Resolving the instability of the Savvidy vacuum by dynamical gluon mass
arXiv:0712.0570 · doi:10.1016/j.physletb.2008.01.013
Abstract
In this paper we apply the formalism of local composite operators as developed by Verschelde et al. in combination with a constant chromomagnetic field as considered in the seventies by Savvidy and others. We find that a nonzero <A_μ^2> minimizes the vacuum energy, as in the case with no chromomagnetic field, and that the chromomagnetic field itself is near-to zero. The Nielsen-Olesen instability, caused by the imaginary part in the action, also vanishes. We further investigate the effect of an external chromomagnetic field on the value of <A_μ^2>, finding that this condensate is destroyed by sufficiently strong fields. The inverse scenario, where <A_μ^2> is considered as external, results in analogous findings: when this condensate is sufficiently large, the induced chromomagnetic field is lowered to a perturbative value slightly below the applied <A_μ^2>.
11 pages, 8 figures
References in corpus (1)
Cited by in corpus (6)
- Indirect lattice evidence for the Refined Gribov-Zwanziger formalism and the gluon condensate in the Landau gauge
- Vacuum polarization corrections to low energy quark effective couplings
- The asymmetry of the dimension 2 gluon condensate: the zero temperature case
- The asymmetry of the dimension 2 gluon condensate: the finite temperature case
- Remarks on confinement driven by axion-like particles in Yang-Mills theories
- Chromomagnetic Condensate in Finite-Temperature SU(2) Yang-Mills Theory under Imaginary Rotation