Nuclear magnetic resonance line shapes of Wigner crystals in C-enriched graphene
arXiv:1705.08311 · doi:10.1103/PhysRevB.95.235411
Abstract
Assuming that the nuclear magnetic resonance (NMR) signal from a C isotope enriched layer of graphene can be made sufficiently intense to be measured, we compute the NMR\ lineshape of the different crystals ground states that are expected to occur in graphene in a strong magnetic field. We first show that in nonuniform states, there is, in addition to the frequency shift due to the spin hyperfine interaction, a second contribution of equal importance from the coupling between the orbital motion of the electrons and the nuclei. We then show that, if the linewidth of the bare signal can be made sufficiently small, the Wigner and bubble crystals have line shapes that differ qualitatively from that of the uniform state at the same density while crystal states that have spin or valley pseudospin textures do not. Finally, we find that a relatively small value of the bare linewidth is sufficient to wash out the distinctive signature of the crystal states in the NMR line shape.
12 pages with 6 eps figures
References in corpus (9)
- The electronic properties of graphene
- Tuning the effective fine structure constant in graphene: opposing effects of dielectric screening on short- and long-range potential scattering
- Hyperfine Interactions in Graphene and Related Carbon Nanostructures
- Melting of a 2D Quantum Electron Solid in High Magnetic Field
- NMR profiling of quantum electron solids in high magnetic fields
- Wigner crystal and bubble phases in graphene in the quantum Hall regime
- Skyrme and Wigner crystals in graphene
- Unusual hyperfine interaction of Dirac electrons and NMR spectroscopy in graphene
- Quantum Hall ferromagnetism in graphene: a SU(4) bosonization approach