Magnetization of a strongly interacting two-dimensional electron system in perpendicular magnetic fields
arXiv:cond-mat/0503123 · doi:10.1103/PhysRevLett.96.046409
Abstract
We measure the thermodynamic magnetization of a low-disordered, strongly correlated two-dimensional electron system in silicon in perpendicular magnetic fields. A new, parameter-free method is used to directly determine the spectrum characteristics (Lande g-factor and the cyclotron mass) when the Fermi level lies outside the spectral gaps and the inter-level interactions between quasiparticles are avoided. Intra-level interactions are found to strongly modify the magnetization, without affecting the determined g* and m*.
As published
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Cited by in corpus (18)
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- Recent developments in the field of the metal-insulator transition in two dimensions
- Strongly enhanced effective mass in dilute two-dimensional electron systems: System-independent origin
- Magnetization in two-dimensional electron gas in a perpendicular magnetic field: the roles of edge states and spin-orbit coupling
- Metal-insulator transition and low-density phases in a strongly-interacting two-dimensional electron system
- Branch-cut Singularities in Thermodynamics of Fermi Liquid Systems
- Alternative method for the quantitative determination of Rashba- and Dresselhaus spin-orbit interaction using the magnetization
- Two-dimensional system of strongly interacting electrons in silicon (100) structures
- A metal-insulator transition in 2D: Established facts and open questions
- Conductivity of a spin-polarized two-dimensional electron liquid in the ballistic regime
- Manifestation of strong correlations in transport in ultra-clean SiGe/Si/SiGe quantum wells
- Spin independence of the strongly enhanced effective mass in ultra-clean SiGe/Si/SiGe two-dimensional electron system
- Measurements of the magnetic properties of conduction electrons
- Spin susceptibility and polarization field in a dilute two-dimensional electron system in (111) silicon
- Microwave response of interacting oxide two-dimensional electron systems
- Shear Bernstein modes in a two-dimensional electron liquid
- Magnetic instability and spin-glass order beyond the Anderson-Mott transition in interacting power-law random banded matrix fermions