Plasma and Fusion Research
Volume 21, 2401005 (2026)
Regular Articles
- 1)
- Université de Mons (UMONS), Mons 700, Belgium
- 2)
- Université Libre de Bruxelles (ULB), Brussels 1050, Belgium
Abstract
The discovery of gravitational waves (GW170817) and the associated kilonova (AT2017gfo) from a neutron star merger in 2017 confirmed the latter as key sites for heavy element production through the r-process. Subsequent observations, including late-time spectra with JWST, have highlighted the need for accurate modeling of kilonova ejecta. In the photospheric phase, atomic level populations can be estimated under LTE using Boltzmann and Saha relations, but about a week after the merger the ejecta enters the nebular phase where non-LTE effects dominate. Modeling nebular spectra therefore requires a detailed treatment of radiative and collisional processes that affect the population of atomic levels. This work focuses on electron-impact excitation in Sr II, a heavy ion relevant for kilonova spectra. Two computational approaches are employed: the Plane-Wave Born approximation within the pseudo-relativistic Hartree-Fock method, and a Distorted Waves method using AUTOSTRUCTURE. The resulting collision strengths are compared against reference R-matrix data to evaluate the accuracy of these approximations and their suitability for large-scale applications to all heavy elements. In addition, radiative parameters for forbidden transitions are computed. These results provide an essential benchmark of approximations that could be used to compute atomic data for nebular-phase kilonova modeling.
Keywords
kilonova, strontium, collision strengths, forbidden transitions, electron-impact excitation, nebular-phase, non-local thermodynamic equilibrium, neutron star merger, plane-wave Born, distorted waves
Full Text
References
- [1] B. Abbott et al., Phys. Rev. Lett. 119, 161101 (2017).
- [2] D. Kasen et al., Nature 551, 80 (2017).
- [3] D. Watson et al., Nature 574, 497 (2019).
- [4] A.J. Levan et al., Nature 626, 737 (2024).
- [5] B.D. Metzger et al., MNRAS 406, 2650 (2010).
- [6] G. Gaigalas et al., Astrophys. J. Suppl. 240, 29 (2019).
- [7] M. Tanaka et al., MNRAS 496, 1369 (2020).
- [8] C.J. Fontes et al., MNRAS 493, 4143 (2020).
- [9] C.J. Fontes et al., MNRAS 519, 2862 (2023).
- [10] A. Flörs et al., MNRAS 524, 3083 (2023).
- [11] J. Deprince et al., A&A 696, A32 (2025).
- [12] Q. Pognan et al., MNRAS 510, 3806 (2022).
- [13] M.M. Kasliwal et al., MNRAS 510, L7 (2022).
- [14] J.H. Gillanders et al., MNRAS 515, 631 (2022).
- [15] L.P. Mulholland et al., MNRAS 532, 2289 (2024).
- [16] R.D. Cowan, The Theory of Atomic Structure and Spectra (University of California Press, 1981).
- [17] N. Badnell, Comput. Phys. Commun. 182, 1528 (2011).
- [18] P.G. Burke, R-Matrix Theory of Atomic Collisions: Application to Atomic, Molecular and Optical Processes (Springer, Berlin, 2011).
- [19] A. Kramida et al., NIST Atomic Spectra Database (ver. 5.12), https://physics.nist.gov/asd (2024).
- [20] C. Moore, Atomic Energy Levels As Derived From the Analyses optical Spectra, Vol. II, National Standard Reference Data Series (National Bureau of Standards, U.S., p. 259 1952).
- [21] J.E. Sansonetti, J. Phys. Chem. Ref. Data 41, 013102 (2012).
- [22] J.H. Gillanders and S.J. Smartt, MNRAS 538, 1663 (2025).
- [23] V. Letchumanan et al., Phys. Rev. A 72, 012509 (2005).
- [24] E. Biémont et al., Eur. Phys. J. D 11, 355 (2000).
- [25] Q. Pognan et al., MNRAS 526, 5220 (2023).
- [26] H. van Regemorter, ApJ 136, 906 (1962).
- [27] T.S. Axelrod, Late time optical spectra from the Ni56 model for Type I Supernovae (California University, Santa Cruz, 1980).
- [28] Q. Pognan et al., MNRAS 536, 2973 (2025).
![[Plasma and Fusion Research]](/PFR/pfr_header.gif)