Effective Fermion Mass in Relativistic and Non-Relativistic Systems
arXiv:2106.08300 · doi:10.1088/1367-2630/ac0203
Abstract
Electrons interact strongly with their environment. The result of these interactions is, most of the time, encoded in an effective mass. In non-relativistic systems, as in condensed matter, the electrons plus interactions form a quasiparticle with an effective mass. From the side of relativistic systems, the fermions also acquire an effective mass due to the interactions with the surrounding medium. We employ a non-perturbative method to calculate the effective mass of relativistic and non-relativistic fermions, in various situations. We find the effective masses up to second order of the iteration method. The results can be of interest in current studies on fermion systems.
arXiv comment12 pages, 3 figures
References in corpus (17)
- Two-Dimensional Gas of Massless Dirac Fermions in Graphene
- Experimental Observation of Quantum Hall Effect and Berry's Phase in Graphene
- Electron-Electron Interactions in Graphene: Current Status and Perspectives
- New Measurement of the Electron Magnetic Moment and the Fine Structure Constant
- Dirac cones reshaped by interaction effects in suspended graphene
- High-precision measurement of the atomic mass of the electron
- Repulsive Fermi polarons in a resonant mixture of ultracold Li atoms
- A QCD Analysis of the Mass Structure of the Nucleon
- Proton Mass Decomposition from the QCD Energy Momentum Tensor
- Effective field theory, three-loop perturbative expansion, and their experimental implications in graphene many-body effects
- The Chiral Fermion Meson Model at Finite Temperature
- Meson Mass Decomposition from Lattice QCD
- Effective mass of quasiparticles from thermodynamics
- Quasiparticle Effective Mass for the Two- and Three-Dimensional Electron Gas
- Repulsive Fermi polarons with negative effective mass
- Symmetry Nonrestoration in a Resummed Renormalized Theory at High Temperature
- Non-perturbative corrections to the quasiparticle velocity in graphene