4.7 Article

Radioactive Heating Rate of r-process Elements and Macronova Light Curve

Journal

ASTROPHYSICAL JOURNAL
Volume 891, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/ab6a98

Keywords

Compact binary stars; Gravitational wave astronomy; R-process

Funding

  1. Lyman Spitzer Jr. Fellowship at the Department of Astrophysical Sciences, Princeton University
  2. Israel Science Foundation [1114/17]
  3. ERC consolidator grant (JetNS)

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We study the heating rate of r-process nuclei and thermalization of decay products in neutron star merger ejecta and macronova (kilonova) light curves. Thermalization of charged decay products, i.e., electrons, alpha-particles, and fission fragments, is calculated according to their injection energy. The gamma-ray thermalization processes are also properly calculated by taking the gamma-ray spectrum of each decay into account. We show that the beta-decay heating rate at later times approaches a power-law decline as proportional to t(-2.8), which agrees with the result of Waxman et al. We present a new analytic model to calculate macronova light curves, in which the density structure of the ejecta is accounted for. We demonstrate that the observed bolometric light curve and temperature evolution of the macronova associated with GW170817 are reproduced well by the beta-decay heating rate with the solar r-process abundance pattern. We interpret the break in the observed bolometric light curve around a week as a result of the diffusion wave crossing a significant part of the ejecta rather than a thermalization break. We also show that the time-weighted integral of the bolometric light curve (Katz integral) is useful to provide an estimate of the total r-process mass from the observed data, which is independent of the highly uncertain radiative transfer. For the macronova in GW170817, the ejecta mass is robustly estimated as 0.05 M for A(min) <= 72 and 85 <= A(min) <= 130 with the solar r-process abundance pattern. The code for computation of the heating rate and light curve for given initial nuclear abundances is publicly available.

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