X-ray edge problem of graphene
arXiv:0708.1366 · doi:10.1103/PhysRevB.76.245411
Abstract
The X-ray edge problem of graphene with the Dirac fermion spectrum is studied. At half-filling the linear density of states suppresses the singular response of the Fermi liquid, while away from half-filling the singular features of the Fermi liquid reappear. The crossover behavior as a function of the Fermi energy is examined in detail. The exponent of the power-law absorption rate depends both on the intra- and inter-valley scattering, and it changes as a function of the Fermi energy, which may be tested experimentally.
7 pages, 1 figure
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Cited by in corpus (7)
- Dynamics of Fractionalization in Quantum Spin Liquids
- Topologically ordered zigzag nanoribbon: fractional edge charge, spin-charge separation, and ground state degeneracy
- Soliton fractional charge of disordered graphene nanoribbon
- Photoabsorption spectra and the X-ray edge problem in graphene
- X-ray edge singularity of bilayer graphene
- Relaxation regimes of the holographic electrons at charge neutrality after a local quench of chemical potential
- Theoretical study of X-ray absorption of three-dimensional topological insulator