Informing direct neutron capture on tin isotopes near the N=82 shell closure

B. Manning, G. Arbanas, J. A. Cizewski, R. L. Kozub, S. Ahn, J. M. Allmond, D. W. Bardayan, K. Y. Chae, K. A. Chipps, M. E. Howard, K. L. Jones, J. F. Liang, M. Matos, C. D. Nesaraja, F. M. Nunes, P. D. O'Malley, S. D. Pain, W. A. Peters, S. T. Pittman, A. RatkiewiczK. T. Schmitt, D. Shapira, M. S. Smith, L. Titus

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Abstract

Half of the elements heavier than iron are believed to be produced through the rapid neutron-capture process (r process). The astrophysical environment(s) where the r process occurs remains an open question, even after recent observations of neutron-star mergers and the associated kilonova. Features in the abundance pattern of r-process ashes may provide critical insight for distinguishing contributions from different possible sites, including neutron-star mergers and core-collapse supernovae. In particular, the largely unknown neutron-capture reaction rates on neutron-rich unstable nuclei near Sn132 could have a significant impact on the final r-process abundances. To better determine these neutron-capture rates, the (d,p) reaction has been measured in inverse kinematics using radioactive ion beams of Sn126 and Sn128 and a stable beam of Sn124 interacting with a (CD2)n target. An array of position-sensitive silicon strip detectors, including the Super Oak Ridge Rutgers University Barrel Array, was used to detect light reaction products. In addition to the present measurements, previous measurements of Sn130,132(d,p) were reanalyzed using state-of-the-art reaction theory to extract a consistent set of spectroscopic factors for (d,p) reactions on even tin nuclei between the heaviest stable isotope Sn124 and doubly magic Sn132. The spectroscopic information was used to calculate direct-semidirect (n,γ) cross sections, which will serve as important input for r-process abundance calculations.

Original languageEnglish
Article number041302
JournalPhysical Review C
Volume99
Issue number4
DOIs
StatePublished - Apr 18 2019

Funding

This Rapid Communication was supported, in part, by the U.S. Department of Energy under Contracts No. DE-FG52-08NA28552 and No. DE-NA0002132 (Rutgers), No. DE-FG02-96ER40983 (UTK), No. DE-SC0001174 (UTK), No. DE-FG02-96ER40955 (TTU), No. DE-AC05-00OR22725 (ORNL), the National Science Foundation under Contracts No. NSF-PHY-1067906, No. NSF-PHY-1404218 (Rutgers), and No. NSF-PHY-1403906 (MSU), the TORUS: Theory of Reactions for Unstable iSotopes a DOE Office of Science Topical Collaboration for Nuclear Theory, and the National Research Foundation of Korea (Grants No. NRF-2016K1A3A7A09005579 and No. NRF-2016R1A5A1013277). This research used resources of the Holifield Radioactive Ion Beam Facility, which was a DOE Office of Science User Facility (HRIBF) operated by the Oak Ridge National Laboratory. The authors are grateful to the HRIBF facility operations staff who made the measurements possible.

FundersFunder number
National Science FoundationNSF-PHY-1404218, 1713857, NSF-PHY-1403906, 1812316, 1811815
U.S. Department of EnergyDE-AC05-00OR22725, DE-FG52-08NA28552
Oak Ridge National Laboratory
Midwestern State University
National Research Foundation of KoreaNRF-2016K1A3A7A09005579

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