Publication | Open Access
Plasmon properties and hybridization effects in silicene
40
Citations
96
References
2017
Year
EngineeringChemistryMonolayer SiliceneSemiconductor NanostructuresOptical PropertiesQuantum MaterialsSiliceneCharge Carrier TransportNanophotonicsPlasmonic MaterialQuantum SciencePlasmon PropertiesPhysicsQuantum ChemistryPlasmonic CharacterPlasmonicsMonolayer GrapheneNatural SciencesApplied PhysicsCondensed Matter PhysicsTopological Heterostructures
The plasmonic character of monolayer silicene is investigated by time-dependent density functional theory in the random phase approximation. Both the intrinsic (undoped) and several extrinsic (carrier doped or gated) conditions are explored by simulating injection of a probe particle (i.e., an electron or a photon) of energy below 20 eV and in-plane momentum smaller than $1.1\phantom{\rule{0.16em}{0ex}}\AA{}{}^{\ensuremath{-}1}$. The energy-loss function of the system is analyzed, with particular reference to its induced charge-density fluctuations, i.e., plasmon resonances and corresponding dispersions, occurring in the investigated energy-momentum region. At energies larger than 1.5 eV, two intrinsic interband modes are detected and characterized. The first one is a hybridized $\ensuremath{\pi}$-like plasmon, which is assisted by competing one-electron processes involving $s{p}^{2}$ and $s{p}^{3}$ states, and depends on the slightest changes in specific geometric parameters, such as nearest-neighbor atomic distance and buckling constant. The second one is a more conventional $\ensuremath{\pi}\ensuremath{-}\ensuremath{\sigma}$ plasmon, which is more intense than the $\ensuremath{\pi}$-like plasmon and more affected by one-electron processes involving the $\ensuremath{\sigma}$ bands with respect to the analogous collective oscillation in monolayer graphene. At energies below 1 eV, two extrinsic intraband modes are predicted to occur, which are generated by distinct types of Dirac electrons (associated with different Fermi velocities at the so-called Dirac points). The most intense of them is a two-dimensional plasmon, having an energy-momentum dispersion that resembles that of a two-dimensional electron gas. The other is an acoustic plasmon that occurs for specific momentum directions and competes with the two-dimensional plasmon at mid-infrared energies. The strong anisotropic character of this mode cannot be explained in terms of the widely used Dirac-cone approximation. As in mono-, bi-, and few-layer graphene, the extrinsic oscillations of silicene are highly sensitive to the concentration of injected or ejected charge carriers. More importantly, the two-dimensional and acoustic plasmons appear to be a signature of the honeycomb lattice, independently of the chemistry of the group-IV elements and the details of the unit-cell geometry.
| Year | Citations | |
|---|---|---|
Page 1
Page 1