13 research outputs found
Chiral Symmetry Restoration at Finite Temperature in the Linear Sigma--Model
The temperature behaviour of meson condensates
is calculated in the -linear sigma model. The couplings of
the Lagrangian are fitted to the physical masses, the pion
decay constant and a scalar mass of GeV. The quartic
terms of the mesonic interaction are converted to a quadratic term with the
help of a Hubbard-Stratonovich transformation. Effective mass terms are
generated this way, which are treated self-consistently to leading order of a
-expansion. We calculate the light and strange -quark condensates using PCAC relations between the meson masses and
condensates. For a cut-off value of 1.5 GeV we find a first-order chiral
transition at a critical temperature MeV. At this temperature the
spontaneously broken subgroup is restored. Entropy density,
energy density and pressure are calculated for temperatures up to and slightly
above the critical temperature. To our surprise we find some indications for a
reduced contribution from strange mesons for .Comment: 17 pages, HD--TVP--93--15. (3 figures - available on request
Radiatively-Induced First-Order Phase Transitions: The Necessity of the Renormalization Group
We advocate a (Wilson) renormalization-group (RG) treatment of
finite-temperature first-order phase transitions, in particular those driven by
radiative corrections such as occur in the standard model, and other
spontaneously-broken gauge theories. We introduce the scale-dependent
coarse-grained free energy S_\La[\phi] which we explicitly calculate, using
the Wilson RG and a (4-\ep)-expansion, for a scalar toy model that shares
many features of the gauged case. As argued by Langer and others, the dynamics
of the phase transition are described by S_\La[\phi] with \La of order the
bubble wall thickness, and {\it not} by the usual (RG-improved)
finite-temperature effective action which is reproduced by S_\La[\phi] for
\La\to 0. We argue that for weakly first-order transitions (such as that in
the standard model) the (4-\ep)-expansion is necessary to control an
inevitable growth of the effective scale-dependent coupling towards the
strong-coupling regime, and that diagrammatic resummation techniques are
unlikely to be appropriate.Comment: 26 pages, two figures, LaTex macropackage. References added and
appendix A revised. LBL preprint LBL-3457
Chiral Symmetry in Two-Color QCD at Finite Temperature
We study the chiral symmetry in two-color QCD with N massless flavors at
finite temperature, using an effective theory. For the gauge group SU(2), the
chiral symmetry is enlarged to SU(2N), which is then spontaneously broken to
Sp(2N) at zero temperature. At finite temperature, and when the axial anomaly
can be neglected, we find a first order phase transition occurring for two or
more flavors. In the presence of instantons, the symmetry restoration
unambiguously remains first order for three or more massless flavors. These
results could be relevant for lattice studies of chiral symmetry at finite
temperature and density.Comment: 10 pages, Revte
Proposal for a Constant Cosmological Constant
It is proposed that the apparent positive acceleration of the cosmological
scale factor is due to the vacuum energy of an incomplete chiral phase
transition in a hidden SU(2) sector. Constraints from primordial
nucleosynthesis imply that the present metastable phase is in a substantially
supercooled state. It is argued that massless chiral condensates can
substantially enhance the possibility of supercooling, and a linear sigma model
exhibiting scale invariance broken only at the quantum level is shown to
accommodate the required supercooling with a reasonable choice of quartic
couplings. The extensive supercooling can in principle be confirmed or rejected
on the basis of interface tension measurements in lattice simulations with
dynamical fermions.Comment: 12 pages, LaTeX, 1 figure; minor rewriting, references corrected,
results unchange
New Universality Classes for Quantum Critical Behavior
We use the epsilon expansion to explore a new universality class of second
order quantum phase transitions associated with a four-dimensional Yukawa field
theory coupled to a traceless Hermitean matrix scalar field. We argue that this
class includes four-fermi models in dimensions with symmetry and a U(N) scalar, iso-vector 4-fermi coupling. The
epsilon expansion indicates that there is a second order phase transition for
, where if .Comment: LaTeX, 9 pages, 1 tarred and uuencoded postscript figure. The new
version contains information on the asymptotic dependence of the critical
number of fermion species on $N_F
Phase transitions in quantum chromodynamics
The current understanding of finite temperature phase transitions in QCD is
reviewed. A critical discussion of refined phase transition criteria in
numerical lattice simulations and of analytical tools going beyond the
mean-field level in effective continuum models for QCD is presented.
Theoretical predictions about the order of the transitions are compared with
possible experimental manifestations in heavy-ion collisions. Various places in
phenomenological descriptions are pointed out, where more reliable data for
QCD's equation of state would help in selecting the most realistic scenario
among those proposed. Unanswered questions are raised about the relevance of
calculations which assume thermodynamic equilibrium. Promising new approaches
to implement nonequilibrium aspects in the thermodynamics of heavy-ion
collisions are described.Comment: 156 pages, RevTex. Tables II,VIII,IX and Fig.s 1-38 are not included
as postscript files. I would like to ask the requestors to copy the missing
tables and figures from the corresponding journal-referenc