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

The neutrino process in supernova nucleosynthesis

19 Jun 2017, 12:40
20m
Sala conferenze (Laboratori Nazionali del Sud)

Sala conferenze

Laboratori Nazionali del Sud

Via S. Sofia 62 I-95123 Catania Italy
Oral Neutrinos and weak interaction in astrophysics r-process 1

Speaker

Mr Andre Sieverding (Technische Universität Darmstadt)

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{The $\nu$ process in supernova nucleosynthesis}\\[3mm] %%% %%% Authors and affiliations are next. The presenter should be %%% underlined as shown below. %%% \AUTHORS{\underline{A. Sieverding$^{1}$}, G. Mart\'inez Pinedo$^{1,2}$, K. Langanke$^{1,2}$, A. Heger$^{3}$ } %%% {\small \it \AFFILIATION{1}{Institut f\"ur Kernphysik (Theoriezentrum), Technische Universit\"at Darmstadt, Germany} \AFFILIATION{2}{Gesellschaft f\"ur Schwerionenforschung Darmstadt (GSI), Darmstadt, Germany} \AFFILIATION{3}{Monash Centre for Astrophysics, School of Physics and Astronomy, Monash University, Australia} } %%% \vspace{12pt} % Do not modify % Enter contact e-mail address here. \centerline{Contact email: {\it asiever@theorie.ikp.physik.tu-darmstadt.de}} \vspace{18pt} % Do not modify \end{center} %%% %%% Abstract proper starts here. %%% Core-collapse supernova explosions are accompanied by large neutrino fluxes emitted from the cooling stellar core. The neutrino irradiation affects the shock-heated nucleosynthesis in the $\nu$ process \cite{Heger.Kolbe.ea:2005} affecting the final composition of the ejecta.\\ Since neutrino energies are relatively high cross sections for the reactions are mainly sensitive to collective excitations and can be calculated fairly well with relatively simple nuclear models that allow calculations for a large range of target nuclei. As state-of-the-art supernova simulations tend to predict neutrino energies to be lower than expected in the past, charged current channels like $\nu_e$ absorption gain in relative importance. Often they are determined by a few low-energy Fermi and Gamow-Teller transitions, for which strengths are in some cases directly known from experiments or can be inferred from mirror nuclei. In the case of the reaction $^{26}$Mg($\nu_e$,e$^-$) $^{26}$Al for example, that contributes to the production of radioactive $^{26}$Al in supernova explosions, the cross section can be derived from the $B(GT)$ strength measured in (t,$^3$He) charge-exchange reactions \cite{Zegers.Akimune.ea:2006}. \\ For high excitation energies these cross sections can be supplemented by calculations for forbidden transitions. Using a set of neutrino-nucleus cross-sections based on experimental data wherever possible and supplemented by RPA-based theoretical calculations we have performed nucleosynthesis calculations with progenitor and explosion models calculated with the 1D stellar evolution and hydrodynamics code KEPLER as e.g. in \cite{Heger.Kolbe.ea:2005}. We have also investigated the effect that the reduction of expected neutrino energies in recent years has on the $\nu$ process in general. We find that the production of the isotopes that are expected to have contributions from the $\nu$ process is reduced but still in good agreement with observations (see also \cite{Balasi.Langanke.ea:2015}). We also find that the neutrino-induced enhancement of the production of $^{26}$Al is reduced from roughly 20\% to 10\% (see also \cite{Balasi.Langanke.ea:2015,Sieverding.Huther.ea:2015}) and we try to quantify how this $\nu$ process contributes to the uncertainty in the yields of $^{26}$Al. \renewcommand{\section}[2]{}% \bigskip {\small \begin{thebibliography}{1} \bibitem{Heger.Kolbe.ea:2005} A.~{Heger}, E.~{Kolbe}, W.~C. {Haxton}, K.~{Langanke}, G.~{Mart{\'{\i}}nez-Pinedo}, Physics Letters B \textbf{606} 258. (2005) \bibitem{Zegers.Akimune.ea:2006} R.~G.~T. {Zegers}, \emph{et~al.}, Phys. Rev. C \textbf{74}~ 024309 (2006). \bibitem{Balasi.Langanke.ea:2015} K.~G. {Balasi}, K.~{Langanke}, G.~{Mart{\'{\i}}nez-Pinedo}, Progress in Particle and Nuclear Physics \textbf{85} 33 (2015) A. Sieverding, L. Huther, G. Martinez-Pinedo and K. Langanke \bibitem{Sieverding.Huther.ea:2015} A. Sieverding, L. Huther, G. Martinez-Pinedo and K. Langanke, submitted, arXiv:1505.01082 (2015) \end{thebibliography} } %%% %%% End of abstract. %%% \end{document}

Primary author

Mr Andre Sieverding (Technische Universität Darmstadt)

Co-authors

Prof. Alexander Heger (Monash University, Melbourne) Prof. Gabriel Martínez Pinedo (Technische Universität Darmstadt) Prof. Karlheinz Langanke (Helmholtz Center for Heavy Ion research (GSI), Darmstadt)

Presentation materials