1,017 research outputs found
Pion-less effective field theory for atomic nuclei and lattice nuclei
We compute the medium-mass nuclei O and Ca using pionless
effective field theory (EFT) at next-to-leading order (NLO). The low-energy
coefficients of the EFT Hamiltonian are adjusted to experimantal data for
nuclei with mass numbers and , or alternatively to results from
lattice quantum chromodynamics (QCD) at an unphysical pion mass of 806 MeV. The
EFT is implemented through a discrete variable representation in the harmonic
oscillator basis. This approach ensures rapid convergence with respect to the
size of the model space and facilitates the computation of medium-mass nuclei.
At NLO the nuclei O and Ca are bound with respect to decay into
alpha particles. Binding energies per nucleon are 9-10 MeV and 30-40 MeV at
pion masses of 140 MeV and 806 MeV, respectively.Comment: 26 page
Close binary evolution I. The tidally induced shear mixing in rotating binaries
We study how tides in a binary system induce some specific internal shear
mixing, able to substantially modify the evolution of close binaries prior to
mass transfer. We construct numerical models accounting for tidal interactions,
meridional circulation, transport of angular momentum, shears and horizontal
turbulence and consider a variety of orbital periods and initial rotation
velocities. Depending on orbital periods and rotation velocities, tidal effects
may spin down (spin down Case) or spin up (spin up Case) the axial rotation. In
both cases, tides may induce a large internal differential rotation. The
resulting tidally induced shear mixing (TISM) is so efficient that the internal
distributions of angular velocity and chemical elements are greatly influenced.
The evolutionary tracks are modified, and in both cases of spin down and spin
up, large amounts of nitrogen can be transported to the stellar surfaces before
any binary mass transfer. Meridional circulation, when properly treated as an
advection, always tends to counteract the tidal interaction, tending to spin up
the surface when it is braked down and vice versa. As a consequence, the times
needed for the axial angular velocity to become equal to the orbital angular
velocity may be larger than given by typical synchronization timescales. Also,
due to meridional circulation some differential rotation remains in tidally
locked binary systems.Comment: 10 pages, 18 figures, Accepted for publication in Astronomy and
Astrophysic
Are some CEMP-s stars the daughters of spinstars?
Carbon-enhanced metal-poor (CEMP)-s stars are long-lived low-mass stars with a very low iron content as well as overabundances of carbon and s-elements. Their peculiar chemical pattern is often explained by pollution from an asymptotic giant branch (AGB) star companion. Recent observations have shown that most CEMP-s stars are in binary systems, providing support to the AGB companion scenario. A few CEMP-s stars, however, appear to be single. We inspect four apparently single CEMP-s stars and discuss the possibility that they formed from the ejecta of a previous-generation massive star, referred to as the “source” star. In order to investigate this scenario, we computed low-metallicity massive-star models with and without rotation and including complete s-process nucleosynthesis. We find that non-rotating source stars cannot explain the observed abundance of any of the four CEMP-s stars. Three out of the four CEMP-s stars can be explained by a 25M⊙ source star with vini ~ 500 km s-1 (spinstar). The fourth CEMP-s star has a high Pb abundance that cannot be explained by any of the models we computed. Since spinstars and AGB predict different ranges of [O/Fe] and [ls/hs], these ratios could be an interesting way to further test these two scenarios. nuclear reactions, nucleosynthesis, abundances / stars: interiors / stars: chemically peculiar / stars: abundances / stars: massiv
Very Massive Star Models: I. Impact of Rotation and Metallicity and Comparisons with Observations
In addition to being spectacular objects, Very Massive Stars (VMS) are
suspected to have a tremendous impact on their environment and on the whole
cosmic evolution. The nucleosynthesis both during their advanced stages and
their final explosion may contribute greatly to the overall enrichment of the
Universe. Their resulting supernovae are candidates for the most superluminous
events and their extreme conditions also lead to very important radiative and
mechanical feedback effects, from local to cosmic scale. We explore the impact
of rotation and metallicity on the evolution of very massive stars across
cosmic times. With the recent implementation of an equation of state in the
GENEC stellar evolution code, appropriate for describing the conditions in the
central regions of very massive stars in the advanced phases, we present new
results on VMS evolution from Population III to solar metallicity. Low
metallicity VMS models are highly sensitive to rotation, while the evolution of
higher metallicity models is dominated by mass loss effects. The mass loss
affects strongly their surface velocity evolution, breaking quickly at high
metallicity while reaching the critical velocity for low metallicity models.
The comparison to observed VMS in the LMC shows that the mass loss
prescriptions used for these models are compatible with observed mass loss
rates. In our framework for modelling rotation, our models of VMS need a high
initial velocity to reproduce the observed surface velocities. The surface
enrichment of these VMS is difficult to explain with only one initial
composition, and could suggest multiple populations in the R136 cluster. At a
metallicity typical of R136, only our non- or slowly rotating VMS models may
produce Pair Instability supernovae. The most massive black holes that can be
formed are less massive than about 60 M.Comment: 13 pages, 11 figure
Effects of three-nucleon forces and two-body currents on Gamow-Teller strengths
We optimize chiral interactions at next-to-next-to leading order to
observables in two- and three-nucleon systems, and compute Gamow-Teller
transitions in carbon-14, oxygen-22 and oxygen-24 using consistent two-body
currents. We compute spectra of the daughter nuclei nitrogen-14, fluorine-22
and fluorine-24 via an isospin-breaking coupled-cluster technique, with several
predictions. The two-body currents reduce the Ikeda sum rule, corresponding to
a quenching factor q^2 ~ 0.84-0.92 of the axial-vector coupling. The half life
of carbon-14 depends on the energy of the first excited 1+ state, the
three-nucleon force, and the two-body current
Evolution of the first stellar generations
Although the theoretical study of very low metallicity (Z) and metal-free
stars is not new, their importance has recently greatly increased since two
related fields have been developing rapidly. The first is cosmological
simulations of the formation of the first stars and of the reionisation period.
The second is the observations of extremely metal poor stars. In this paper, we
present pre-supernova evolution models of massive rotating stars at very low Z
(Z=1e-8) and at Z=0. Rotation has a strong impact on mass loss and
nucleosynthesis. Models reaching break-up velocities lose up to ten percents of
their initial mass. In very low Z models, rotational and convective mixing
enhances significantly the surface content in carbon, nitrogen and oxygen (CNO)
when the star becomes a red supergiant. This induces a strong mass loss for
stars more massive than about 60 solar masses. Our models predict type Ib,c
supernovae and gamma-ray bursts at very low Z. Rotational mixing also induces a
large production of CNO elements, in particular of primary nitrogen. The
stellar wind chemical composition is compatible with the most metal-poor star
know to date, HE 1327-2326, for CNO elements. Our models reproduce the early
evolution of nitrogen in the Milky Way.Comment: 6 pages, 3 figure, to appear in the proceedings of "Chemodynamics:
from the first stars to local galaxies ...", Lyon, France, 10-14 July 200
Effects of rotation on the evolution of primordial stars
(Abridged) Rotation has been shown to play a determinant role at very low
metallicity, bringing heavy mass loss where almost none was expected. Is this
still true when the metallicity strictly equals zero? The aim of our study is
to get an answer to this question, and to determine how rotation changes the
evolution and the chemical signature of the primordial stars. We have
calculated 14 differentially-rotating and non-rotating stellar models at zero
metallicity, with masses between 9 and 200 Msol. The evolution has been
followed up to the pre-supernova stage. We find that Z=0 models rotate with an
internal profile Omega(r) close to local angular momentum conservation, because
of a very weak core-envelope coupling. Rotational mixing drives a H-shell boost
due to a sudden onset of CNO cycle in the shell. This boost leads to a high 14N
production. Generally, the rotating models produce much more metals than their
non-rotating counterparts. The mass loss is very low, even for the models that
reach the critical velocity during the main sequence. Due to the low mass loss
and the weak coupling, the core retains a high angular momentum at the end of
the evolution. The high rotation rate at death probably leads to a much
stronger explosion than previously expected, changing the fate of the models.
The inclusion of our yields in a chemical evolution model of the Galactic halo
predicts log values of N/O, C/O and 12C/13C ratios of -2.2, -0.95 and 50
respectively at log O/H +12 = 4.2.Comment: 14 pages, 9 figures, accepted for publication in A&A (English not
corrected
An optimized chiral nucleon-nucleon interaction at next-to-next-to-leading order
We optimize the nucleon-nucleon interaction from chiral effective field
theory at next-to-next- to-leading order. The resulting new chiral force
NNLOopt yields \chi^2 \approx 1 per degree of freedom for laboratory energies
below approximately 125 MeV. In the A = 3, 4 nucleon systems, the contributions
of three-nucleon forces are smaller than for previous parametrizations of
chiral interactions. We use NNLOopt to study properties of key nuclei and
neutron matter, and demonstrate that many aspects of nuclear structure can be
understood in terms of this nucleon-nucleon interaction, without explicitly
invoking three-nucleon forces.Comment: 6 pages, 4 figure
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