DOI: 10.1140/epjc/s2003-01170-0
Confinement and mass gap in abelian gauge
U. Ellwanger1 and N. Wschebor1, 21 Laboratoire de Physique Théorique , Université de Paris XI, Bâtiment 210, 91405 Orsay Cedex, France
2 Instituto de Física, Facultad de Ingeniería (C.C. 30, CP 1100), Montevideo, Uruguay
(Received: 27 November 2002 / Published online: 14 April 2003 )
Abstract
First, we present a simple confining abelian pure gauge theory.
Classically, its kinetic term is not positive definite, and it
contains
a simple UV regularized
F4 interaction. This provokes the
formation
of a condensate
such that, at the saddle point
of the effective potential, the wave function
normalization constant of the abelian gauge fields
vanishes exactly. Then
we study
SU(2) pure
Yang-Mills theory in an abelian gauge and introduce an auxiliary
field
for a BRST invariant condensate of dimension 2, which
renders
the charged sector massive. Under simple assumptions its effective
low
energy theory reduces to the confining abelian model discussed
before,
and the VEV of
is seen to scale correctly with the
renormalization point. Under these assumptions, the confinement
condition
Zeff = 0 also holds for the massive
charged sector,
which suppresses the couplings of the charged fields to the abelian
gauge bosons in the infrared regime.
© Società Italiana di Fisica, Springer-Verlag 2003