538 research outputs found
Phase structure of compactified gauge theories in magnetic backgrounds
We discuss the properties of non-abelian gauge theories formulated on
manifolds with compactified dimensions and in the presence of fermionic fields
coupled to magnetic backgrounds. We show that different phases may emerge,
corresponding to different realizations of center symmetry and translational
invariance, depending on the compactification radius and on the magnitude of
the magnetic field. Our discussion focuses on the case of an gauge
theory in 4 dimensions with fermions fields in the fundamental representation,
for which we provide some exploratory numerical lattice results.Comment: 5 pages, 7 figure
Magnetic susceptibility and equation of state of N_f = 2+1 QCD with physical quark masses
We determine the free energy of strongly interacting matter as a function of
an applied constant and uniform magnetic field. We consider N_f = 2+1 QCD with
physical quark masses, discretized on a lattice by stout improved staggered
fermions and a tree level improved Symanzik pure gauge action, and explore
three different lattice spacings. For magnetic fields of the order of those
produced in non-central heavy ion collisions (eB ~ 0.1 GeV^2) strongly
interacting matter behaves like a medium with a linear response, and is
paramagnetic both above and below the deconfinement transition, with a
susceptibility which steeply rises in the deconfined phase. We compute the
equation of state, showing that the relative increase in the pressure due to
the magnetic field gets larger around the transition, and of the order of 10 %
for eB ~ 0.1 GeV^2.Comment: 11 pages, 10 figures, 3 tables. Final version published in Physical
Review
Magnetic Susceptibility of Strongly Interacting Matter across the Deconfinement Transition
We propose a method to determine the total magnetic susceptibility of
strongly interacting matter by lattice QCD simulations, and present first
numerical results for the theory with two light flavors, which suggest a weak
magnetic activity in the confined phase and the emergence of strong
paramagnetism in the deconfined, Quark-Gluon Plasma phase.Comment: 6 pages, 6 figures, 2 tables. Final version published in Physical
Review Letter
Susceptibility of the QCD vacuum to CP-odd electromagnetic background fields
We investigate two flavor QCD in presence of CP-odd electromagnetic
background fields and determine, by means of lattice QCD simulations, the
induced effective theta term to the first order in the scalar product of E and
B. We employ a rooted staggered discretization and study lattice spacings down
to 0.1 fm and Goldstone pion masses around 480 MeV. In order to deal with a
positive measure, we consider purely imaginary electric fields and real
magnetic fields, then exploiting analytic continuation. Our results are
relevant to a description of the effective pseudoscalar QED-QCD interactions.Comment: 5 pages, 4 figures, 1 table. New data and references added. Matches
the published versio
Curvature of the chiral pseudo-critical line in QCD
We determine the curvature of the pseudo-critical line of strong interactions
by means of numerical simulations at imaginary chemical potentials. We consider
stout improved staggered fermions with physical quark masses and the
tree level Symanzik gauge action, and explore two different sets of lattice
spacings, corresponding to temporal extensions and . Both
the renormalized chiral condensate and the renormalized chiral susceptibility
are used to locate the transition. The determinations obtained from the two
quantities are in good agreement, a preliminary continuum extrapolation yields
. We also investigate the impact of a non-zero strange
quark chemical potential and compare our results to previous determinations in
the literature, discussing the possible sources of systematic errors affecting
the various procedures.Comment: 16 pages, 12 figures, 11 tables. Published versio
Anisotropy of the quark-antiquark potential in a magnetic field
We investigate the static -potential for QCD at
the physical point in the presence of a constant and uniform external magnetic
field. The potential is found to be anisotropic and steeper in the directions
transverse to the magnetic field than in the longitudinal one. In particular,
when compared to the standard case with zero background field, the string
tension increases (decreases) in the transverse (longitudinal) direction, while
the absolute value of the Coulomb coupling and the Sommer parameter show an
opposite behavior.Comment: 6 pages, 5 figures, 1 table. Final published versio
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