4.7 Article

Nebular emission from lanthanide-rich ejecta of neutron star merger

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 506, Issue 4, Pages 5863-5877

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stab1975

Keywords

neutron star mergers

Funding

  1. Japan Society for the Promotion of Science (JSPS) [20K14513]
  2. Grants-in-Aid for Scientific Research [20K14513] Funding Source: KAKEN

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The study of the nebular phase of lanthanide-rich ejecta from a neutron star merger provides insights into the cooling mechanisms and stability of ionization and thermal balance over time. Both permitted and forbidden lines contribute to the cooling rate of Ndii and Ndiii, with the kinetic temperature and ionization degree stabilizing after a thermalization break. The emission-line nebular spectrum of pure Nd ejecta exhibits distinctive peak structures.
The nebular phase of lanthanide-rich ejecta of a neutron star merger (NSM) is studied by using a one-zone model, in which the atomic properties a represented by a single species, neodymium (Nd). Under the assumption that beta-decay of r-process nuclei is the heat and ionization source, we solve the ionization and thermal balance of the ejecta under non-local thermodynamic equilibrium. The atomic data including energy levels, radiative transition rates, collision strengths, and recombination rate coefficients are obtained by using atomic structure codes, grasp2k and hullac. We find that both permitted and forbidden lines roughly equally contribute to the cooling rate of Ndii and Ndiii at the nebular temperatures. We show that the kinetic temperature and ionization degree increase with time in the early stage of the nebular phase, while these quantities become approximately independent of time after the thermalization break of the heating rate because the processes relevant to the ionization and thermalization balance are attributed to two-body collision between electrons and ions at later times. As a result, in spite of the rapid decline of the luminosity, the shape of the emergent spectrum does not change significantly with time after the break. We show that the emission-line nebular spectrum of the pure Nd ejecta consists of a broad structure from to with two distinct peaks around and .

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