18–23 Jun 2017
Laboratori Nazionali del Sud
Europe/Rome timezone

Roles of nuclear weak rates on the evolution of degenerate cores in stars

19 Jun 2017, 13:00
20m
Sala conferenze (Laboratori Nazionali del Sud)

Sala conferenze

Laboratori Nazionali del Sud

Via S. Sofia 62 I-95123 Catania Italy

Speaker

Prof. Toshio Suzuki (Nihon University)

Description

% % Nuclear Physics in Astrophysics 8 template for abstract % % Format: LaTeX2e. % % Rename this file to name.tex, where `name' is the family name % of the first author, and edit it to produce your abstract. % \documentstyle[11pt]{article} % % PAGE LAYOUT: % \textheight=9.9in \textwidth=6.3in \voffset -0.85in \hoffset -0.35in \topmargin 0.305in \oddsidemargin +0.35in \evensidemargin -0.35in %\renewcommand{\rmdefault}{ptm} % to use Times font \long\def\TITLE#1{{\Large{\bf#1}}}\long\def\AUTHORS#1{ #1\\[3mm]} \long\def\AFFILIATION#1#2{$^{#1}\,$ #2\\} \begin{document} {\small \it Nuclear Physics in Astrophysics 8, NPA8: 18-23 June 2017, Catania, Italy} \vspace{12pt} \thispagestyle{empty} \begin{center} %%% %%% Title goes here. %%% \TITLE{Roles of nuclear weak rates on the evolution of degenerate cores in stars}\\[3mm] %%% %%% Authors and affiliations are next. The presenter should be %%% underlined as shown below. %%% \AUTHORS{ Toshio Suzuki$^{1,2}$, N. Tsunoda$^{3}$, Y. Tsunoda$^{3}$, N. Shimizu$^{3}$, T. Otsuka$^{4,5}$} %%% {\small \it \AFFILIATION{1}{Department of Physics, College of Humanities and Sciences, Nihon University, Setagaya-ku, Tokyo 156-8550, Japan} \AFFILIATION{2}{National Astronomical Observatory of Japan, Mitaka, Tokyo 181-8588, Japan} \AFFILIATION{3}{Center for Nuclear Study, The University of Tokyo, Hongo, Tokyo 113-0033, Japan} \AFFILIATION{4}{Department of Physics, The University of Tokyo, Hongo, Tokyo 113-0033, Japan} \AFFILIATION{5}{National Superconducting Cyclotron Laboratory, Michigan State University, %East Lansing, MI 48824, USA} } %%% \vspace{12pt} % Do not modify % Enter contact e-mail address here. \centerline{Contact email: {\it suzuki@phys.chs.nihon-u.ac.jp}} \vspace{18pt} % Do not modify \end{center} %%% %%% Abstract proper starts here. %%% Electron-capture and $\beta$-decay rates in nuclei at stellar environments evaluated with new shell-model Hamiltonians have been applied to cooling processes and nucleosynthesis in electron-degenerate cores in stars. Nuclear Urca processes in electron-degenerate O-Ne-Mg cores of stars with initial masses of 8-10 M$_{\odot}$ have been studied using the weak rates for $sd$-shell nuclei obtained for the USDB Hamiltonian, and the processes for nuclear pairs with A=23 and 25 are found to be important for the cooling of the cores and determination of the final fate of the stars [1]. Important roles of the nuclear Urca processes have been pointed out also in C-O and hybrid C-O-Ne white dwarfs (WD) [2,3]. The nuclear weak rates obtained in a large region of $pf$-shell nuclei by GXPF1J [4] have been applied to study nucleosynthesis in Type-Ia supernova explosions (SNe), which result from accreting C-O WD in close binaries. Over-production of neutron-rich isotopes in the iron group elements compared to the solar abundance noticed for the Fuller-Fowler-Newman rates has been considerably reduced [5]. We extend our study of applications of updated nuclear weak rates to cooling processes and evolution of degenerate cores in stars in the region outside one-major $sd$- and $pf$-shells. The weak rates for nuclear pairs important for Urca processes in neutron star crusts [6] are studied. In particular, weak rates of nuclei in the island of inversion such as $^{31}$Mg are evaluated based on microscopic interactions obtained by extended Kuo-Krenciglowa (EKK) method [7]. The method can explain well the structure of neutron-rich Mg isotopes. Spectra of $^{31}$Mg, in particular, are successfully reproduced by the EKK method in contrast to other approaches. Fe-core-collapse SNe are sensitive to the e-capture rates for extremely neutron-rich isotopes near $^{78}$Ni [8] as well as iron group nuclei. Electron-capture rates in $^{78}$Ni are evaluated with extension of the configuration space outside the $pf$-shell [9], and compared with RPA calculations and Sullivan’s approximate formula [8]. In $p$-shell region, an accurate shell-model evaluation is carried out for e-capture rates on $^{13}$N, which is important during carbon simmering stage of C-O WD prior to the onset of thermonuclear explosions [3]. Nuclear weak transition rates, thus, play important roles on the final evolution of degenerate cores in stars. Accurate evaluation of the nuclear weak rates is essential for the studies of astrophysical processes sensitive to the rates. \bigskip {\small \noindent [1] T. Suzuki, H. Toki and K. Nomoto, ApJ. 817 (2016) 163; H. Toki, T. Suzuki, K. Nomoto, S. Jones and R. Hirsci, Phys. Rev. C 88 (2013) 015806; S. Jones et al., ApJ. 772 (2013) 150. \noindent [2] P. A. Dennisenkov et al., MNRAS 447 (2015) 2696. \noindent [3] H. Martinez-Rodriguez et al., ApJ. 825 82016) 57. \noindent [4] M. Honma et al., Phy. Rev. C 69 (2004) 034335; J. Phys. Conf. Ser. 20 (2005) 7. \noindent [5] K. Mori, M. A. Famiano, T. Kajino, T. Suzuki et al., %, J. Hidaka, M. Honma, K. Iwamoto, K. Nomoto and T. Otsuka, ApJ. 833 (2016) 179. \noindent [6] H. Schatz et al., Nature 505 (2014) 62. \noindent [7] N. Tsunoda, T. Otsuka, K.Shimizu, M. Hjorth-Jensen, K, Takayanagi and T. Suzuki, Phys. Rev. C (2017) to be published. \noindent [8] C. Sullivan et al., ApJ. 816 (2016) 44. \noindent [9] Y. Tsunoda et al, Phys. Rev. C 89 (2014) 031301(R).} %%% %%% End of abstract. %%% \end{document}

Primary author

Prof. Toshio Suzuki (Nihon University)

Co-authors

Dr Naofumi Tsunoda (Center for Nuclear Study, The University of Tokyo) Prof. Noritaka Shimizu (Center for Nuclear Study, The University of Tokyo) Prof. Takaharu Otsuka (Department of Physics, The University of Tokyo) Dr Yusuke Tsunoda (Center for Nuclear Study, The University of Tokyo)

Presentation materials