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The r-Process: History, Required Conditions, Astrophysical Sites, and Observations

Friedrich-Karl Thielemann, John J. Cowan

TL;DR

This review traces the history and current understanding of the r-process, combining solar-system residual analyses with site-independent nuclear-physics predictions and a comprehensive survey of proposed astrophysical sites. It emphasizes that a single r-process site cannot explain the entire solar pattern and that multiple environments—most notably neutron-star mergers for the main, and magneto-rotational supernovae or collapsars for additional components—shape the observed abundances. The authors compare predictions to observations, including kilonovae and metal-poor stars, and discuss galactic chemical evolution and cosmochronology to assess the timing and frequency of contributing events. The work highlights the need for improved nuclear data and continued multi-messenger observations to identify the dominant sites and their roles across cosmic time.

Abstract

This review of the rapid-neutron-capture (i.e. r-) process starts with determining the Solar System r-abundance pattern via first obtaining (and subtracting) the contribution from the slow-neutron capture (s-) process. We emphasize the extensive work in this area by our late colleague Roberto Gallino and continue in an overview, concentrating on attempts to reproduce the solar r-process pattern with historical site-independent approaches, based on nuclear physics far from stability. In a second step we address the existing proposals for astrophysical sites. Among stellar observations we start with available observations of individual events before analyzing low-metallicity stars, which witness r-process contributions in the early Galaxy. We conclude with a comparison of observations and model predictions, focusing on our present ability to identify the responsible individual astrophysical sites by their imprint in Galactic evolution.

The r-Process: History, Required Conditions, Astrophysical Sites, and Observations

TL;DR

This review traces the history and current understanding of the r-process, combining solar-system residual analyses with site-independent nuclear-physics predictions and a comprehensive survey of proposed astrophysical sites. It emphasizes that a single r-process site cannot explain the entire solar pattern and that multiple environments—most notably neutron-star mergers for the main, and magneto-rotational supernovae or collapsars for additional components—shape the observed abundances. The authors compare predictions to observations, including kilonovae and metal-poor stars, and discuss galactic chemical evolution and cosmochronology to assess the timing and frequency of contributing events. The work highlights the need for improved nuclear data and continued multi-messenger observations to identify the dominant sites and their roles across cosmic time.

Abstract

This review of the rapid-neutron-capture (i.e. r-) process starts with determining the Solar System r-abundance pattern via first obtaining (and subtracting) the contribution from the slow-neutron capture (s-) process. We emphasize the extensive work in this area by our late colleague Roberto Gallino and continue in an overview, concentrating on attempts to reproduce the solar r-process pattern with historical site-independent approaches, based on nuclear physics far from stability. In a second step we address the existing proposals for astrophysical sites. Among stellar observations we start with available observations of individual events before analyzing low-metallicity stars, which witness r-process contributions in the early Galaxy. We conclude with a comparison of observations and model predictions, focusing on our present ability to identify the responsible individual astrophysical sites by their imprint in Galactic evolution.
Paper Structure (29 sections, 7 equations, 24 figures)

This paper contains 29 sections, 7 equations, 24 figures.

Figures (24)

  • Figure 1: Solar System abundances $Y$, scaled to $Y$(Si)=10$^6$ from Cowan.Sneden.ea:2021. Abundances are compiled from meteorite measurements Lodders19Lodders:2021 and solar spectra Asplund.Grevesse.ea:2009Asplund.Amarsi.ea:2021 and are indicative of the values at time of formation of the Solar System.
  • Figure 2: Roberto Gallino (left, to whom this volume is dedicated) in animated conversation with Franz Käppeler (right) during a scientific meeting in Basel, Switzerland in October 2011
  • Figure 3: A breakdown of the heavy neutron-capture elements into individual s- and r-process contributions. Scale based upon log $\epsilon$ = 12 for the element H; from Cowan.Thielemann:2004.
  • Figure 4: Solar r-process abundances (residuals) from Cowan.Thielemann.Truran:1991 and Goriely:1999.
  • Figure 5: Three r-process paths for $n_n=10^{20}$cm$^{-3}$ (blue), $n_n=10^{23}$cm$^{-3}$ (red), and $n_n=10^{26}$cm$^{-3}$ (green) and the same $T=1.35\times 10^9$K. Inserts show abundances attained after 1.2, 1.6, and 2.5s for the different conditions, in all cases starting with a seed nucleus at $Z=26$. The bottom line indicates for which nuclei experimental beta-decay half lives existed at that time ($^{79}$Cu, $^{80}$Zn, $^{81}$Ga, $^{91,92}$Br, $^{97-100}$Rb, $^{130}$Cd, $^{131}$In, Gill.Casten.ea:1986Kratz.Gabelmann.ea:1986. Due to the different distances of the path from stability (with declining beta-decay half-lives), comparable timescales allow for different endpoints in $A$.
  • ...and 19 more figures