Finite temperature quark-gluon vertex with a magnetic field in the Hard Thermal Loop approximation
arXiv:1410.6388 · doi:10.1103/PhysRevD.91.016007
Abstract
We compute the thermo-magnetic correction to the quark-gluon vertex in the presence of a weak magnetic field within the Hard Thermal Loop approximation. The vertex satisfies a QED-like Ward identity with the quark self-energy. The only vertex components that get modified are the longitudinal ones. The calculation provides a first principles result for the quark anomalous magnetic moment at high temperature in a weak magnetic field. We extract the effective thermo-magnetic quark-gluon coupling and show that this decreases as a function of the field strength. The result supports the idea that the properties of the effective quark-gluon coupling in the presence of a magnetic field are an important ingredient to understand the inverse magnetic catalysis phenomenon.
9 pages, 4 figures
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- One-loop QCD thermodynamics in a strong homogeneous and static magnetic field
- Magnetic field dependence of the neutral pion mass in the linear sigma model with quarks: The strong field case
- Strong magnetic fields in nonlocal chiral quark models
- Hard dilepton production from a weakly magnetized hot QCD medium
- Thermomagnetic correlation lengths of strongly interacting matter in the Nambu--Jona-Lasinio model
- Thermo-magnetic nonlocal NJL model in the real and imaginary time formalisms
- Hadronic matter at the edge: A survey of some theoretical approaches to the physics of the QCD phase diagram