Statistical repulsion/attraction of electrons in graphene in a magnetic field
arXiv:1310.7154 · doi:10.1016/j.physb.2013.10.004
Abstract
The aim of this work is to describe the thermodynamic properties of an electron gas in graphene placed in a constant magnetic field. The electron gas is constituted by Bloch electrons in the long wavelength approximation. The partition function is analyzed in terms of a perturbation expansion of the dimensionless constant . The statistical repulsion/attraction potential for electrons in graphene is obtained in the respective case in which antisymmetric/symmetric states in the coordinates are chosen. Thermodynamic functions are computed for different orders in the perturbation expansion and the different contributions are compared for symmetric and antisymmetric states, showing remarkable differences between them due to the spin exchange correlation. A detailed analysis of the statistical potential is done, showing that, although electrons satisfy Fermi statistics, attractive potential at some interparticle distances can be found.
Physica B, 2013
References in corpus (8)
- The electronic properties of graphene
- Quantum Hall Ferromagnetism in Graphene
- Electron interactions in graphene in a strong magnetic field
- Quantum transport of Dirac electrons in graphene in the presence of a spatially modulated magnetic field
- Dynamical polarization of monolayer graphene in a magnetic field
- Traits and Characteristics of Interacting Dirac fermions in Monolayer and Bilayer Graphene
- Band Collapse and the Quantum Hall Effect in Graphene
- Green functions of electrons in monolayer and bilayer graphene in a magnetic field
Cited by in corpus (5)
- Ground state magnetization of conduction electrons in graphene with Zeeman effect
- Valley properties of doped graphene in a magnetic field
- Magnetization in pristine graphene with Zeeman splitting and variable spin-orbit coupling
- Influence of temperature on the magnetic oscillations in graphene with spin splitting: a new approach
- Temperature effect on the magnetic oscillations in 2D materials