4,363 research outputs found

    Phase transition in the massive Gross-Neveu model in toroidal topologies

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    We use methods of quantum field theory in toroidal topologies to study the NN-component DD-dimensional massive Gross-Neveu model, at zero and finite temperature, with compactified spatial coordinates. We discuss the behavior of the large-NN coupling constant (gg), investigating its dependence on the compactification length (LL) and the temperature (TT). For all values of the fixed coupling constant (λ\lambda), we find an asymptotic-freedom type of behavior, with g→0g\to 0 as L→0L\to 0 and/or T→∞T\to \infty. At T=0, and for λ≄λc(D)\lambda \geq \lambda_{c}^{(D)} (the strong coupling regime), we show that, starting in the region of asymptotic freedom and increasing LL, a divergence of gg appears at a finite value of LL, 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, Lc(D)L_{c}^{(D)}, and the deconfining temperature, Td(D)T_{d}^{(D)}, are determined as functions of λ\lambda and the mass (mm) of the fermions, in the case of D=2,3,4D=2,3,4. Taking mm as the constituent quark mass (≈350 MeV\approx 350\: MeV), the results obtained are of the same order of magnitude as the diameter (≈1.7fm\approx 1.7 fm) and the estimated deconfining temperature (≈200 MeV\approx 200\: MeV) of hadrons.Comment: 14 pages, 10 figures, 1 table, to appear in Phys. Rev.

    Fermionic vacuum polarization induced by a non-Abelian vortex

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    In this paper, we analyze the fermionic condensate (FC) and the vacuum expectation value (VEV) of the energy-momentum tensor associated with an isospin-1/21/2 charged massive fermionic field induced by the presence of a SU(2)SU(2) 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 ±1/2\pm 1/2 fermionic components of the isospin operator, τ3/2\tau^3/2. 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

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    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 σ = 2.2 ± 0.4 km s^(–1). We reproduce this measurement, but demonstrate that it is inflated by unresolved binary stars. For our sample of 61 stars, the velocity dispersion is σ = 0.7^(+0.6)_(–0.5) km s^(–1). Combining our DEIMOS data with literature values, our final velocity dispersion is σ = 0.4^(+0.4)_( –0.3) km s^(–1). We determine a spectroscopic metallicity of [Fe/H] = –1.6 ± 0.1 dex, placing a 1σ upper limit of σ_([Fe/H]) ~ 0.2 dex on any internal metallicity spread. We determine Palomar 13's total luminosity to be M_V = –2.8 ± 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 = –2.8 ± 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)_(–1.3) × 10^3 M_☉ and a mass-to-light ratio of M/L_V = 2.4^(+5.0)_(–2.4) M_☉/L_☉. 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

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    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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