60 research outputs found

    The r-process nucleosynthesis in the various jet-like explosions of magnetorotational core-collapse supernovae

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    The r-process nucleosynthesis in core-collapse supernovae (CC-SNe) is studied, with a focus on the explosion scenario induced by rotation and strong magnetic fields. Nucleosynthesis calculations are conducted based on magneto-hydrodynamical explosion models with a wide range of parameters for initial rotation and magnetic fields. The explosion models are classified in two different types: i.e., prompt-magnetic-jet and delayed-magnetic-jet, for which the magnetic fields of proto-neutron stars (PNSs) during collapse and the core-bounce are strong and comparatively moderate, respectively. Following the hydrodynamical trajectories of each explosion model, we confirmed that r-processes successfully occur in the prompt-magnetic-jets, which produce heavy nuclei including actinides. On the other hand, the r-process in the delayed-magnetic-jet is suppressed, which synthesizes only nuclei up to the second peak (A∼130A \sim 130). Thus, the r-process in the delayed-magnetic-jets could explain only "weak r-process" patterns observed in metal-poor stars rather than the "main r-process", represented by the solar abundances. Our results imply that core-collapse supernovae are possible astronomical sources of heavy r-process elements if their magnetic fields are strong enough, while weaker magnetic explosions may produce "weak r-process" patterns (A≲130A \lesssim 130). We show the potential importance and necessity of magneto-rotational supernovae for explaining the galactic chemical evolution, as well as abundances of r-process enhanced metal-poor stars. We also examine the effects of the remaining uncertainties in the nature of PNSs due to weak interactions that determine the final neutron-richness of ejecta. Additionally, we briefly discuss radioactive isotope yields in primary jets (e.g., 56^{56}Ni), with relation to several optical observation of SNe and relevant high-energy astronomical phenomena.Comment: 25 pages, 17 figures, 6 tables, ApJ in press, numerical data are available at http://www.astro.keele.ac.uk/~nobuya/mrsn and https://github.com/nnobuya/mrs

    Impact of the first-forbidden β\beta decay on the production of A∼195A \sim 195 r-process peak

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    We investigated the effects of first-forbidden transitions in β\beta decays on the production of the r-process A∼195A \sim 195 peak. The theoretical calculated β\beta-decay rates with β\beta-delayed neutron emission were examined using several astrophysical conditions. As the first-borbidden decay is dominant in N∼126N \sim 126 neutron-rich nuclei, their inclusion shortens β\beta-decay lifetimes and shifts the abundance peak towards higher masses. Additionally, the inclusion of the β\beta-delayed neutron emission results in a wider abundance peak, and smoothens the mass distribution by removing the odd-even mass staggering. The effects are commonly seen in the results of all adopted astrophysical models. Nevertheless there are quantitative differences, indicating that remaining uncertainty in the determination of half-lives for N=126N=126 nuclei is still significant in order to determine the production of the r-process peak.Comment: 6 pages, 4 figures, 1 table, Phys. Lett. B, in pres

    Mass Ejection from the Remnant of a Binary Neutron Star Merger: Viscous-Radiation Hydrodynamics Study

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    We perform long-term general relativistic neutrino radiation hydrodynamics simulations (in axisymmetry) for a massive neutron star (MNS) surrounded by a torus, which is a canonical remnant formed after the binary neutron star merger. We take into account the effects of viscosity, which is likely to arise in the merger remnant due to magnetohydrodynamical turbulence. As the initial condition, we employ the azimuthally averaged data of the MNS-torus system derived in a three-dimensional, numerical-relativity simulation for the binary neutron star merger. The viscous effect plays key roles for the remnant evolution and mass ejection from it in two phases of the evolution. In the first t≲10t\lesssim10 ms, a differential rotation state of the MNS is changed to a rigidly rotating state, and as a result, a sound wave, which subsequently becomes a shock wave, is formed in the vicinity of the MNS due to the variation of the quasi-equilibrium state of the MNS. The shock wave induces significant mass ejection of mass ∼(0.5−2.0)×10−2M⊙\sim(0.5-2.0)\times 10^{-2}M_\odot for the alpha viscosity parameter of 0.01−0.040.01-0.04. For the longer-term evolution with ∼0.1−10\sim 0.1-10 s, a significant fraction of the torus material is ejected. The ejecta mass is likely to be of order 10−2M⊙10^{-2}M_\odot, so that the total mass of the viscosity-driven ejecta could dominate that of the dynamical ejecta of mass ≲10−2M⊙\lesssim 10^{-2}M_\odot. The electron fraction, YeY_e, of the ejecta is always high enough (Ye≳0.25Y_e\gtrsim0.25) that this post-merger ejecta is lanthanide-poor; hence, the opacity of the ejecta is likely to be ∼10−100\sim 10-100 times lower than that of the dynamical ejecta. This indicates that the electromagnetic signal from the ejecta would be rapidly evolving, bright, and blue if it is observed from a small viewing angle (≲45∘\lesssim 45^\circ) for which the effect of the dynamical ejecta is minor.Comment: 21 pages, 18 figures, accepted for publication in Ap

    State of sulphur and Iron-Sulphur Interaction in Soda Silicate Glasses(Materials, Metallurgy, Weldability)

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    Production of all the r-process nuclides in the dynamical ejecta of neutron star mergers

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    Recent studies suggest that binary neutron star (NS-NS) mergers robustly produce the heavy r-process nuclei above the atomic mass number A ~ 130 because of their ejecta consisting of almost pure neutrons (electron fraction of Y_e < 0.1). However, little production of the lighter r-process nuclei (A = 90-120) conflicts with the spectroscopic results of r-process-enhanced Galactic halo stars. We present, for the first time, the result of nucleosynthesis calculations based on the fully general-relativistic simulation of a NS-NS merger with approximate neutrino transport. It is found that the bulk of the dynamical ejecta are appreciably shock-heated and neutrino-processed, resulting in a wide range of Y_e (= 0.09-0.45). The mass-averaged abundance distribution of calculated nucleosynthesis yields is in reasonable agreement with the full-mass range (A = 90-240) of the solar r-process curve. This implies, if our model is representative of such events, that the dynamical ejecta of NS-NS mergers can be the origin of the Galactic r-process nuclei. Our result also shows that the radioactive heating after ~ 1 day from the merging, giving rise to r-process-powered transient emission, is dominated by the beta-decays of several species close to stability with precisely measured half-lives. This implies that the total radioactive heating rate for such an event can be well constrained within about a factor of two if the ejected material has a solar-like r-process pattern.Comment: 6 pages, 5 figures, accepted for publication in ApJL. Section 2 was significantly changed according to the referee's advices. Our result was unchange

    Impact of New beta-decay Half-lives on r-process Nucleosynthesis

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    We investigate the effects of newly measured beta-decay half-lives on r-process nucleosynthesis. These new rates were determined by recent experiments at the radioactive isotope beam factory facility in the RIKEN Nishina Center. We adopt an r-process nucleosynthesis environment based on a magnetohydrodynamic supernova explosion model that includes strong magnetic fields and rapid rotation of the progenitor. A number of the new beta-decay rates are for nuclei on or near the r-process path, and hence they affect the nucleosynthesis yields and time scale of the r-process. The main effect of the newly measured beta-decay half-lives is an enhancement in the calculated abundance of isotopes with mass number A = 110 -- 120 relative to calculated abundances based upon beta-decay rates estimated with the finite-range droplet mass model. This effect slightly alleviates, but does not fully explain, the tendency of r-process models to underproduce isotopes with A = 110 -- 120 compared to the solar-system r-process abundances.Comment: 9 pages, 3 figures, 1 table, published in PR
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