S-wave scattering lengths for the Be 7 +p system from an R-matrix analysis

S. N. Paneru, C. R. Brune, R. Giri, R. J. Livesay, U. Greife, J. C. Blackmon, D. W. Bardayan, K. A. Chipps, B. Davids, D. S. Connolly, K. Y. Chae, A. E. Champagne, C. Deibel, K. L. Jones, M. S. Johnson, R. L. Kozub, Z. Ma, C. D. Nesaraja, S. D. Pain, F. SarazinJ. F. Shriner, D. W. Stracener, M. S. Smith, J. S. Thomas, D. W. Visser, C. Wrede

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8 Scopus citations

Abstract

The astrophysical S factor for the radiative proton capture reaction on Be7 (S17) at low energies is affected by the s-wave scattering lengths. We report the measurement of elastic and inelastic scattering cross sections for the Be7+p system in the center-of-mass energy range 0.474-2.740 MeV and center-of-mass angular range 70-150. A radioactive Be7 beam produced at Oak Ridge National Laboratory's (ORNL) Holifield Radioactive Ion Beam Facility was accelerated and bombarded a thin polypropylene (CH2)n target. Scattered ions were detected in the segmented Silicon Detector Array. Using an R-matrix analysis of ORNL and Louvain-la-Neuve cross-section data, the s-wave scattering lengths for channel spins 1 and 2 were determined to be 17.34-1.33+1.11 and -3.18-0.50+0.55 fm, respectively. The uncertainty in the s-wave scattering lengths reported in this work is smaller by a factor of 5-8 compared to the previous measurement, which may reduce the overall uncertainty in S17 at zero energy. The level structure of B8 is discussed based upon the results from this work. Evidence for the existence of 0+ and 2+ levels in B8 at 1.9 and 2.21 MeV, respectively, is observed.

Original languageEnglish
Article number045807
JournalPhysical Review C
Volume99
Issue number4
DOIs
StatePublished - Apr 30 2019

Funding

We are grateful to R. J. deBoer for his assistance with azure 2. We thank D. R. Phillips for taking part in constructive discussions. This work was supported in part by the U.S. Department of Energy under Grants No. DE-NA0002905, No. DE-NA0003883, No. DE-FG02-88ER40387, and No. DE-FG02-93ER40789 and Contract No. DE-AC05-00OR22725 (ORNL). D.W.B. acknowledges support from the NSF under Grant No. PHY-1713857. B.D. acknowledges support from the NSERC, Canada. The work of K.Y.C. was supported in part by National Research Foundation of Korea (NRF) Grants No. NRF-2016R1A5A1013277 and No. NRF-2013M7A1A1075764 funded by the Korean government (MEST). This research used resources of the Holifield Radioactive Ion Beam Facility, which was a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The authors are grateful to the staff of the HRIBF whose hard work made the experiment possible.

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