Acoustic phonons and spin relaxation in graphene nanoribbons
arXiv:1104.3520 · doi:10.1103/PhysRevB.84.155404
Abstract
Phonons are responsible for limiting both the electron mobility and the spin relaxation time in solids and provide a mechanism for thermal transport. In view of a possible transistor function as well as spintronics applications in graphene nanoribbons, we present a theoretical study of acoustic phonons in these nanostructures. Using a two-dimensional continuum model which takes into account the monatomic thickness of graphene, we derive Hermitian wave equations and infer phonon creation and annihilation operators. We elaborate on two types of boundary configuration, which we believe can be realized in experiment: (i) fixed and (ii) free boundaries. The former leads to a gapped phonon dispersion relation, which is beneficial for high electron mobilites and long spin lifetimes. The latter exhibits an ungapped dispersion and a finite sound velocity of out-of-plane modes at the center of the Brillouin zone. In the limit of negligible boundary effects, bulk-like behavior is restored. We also discuss the deformation potential, which in some cases gives the dominant contribution to the spin relaxation rate T_1^{-1}.
7 pages, 4 figures
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Cited by in corpus (9)
- Phonon Transport in Graphene
- Determination of the spin-lifetime anisotropy in graphene using oblique spin precession
- Ab initio spin-flip conductance of hydrogenated graphene nanoribbons: Spin-orbit interaction and scattering with local impurity spins
- Spintronics with graphene quantum dots
- Electron Spin Relaxation in Graphene Nanoribbon Quantum Dots
- The role of atomic vacancies and boundary conditions on ballistic thermal transport in graphene nanoribbons
- Ultra long spin decoherence times in graphene quantum dots with a small number of nuclear spins
- Tuning the polarized quantum phonon transmission in graphene nanoribbons
- Bending mode fluctuations and structural stability of graphene nanoribbons