High density limit of the two-dimensional electron liquid with Rashba spin-orbit coupling
arXiv:1008.3729 · doi:10.1103/PhysRevB.83.235309
Abstract
We discuss by analytic means the theory of the high-density limit of the unpolarized two-dimensional electron liquid in the presence of Rashba or Dresselhaus spin-orbit coupling. A generalization of the ring-diagram expansion is performed. We find that in this regime the spin-orbit coupling leads to small changes of the exchange and correlation energy contributions, while modifying also, via repopulation of the momentum states, the noninteracting energy. As a result, the leading corrections to the chirality and total energy of the system stem from the Hartree-Fock contributions. The final results are found to be vanishing to lowest order in the spin-orbit coupling, in agreement with a general property valid to every order in the electron-electron interaction. We also show that recent quantum Monte Carlo data in the presence of Rashba spin-orbit coupling are well understood by neglecting corrections to the exchange-correlation energy, even at low density values.
11 pages, 5 figures
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Cited by in corpus (12)
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- A generalized Stoner criterion and versatile spin ordering in two-dimensional spin-orbit coupled electron systems
- Polarization of a quasi two-dimensional repulsive Fermi gas with Rashba spin-orbit coupling: a variational study
- Signatures of an annular Fermi sea
- Suppression of Coulomb exchange energy in quasi-two-dimensional hole systems
- Coupled spin-charge dynamics in helical Fermi liquids beyond the random phase approximation
- Quasiparticle velocities in 2D electron/hole liquids with spin-orbit coupling
- Phase diagram of the interacting persistent spin-helix state
- Spectrum of a family of spin-orbit coupled Hamiltonians with singular perturbation
- Coulomb-exchange effects in nanowires with spin splitting due to a radial electric field