461 research outputs found
Correlation between conserved charges in PNJL Model with multi-quark interactions
We present a study of correlations among conserved charges like baryon
number, electric charge and strangeness in the framework of 2+1 flavor Polyakov
loop extended Nambu-Jona-Lasinio model at vanishing chemical potentials, up to
fourth order. Correlations up to second order have been measured in Lattice QCD
which compares well with our estimates given the inherent difference in the
pion masses in the two systems. Possible physical implications of these
correlations and their importance in understanding the matter obtained in
heavy-ion collisions are discussed. We also present comparison of the results
with the commonly used unbound effective potential in the quark sector of this
model
Susceptibilities with multi-quark interactions in PNJL model
We have investigated the fluctuations and the higher order susceptibilities
of quark number, isospin number, electric charge and strangeness at vanishing
chemical potential for 2+1 flavor Polyakov loop extended Nambu--Jona-Lasinio
model. The calculations are performed for the bound effective potential in the
quark sector requiring up to eight quark interaction terms. These have been
contrasted to the lattice results which currently have somewhat heavier quarks
in the light flavor sector. The results show sufficient qualitative agreement.
For comparison we also present the results obtained with the conventional
effective potential containing upto six quark interaction terms.Comment: To appear Physical Review
Trouble Finding the Optimal AdS/QCD
In the bottom-up approach to AdS/QCD based on a five-dimensional gravity
dilaton action the exponential of the dilaton field is usually identified as
the strong or 't Hooft coupling. There is currently no model known which fits
the measurements of the running coupling and lattice results for pressure at
the same time. With a one parametric toy model we demonstrate the effect of
fitting the pressure on the coupling and vice versa.Comment: 4 pages, 3 figure
Neutrino and antineutrino CCQE scattering in the SuperScaling Approximation from MiniBooNE to NOMAD energies
We compare the predictions of the SuperScaling model for charged current
quasielastic muonic neutrino and antineutrino scattering from C with
experimental data spanning an energy range up to 100 GeV. We discuss the
sensitivity of the results to different parametrizations of the nucleon vector
and axial-vector form factors. Finally, we show the differences between
electron and muon (anti-)neutrino cross sections relevant for the STORM
facility.Comment: 14 pages, 7 figures; v2: small corrections in the text and two added
references; version accepted for publication by Phys. Lett.
The Phase Structure of the Polyakov--Quark-Meson Model
The relation between the deconfinement and chiral phase transition is
explored in the framework of an Polyakov-loop-extended two-flavor quark-meson
(PQM) model. In this model the Polyakov loop dynamics is represented by a
background temporal gauge field which also couples to the quarks. As a novelty
an explicit quark chemical potential and N_f-dependence in the Polyakov loop
potential is proposed by using renormalization group arguments. The behavior of
the Polyakov loop as well as the chiral condensate as function of temperature
and quark chemical potential is obtained by minimizing the grand canonical
thermodynamic potential of the system. The effect of the Polyakov loop dynamics
on the chiral phase diagram and on several thermodynamic bulk quantities is
presented.Comment: 13 pages, 12 figures, RevTex4; discussion of mu-dependence extended,
references added, version to be published in PR
The frozen nucleon approximation in two-particle two-hole response functions
We present a fast and efficient method to compute the inclusive two-particle
two-hole (2p-2h) electroweak responses in the neutrino and electron
quasielastic inclusive cross sections. The method is based on two
approximations. The first neglects the motion of the two initial nucleons below
the Fermi momentum, which are considered to be at rest. This approximation,
which is reasonable for high values of the momentum transfer, turns out also to
be quite good for moderate values of the momentum transfer . The
second approximation involves using in the "frozen" meson-exchange currents
(MEC) an effective -propagator averaged over the Fermi sea. Within the
resulting "frozen nucleon approximation", the inclusive 2p-2h responses are
accurately calculated with only a one-dimensional integral over the emission
angle of one of the final nucleons, thus drastically simplifying the
calculation and reducing the computational time. The latter makes this method
especially well-suited for implementation in Monte Carlo neutrino event
generators.Comment: 8 pages, 5 figures and 1 tabl
Extensions of Superscaling from Relativistic Mean Field Theory: the SuSAv2 Model
We present a systematic analysis of the quasielastic scaling functions
computed within the Relativistic Mean Field (RMF) Theory and we propose an
extension of the SuperScaling Approach (SuSA) model based on these results. The
main aim of this work is to develop a realistic and accurate phenomenological
model (SuSAv2), which incorporates the different RMF effects in the
longitudinal and transverse nuclear responses, as well as in the isovector and
isoscalar channels. This provides a complete set of reference scaling functions
to describe in a consistent way both processes and the
neutrino/antineutrino-nucleus reactions in the quasielastic region. A
comparison of the model predictions with electron and neutrino scattering data
is presented.Comment: 19 pages, 24 figure
Two-nucleon emission in neutrino and electron scattering from nuclei: the modified convolution approximation
The theoretical formalism of inclusive lepton-nucleus scattering in the
two-nucleon emission channel is discussed in the context of a simplified
approach, the modified convolution approximation. This allows one to write the
2p2h responses of the relativistic Fermi gas as a folding integral of two 1p1h
responses with the energies and momenta transferred to each nucleon. The idea
behind this method is to introduce different average momenta for the two
initial nucleons in the matrix elements of the two-body current, with the
innovation that they depend on the transferred energies and momenta. This
method treats exactly the two-body phase space kinematics, and reduces the
formulae of the response functions from seven-dimensional integrals over
momenta to much simpler three-dimensional ones. The applicability of the method
is checked by comparing with the full results within a model of electroweak
meson-exchange currents. The predictions are accurate enough, especially in the
low-energy threshold region where the average momentum approximation works the
best.Comment: 35 pages, 13 figure
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