Electron mass operator in a strong magnetic field
arXiv:hep-ph/0204168 · doi:10.1142/S0217732302006321
Abstract
The electron mass operator in a strong magnetic field is calculated by summation of the leading log contributions in all orders of the perturbation theory. An influence of the strong field on the virtual photon polarization operator is taken into account. The contribution of higher Landau levels of virtual electrons, along with the ground Landau level, is shown to be essential in the leading log approximation.
7 pages, LATEX, 1 PS figure, submitted to Modern Physics Letters A
References in corpus (1)
Cited by in corpus (15)
- Quark matter under strong magnetic fields in the su(3) Nambu-Jona-Lasinio Model
- Modified Coulomb Law in a Strongly Magnetized Vacuum
- Electric field of a pointlike charge in a strong magnetic field and ground state of a hydrogenlike atom
- Modification of Coulomb law and energy levels of the hydrogen atom in a superstrong magnetic field
- Positronium collapse and the maximum magnetic field in pure QED
- Bethe-Salpeter approach for relativistic positronium in a strong magnetic field
- Is the photon paramagnetic?
- Atomic levels in superstrong magnetic fields and D=2 QED of massive electrons: screening
- Electron Mass Operator in a Strong Magnetic Field and Dynamical Chiral Symmetry Breaking
- Photon Magnetic Moment and Vacuum Magnetization in an Asymptotically Large Magnetic Field
- Dynamical Electron Mass in a Strong Magnetic Field
- The 1-loop self-energy of an electron in a strong external magnetic field revisited
- Fermion mass and width in QED in a magnetic field
- Magnetic Field Effect in the Fine-Structure Constant and Electron Dynamical Mass
- Reply to Comment on ``Electron Mass Operator in a Strong Magnetic Field and Dynamical Chiral Symmetry Breaking''