Neutron-Capture Elements in the Early Galaxy: Insights from a Large Sample of Metal-poor Giants

By D. Burris, C. Pilachowski, T. Armandroff, C. Sneden, J. Cowan, H. Roe. 2000

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New abundances for neutron-capture (n-capture) elements in a large sample of metal-poor giants from the Bond survey are presented. The spectra were acquired with the KPNO 4 m echelle and coudé feed spectrographs, and have been analyzed using LTE fine-analysis techniques with both line analysis and spectral synthesis. Abundances of eight n-capture elements (Sr, Y, Zr, Ba, La, Nd, Eu, and Dy) in 43 stars have been derived from blue (λλ4070-4710, R ~ 20,000, S/N ratio ~ 100-200) echelle spectra and red (λλ6100-6180, R ~ 22,000, S/N ratio ~ 100-200) coudé spectra, and the abundance of Ba only has been derived from the red spectra for an additional 27 stars. Overall, the abundances show clear evidence for a large star-to-star dispersion in the heavy element-to-iron ratios. This condition must have arisen from individual nucleosynthetic events in rapidly evolving halo progenitors that injected newly manufactured n-capture elements into an inhomogeneous early Galactic halo interstellar medium. The new data also confirm that at metallicities [Fe/H] ≲ -2.4, the abundance pattern of the heavy (Z ≥ 56) n-capture elements in most giants is well-matched to a scaled solar system r-process nucleosynthesis pattern. The onset of the main r-process can be seen at [Fe/H] ≈ -2.9; this onset is consistent with the suggestion that low mass Type II supernovae are responsible for the r-process. Contributions from the s-process can first be seen in some stars with metallicities as low as [Fe/H] ~ -2.75 and are present in most stars with metallicities [Fe/H] > -2.3. The appearance of s-process contributions as metallicity increases presumably reflects the longer stellar evolutionary timescale of the (low-mass) s-process nucleosynthesis sites. The lighter n-capture elements (Sr-Y-Zr) are enhanced relative to the heavier r-process element abundances. Their production cannot be attributed solely to any combination of the solar system r- and main s-processes, but requires a mixture of material from the r-process and from an additional n-capture process that can operate at early Galactic time. This additional process could be the weak s-process in massive (~25 M☉) stars, or perhaps a second r-process site, i.e., different from the site that produces the heavier (Z ≥ 56) n-capture elements.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/d79eaac451dd11a72b72d0d5e250f4c3231648a4

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In Astronomy and Astrophysics

  1. Timothy C. Beers
  2. C. Sneden
  3. Roberto Gallino
  4. A. Frebel
  5. J. Cowan
  6. Martin Asplund
  7. J. Norris
  8. P. Hopkins

In Nuclear and High Energy Physics

  1. Stan Woosley
  2. Alexander Heger
  3. Hans-Thomas Janka
  4. C. Sneden
  5. E. Quataert
  6. Bernhard Müller
  7. S. Wanajo
  8. P. Hopkins

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