https://doi.org/10.1140/epjc/s2004-02072-3
theoretical physics
T-dependent Dyson-Schwinger equation in IR regime of QCD: the critical point
Center for Academic Excellence on Cosmology & Particle Astrophysics, National Taiwan University, Taipei 106, Taiwan, R.O.C
* e-mail: ganmitra@nde.vsnl.net.in
The quark mass function in QCD is revisited, using a gluon propagator in the form 1/(k
2 + m
g
2) plus
, where the second (IR) term gives linear confinement for m
g
= 0 in the instantaneous limit, μ being another scale. To find
we propose a new (differential) form of the Dyson-Schwinger equation (DSE) for
, based on an infinitesimal subtractive renormalization via a differential operator which lowers the degree of divergence in integration on the RHS, by two units. This warrants
in the integrand since its k-dependence is no longer sensitive to the principal term (p-k)2 in the quark propagator. The simplified DSE (which incorporates the Ward-Takahashi (WT) identity in the Landau gauge) is satisfied for large p
2 by
=
, except for Log factors. The limit p
2 = 0 determines
. A third limit, p
2 = -m
0
2, defines the dynamical mass m
0 via
. After two checks (
MeV and
=
), for
with
MeV, the T-dependent DSE is used in the real time formalism to determine the “critical” index
analytically, with the IR term partly serving as the H-field. We find
MeV and check the vanishing of
and
at T
c.
© Springer-Verlag, 2005