TY - JOUR
T1 - Supernova equations of state including full nuclear ensemble with in-medium effects
AU - Furusawa, Shun
AU - Sumiyoshi, Kohsuke
AU - Yamada, Shoichi
AU - Suzuki, Hideyuki
N1 - Funding Information:
S.F. gratefully acknowledges S. Nishimura, M. Takano, M. Hempel and I. Mishustin for their useful discussions. S.F. is supported by Japan Society for the Promotion of Science Postdoctoral Fellowships for Research Abroad ( 28-472 ). Some numerical calculations were carried out on PC cluster at Center for Computational Astrophysics, National Astronomical Observatory of Japan. This work is supported in part by the usage of supercomputer systems through the Large Scale Simulation Program (No. 15/16/-08 ) of High Energy Accelerator Research Organization (KEK) and Post-K Projects (hp160071, hp160211) at K-computer, RIKEN AICS as well as the computational resources provided by RCNP at Osaka University, YITP at Kyoto University, University of Tokyo and JLDG. This work was supported by Grant-in-Aid for the Scientific Research from the Ministry of Education, Culture, Sports, Science and Technology ( MEXT ), Japan ( 24103006 , 24244036 , 16H03986 , 15K05093 , 24105008 , 26104006 ).
Publisher Copyright:
© 2016 Elsevier B.V.
PY - 2017/1/1
Y1 - 2017/1/1
N2 - We construct new equations of state for baryons at sub-nuclear densities for the use in core-collapse supernova simulations. The abundance of various nuclei is obtained together with thermodynamic quantities. The formulation is an extension of the previous model, in which we adopted the relativistic mean field theory with the TM1 parameter set for nucleons, the quantum approach for d, t, h and α as well as the liquid drop model for the other nuclei under the nuclear statistical equilibrium. We reformulate the model of the light nuclei other than d, t, h and α based on the quasi-particle description. Furthermore, we modify the model so that the temperature dependences of surface and shell energies of heavy nuclei could be taken into account. The pasta phases for heavy nuclei and the Pauli- and self-energy shifts for d, t, h and α are taken into account in the same way as in the previous model. We find that nuclear composition is considerably affected by the modifications in this work, whereas thermodynamical quantities are not changed much. In particular, the washout of shell effect has a great impact on the mass distribution above T∼1 MeV. This improvement may have an important effect on the rates of electron captures and coherent neutrino scatterings on nuclei in supernova cores.
AB - We construct new equations of state for baryons at sub-nuclear densities for the use in core-collapse supernova simulations. The abundance of various nuclei is obtained together with thermodynamic quantities. The formulation is an extension of the previous model, in which we adopted the relativistic mean field theory with the TM1 parameter set for nucleons, the quantum approach for d, t, h and α as well as the liquid drop model for the other nuclei under the nuclear statistical equilibrium. We reformulate the model of the light nuclei other than d, t, h and α based on the quasi-particle description. Furthermore, we modify the model so that the temperature dependences of surface and shell energies of heavy nuclei could be taken into account. The pasta phases for heavy nuclei and the Pauli- and self-energy shifts for d, t, h and α are taken into account in the same way as in the previous model. We find that nuclear composition is considerably affected by the modifications in this work, whereas thermodynamical quantities are not changed much. In particular, the washout of shell effect has a great impact on the mass distribution above T∼1 MeV. This improvement may have an important effect on the rates of electron captures and coherent neutrino scatterings on nuclei in supernova cores.
KW - Core-collapse supernova
KW - Equation of state
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U2 - 10.1016/j.nuclphysa.2016.09.002
DO - 10.1016/j.nuclphysa.2016.09.002
M3 - Article
AN - SCOPUS:84987947904
SN - 0375-9474
VL - 957
SP - 188
EP - 207
JO - Nuclear Physics A
JF - Nuclear Physics A
ER -