Polarization field in a single-valley strongly-interacting 2D electron system

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.

References in corpus (8)

• Metal-insulator transition in two-dimensional electron systems
• Transport in strongly correlated two dimensional electron fluids
• Theoretical Studies of Superconductor-Insulator Transitions
• Quantum Critical Transport Near the Mott Transition
• Localized - delocalized electron quantum phase transitions
• Effective mass suppression in dilute, spin-polarized two-dimensional electron systems
• Self-doping instability of the Wigner-Mott insulator
• Contrast between spin and valley degrees of freedom

Cited by in corpus (2)

• The effective electron mass in high-mobility SiGe/Si/SiGe quantum wells
• Two dimensional electrons in (100) oriented silicon field effect structures in the region of low concentrations and high mobilities