Spin transition in the fractional quantum Hall regime: Effect of extent of the wave function
arXiv:1210.0387 · doi:10.1103/PhysRevB.87.081306
Abstract
Using a magnetocapacitance technique, we determine the magnetic field of the spin transition, B*, at filling factor nu=2/3 in the 2D electron system in GaAs/AlGaAs heterojunctions. The field B* is found to decrease appreciably as the wave function extent controlled by back gate voltage is increased. Our calculations show that the contributions to the shift of B* from the change of the Coulomb energy and the g factor change due to nonparabolicity are approximately the same. The observed relative shift of B* is described with no fitting parameters.
as published
References in corpus (6)
- Measurements of the density-dependent many-body electron mass in 2D GaAs/AlGaAs Heterostructures
- Spinful Composite Fermions in a Negative Effective Field
- Direct measurements of the fractional quantum Hall effect gaps
- Spin-texture and magneto-roton excitations at nu=1/3
- Absorption in the fractional quantum Hall regime: trion dichroism and spin polarization
- Filling factor dependence of the fractional quantum Hall effect gap
Cited by in corpus (4)
- Spin-Polarization of Composite Fermions and Particle-Hole Symmetry Breaking
- Half-integer conductance plateau at the fractional quantum Hall state in a quantum point contact
- Determination of the Fermi Contour and Spin-polarization of Composite Fermions via Ballistic Commensurability Measurements
- Topological Protection in a Landau Flat Band at , a Candidate Filling Factor for Unconventional Correlations