4,363 research outputs found
Phase transition in the massive Gross-Neveu model in toroidal topologies
We use methods of quantum field theory in toroidal topologies to study the
-component -dimensional massive Gross-Neveu model, at zero and finite
temperature, with compactified spatial coordinates. We discuss the behavior of
the large- coupling constant (), investigating its dependence on the
compactification length () and the temperature (). For all values of the
fixed coupling constant (), we find an asymptotic-freedom type of
behavior, with as and/or . At T=0, and for
(the strong coupling regime), we show that,
starting in the region of asymptotic freedom and increasing , a divergence
of appears at a finite value of , signaling the existence of a phase
transition with the system getting spatially confined. Such a spatial
confinement is destroyed by raising the temperature. The confining length,
, and the deconfining temperature, , are determined
as functions of and the mass () of the fermions, in the case of
. Taking as the constituent quark mass (), the
results obtained are of the same order of magnitude as the diameter () and the estimated deconfining temperature () of
hadrons.Comment: 14 pages, 10 figures, 1 table, to appear in Phys. Rev.
Fermionic vacuum polarization induced by a non-Abelian vortex
In this paper, we analyze the fermionic condensate (FC) and the vacuum
expectation value (VEV) of the energy-momentum tensor associated with an
isospin- charged massive fermionic field induced by the presence of a
vortex, taking into account the effect of the conical geometry produced
by this object. We consider the vortex as an idealized topological defect,
i.e., very thin, straight and carrying a magnetic flux running along its core.
Besides the direct coupling of the fermionic field with the iso-vector gauge
field, we also admit the coupling with the scalar sector of the non-Abelian
vortex system, expressed as a vector in the three-dimensional isospace. Due to
this interaction, the FC is expressed as the sum of two contributions
associated with the two different effective masses for the fermionic
components of the isospin operator, . The VEV of the energy-tensor
also presents a similar structure. The vacuum energy density is equal to the
radial and axial stresses. As to the azimuthal one, it is expressed in terms of
the radial derivative of energy-density. Regarding to the magnetic flux, both,
the FC and the VEV of the energy-momentum tensor, can be positive or negative.
Another interesting consequence of the interaction with the bosonic sector, the
FC and VEV of the energy-momentum tensor, present different intensity for
different values of the ratio between the scalar coupling constant and the mass
of the fermionic field. This is a new feature that the system presents.Comment: 24 pages, 4 figures. Version accepted for publication in IJMP
Structure and Dynamics of the Globular Cluster Palomar 13
We present Keck/DEIMOS spectroscopy and Canada-France-Hawaii Telescope/MegaCam photometry for the Milky Way globular cluster Palomar 13. We triple the number of spectroscopically confirmed members, including many repeat velocity measurements. Palomar 13 is the only known globular cluster with possible evidence for dark matter, based on a Keck/High Resolution Echelle Spectrometer 21 star velocity dispersion of Ï = 2.2 ± 0.4 km s^(â1). We reproduce this measurement, but demonstrate that it is inflated by unresolved binary stars. For our sample of 61 stars, the velocity dispersion is Ï = 0.7^(+0.6)_(â0.5) km s^(â1). Combining our DEIMOS data with literature values, our final velocity dispersion is Ï = 0.4^(+0.4)_( â0.3) km s^(â1). We determine a spectroscopic metallicity of [Fe/H] = â1.6 ± 0.1 dex, placing a 1Ï upper limit of Ï_([Fe/H]) ~ 0.2 dex on any internal metallicity spread. We determine Palomar 13's total luminosity to be M_V = â2.8 ± 0.4, making it among the least luminous known globular clusters. The photometric isophotes are regular out to the half-light radius and mildly irregular outside this radius. The outer surface brightness profile slope is shallower than typical globular clusters (ÎŁ α r^η, η = â2.8 ± 0.3). Thus at large radius, tidal debris is likely affecting the appearance of Palomar 13. Combining our luminosity with the intrinsic velocity dispersion, we find a dynamical mass of M_(1/2) = 1.3^(+2:7)_(â1.3) Ă 10^3 M_â and a mass-to-light ratio of M/L_V = 2.4^(+5.0)_(â2.4) M_â/L_â. Within our measurement errors, the mass-to-light ratio agrees with the theoretical predictions for a single stellar population. We conclude that, while there is some evidence for tidal stripping at large radius, the dynamical mass of Palomar 13 is consistent with its stellar mass and neither significant dark matter, nor extreme tidal heating, is required to explain the cluster dynamics
Bosonic Casimir effect in an aether-like Lorentz-violating scenario with higher order derivatives
In this paper we investigate the bosonic Casimir effect in a
Lorentz-violating symmetry scenario. The theoretical model adopted consists of
a real massive scalar quantum field confined in a region between two large
parallel plates, having its dynamics governed by a modified Klein-Gordon
equation that presents a Lorentz symmetry breaking term. In this context we
admit that the quantum field obeys specific boundary conditions on the plates.
The Lorentz-violating symmetry is implemented by the presence of an arbitrary
constant space-like vector in a CPT-even aether-like approach, considering a
direct coupling between this vector with the derivative of the field in higher
order. The modification on the Klein-Gordon equation produces important
corrections on the Casimir energy and pressure. Thus, we show that these
corrections strongly depend on the order of the higher derivative term and the
specific direction of the constant vector, as well as the boundary conditions
considered.Comment: 21 pages, 5 figure
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