Polarization field in a single-valley strongly-interacting 2D electron system
arXiv:1206.2799 · doi:10.1134/S0021364012110021
Abstract
The magnetic field of complete spin polarization is calculated in a disorderless single-valley strongly-interacting 2D electron system. In the metallic region above the Wigner-Mott transition, non-equilibrium spin states are predicted, which should give rise to hysteresis in the magnetization.