Bogoliubov condensation of gluons and spontaneous gauge symmetry breaking in QCD

The problem of the gluonic quasiparticle excitations in QCD is considered under the aspect of the condensation of gluon pairs in the ''squeezed'' vacuum. The present approach is a field theoretical generalization of the Bogoliubov model which successfully reproduced the Landau spectrum in the microscopic theory of superfluidity. We construct a gauge invariant QCD Hamiltonian by formally solving the Gauss equation such that the physical variables are separated by a non-Abelian projection operator, instead of fixing a gauge. By using Dirac quantization we show that the Bogoliubov condensation of gluon pairs destroys this projection operator, and the spontaneous appearance of a gluon mass is accompanied by a longitudinal component for the gluon field in correspondence with the relativistic covariance. Gauge symmetry is broken spontaneously since the gauge invariance of the Hamiltonian is not shared by the vacuum. The squeezed vacuum in the present model is characterized by one free parameter related to the contraction of a pair of zero momentum gluon fields which is fixed from the difference of the $\eta'$ and the $\eta$ - meson masses ($ U(1)$-problem) and results in a value for the gluon condensate which is in good agreement with the value obtained by Shifman, Vainshtein and Zakharov.