Abstract

We present a detailed study of gaseous Br<sub>2</sub> adsorption and charge transfer on graphene, combining <i>in situ</i> Raman spectroscopy and density functional theory (DFT). When graphene is encapsulated by hexagonal boron nitride (h-BN) layers on both sides, in a h-BN/graphene/h-BN sandwich structure, it is protected from doping by strongly oxidizing Br<sub>2</sub>. Graphene supported on only one side by h-BN shows strong hole doping by adsorbed Br<sub>2</sub>. Using Raman spectroscopy, we determine the graphene charge density as a function of pressure. DFT calculations reveal the variation in charge transfer per adsorbed molecule as a function of coverage. The molecular adsorption isotherm (coverage <i>versus</i> pressure) is obtained by combining Raman spectra with DFT calculations. The Fowler–Guggenheim isotherm fits better than the Langmuir isotherm. The fitting yields the adsorption equilibrium constant (∼0.31 Torr<sup>–1</sup>) and repulsive lateral interaction (∼20 meV) between adsorbed Br<sub>2</sub> molecules. The Br<sub>2</sub> molecule binding energy is ∼0.35 eV. We estimate that at monolayer coverage each Br<sub>2</sub> molecule accepts 0.09 e<sup>–</sup> from single-layer graphene. If graphene is supported on SiO<sub>2</sub> instead of h-BN, a threshold pressure is observed for diffusion of Br<sub>2</sub> along the (somewhat rough) SiO<sub>2</sub>/graphene interface. At high pressure, graphene supported on SiO<sub>2</sub> is doped by adsorbed Br<sub>2</sub> on both sides

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