring the optical spectrum of nanomaterials.

References

[1] Horng et al. (2011) Phys Rev B 83:165113

[2] Low & Avouris (2014) ACS Nano 8:1086

[3] Kuzmenko et al. (2009) Phys Rev Lett 103:116804

[4] Rousseau et al. (2014) arXiv preprint arxiv:1407.8141

[5] Lapointe et al. (2012) Phys Rev Lett 109:097402