Magnetic renormalons in a scalar self interacting theory
arXiv:1901.06426 · doi:10.1103/PhysRevD.99.096024
Abstract
We present an analysis about the influence of an external magnetic field on renormalons in a self interacting theory . In the weak magnetic field region, using an appropriate expansion for the Schwinger propagator's, we find new renormalons as poles on the real axis of the Borel plane, whose position do not depend on the magnetic field, but where the residues acquire in fact a magnetic dependence. In the strong magnetic limit, working in the lowest Landau level approximation (LLLA), these new poles are not longer present. We compare the magnetic scenario with previous results in the literature concerning thermal effects on renormalons in this theory.
7 pages, 4 figures. Typos and misprints have been corrected. Explicit calculations have also been given, the conclusions remain the same as in the first version. Accepted for publication in Phys. Rev. D
References in corpus (10)
- Inverse magnetic catalysis for the chiral transition induced by thermo-magnetic effects on the coupling constant
- Inverse magnetic catalysis in the linear sigma model with quarks
- The melting of charmonium in a magnetic field from an effective AdS/QCD model
- Charmonium Spectroscopy in Strong Magnetic Fields by QCD Sum Rules: S-Wave Ground States
- QCD sum rules for magnetically induced mixing between and
- Heavy meson spectroscopy under strong magnetic field
- Spectral properties of meson in a magnetic field
- Magnetic field dependence of the neutral pion mass in the linear sigma model with quarks: The strong field case
- A new perspective for the magnetic corrections to - Scattering Lengths in the Linear Sigma Model
- Renormalons beyond the Borel plane