Beschreibung:
<jats:p> 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<jats:sup>-1</jats:sup>. [3]</jats:p>
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<jats:p>In a first time, we show experimentally that grafting SLG with halogenophenyl moieties induces optical transparencies at two specific energies: 1250 and 1600 cm<jats:sup>-1</jats:sup> [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 <jats:italic>decrease </jats:italic>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. </jats:p>
<jats:p>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. </jats:p>
<jats:p>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.</jats:p>
<jats:p>References</jats:p>
<jats:p>[1] Horng <jats:italic>et al.</jats:italic> (2011) <jats:italic>Phys Rev B</jats:italic> 83:165113 </jats:p>
<jats:p>[2] Low & Avouris (2014) <jats:italic>ACS Nano </jats:italic>8:1086 </jats:p>
<jats:p>[3] Kuzmenko <jats:italic>et al.</jats:italic> (2009) <jats:italic>Phys Rev Lett</jats:italic> 103:116804 </jats:p>
<jats:p>[4] Rousseau <jats:italic>et al.</jats:italic> (2014)<jats:italic> arXiv preprint </jats:italic>arxiv:1407.8141 </jats:p>
<jats:p>[5] Lapointe <jats:italic>et al</jats:italic>. (2012) <jats:italic>Phys Rev Lett</jats:italic> 109:097402 </jats:p>
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