Silicene and germanene
Upon synthesis of graphene, we wondered whether the same atomic structure could be supported by silicon or germanium atoms, which are below carbon in the periodic table. Planar structure of graphene is supported by the pi-bonds, which are strong and effective due to a relatively smaller core of carbon atoms. Calculating phonon dispersions, we have shown that the planar structure of silicene and germanene is unstable but can gain stability upon buckling. Three years later, silicene was synthesized on the Ag(111) surface. This development inspired theoretical studies searching for other 2D materials without a bulk parent material. Silicene quickly became a hot topic, and many groups reported its synthesis on various substrates. However, results seen in the experiments required explanation in three aspects: (i) ARPES measurements taken from the 3×3 silicene structure grown on the Ag(111) surface revealed a linear band as expected, but the Fermi velocity of this band was three times what was expected (ii) when deposition was continued, a √3×√3 silicene structure was formed but it acquired a mysterious 5 % contraction in the lattice constant thereby becoming mismatched with the substrate (iii) when growth continued even further, a multilayer silicene preserving the shrunk √3×√3 lattice constant (not matching any known bulk structure of silicon) appeared. We have made important contributions to these three scientific discussions with our studies. First, we projected the bands of the 3×3 structure onto the unit cell using the band-unfolding technique and showed that the observed linear band is due to hybridization between Ag(111) surface atoms and silicon atoms. Next, we showed that when new silicon atoms are deposited on the formed silicene, a dumbbell structure forms, and, when surface interactions are taken into account, these dumbbells form a 5% shrunken √3×√3 structure, as observed in the experiment. Finally, we showed that a novel layered silicon structure is formed when silicon atoms are continued to be added to the resulting √3×√3 structure. In the meantime, we also investigated the thermoelectric properties of silicene and germanene. We collaborated with experimentalists and provided crucial theoretical insight in a study that reported the first-ever synthesis of germanene on Au(111) surfaces. We continued our collaboration with experimentalists in two recent studies investigating the vibrational properties of pristine and hydrogenated silicene on Ag(111). We have written a book and a chapter summarizing the literature on silicene and other 2D materials.