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.
Citation:
V. T. Dolgopolov, A. A. Shashkin, “Polarization field in a single-valley strongly-interacting 2D electron system”, Pis'ma v Zh. Èksper. Teoret. Fiz., 95:11 (2012), 648–652; JETP Letters, 95:11 (2012), 570–574