Strong multistep interference effects in C12(d,p) to the 9/21+ state in C13

N. Keeley, K. W. Kemper, and K. Rusek
Phys. Rev. C 92, 054618 – Published 25 November 2015

Abstract

The population of the 9.50 MeV 9/21+ resonance in C13 by single-neutron transfer reactions is expected to be dominated by the two-step route through the C12 21+ (4.44 MeV) state, with another possible contribution via the strongly excited 31 (9.64 MeV) resonance in C12. However, we find that a good description of the angular distribution for population of this state via the C12(d,p)C13 reaction is only possible when both direct 01+g9/2 and two-step (via the 4.44 MeV C12 21+ state) 21+d5/2 paths are included in a coupled reaction channel calculation. While the calculated angular distribution is almost insensitive to the presence of the two-step path via the 9.64 MeV C12 31 resonance, despite a much greater contribution to the wave function from the 31f7/2 configuration, its inclusion is required to fit the details of the experimental angular distribution. The very large interference between the various components of the calculations, even when these are small, arises through the “kinematic” effect associated with the different transfer routes.

  • Figure
  • Figure
  • Received 6 October 2015

DOI:https://doi.org/10.1103/PhysRevC.92.054618

©2015 American Physical Society

Authors & Affiliations

N. Keeley1,*, K. W. Kemper2, and K. Rusek3

  • 1National Centre for Nuclear Research, ul. Andrzeja Sołtana 7, 05-400 Otwock, Poland
  • 2Department of Physics, Florida State University, Tallahassee, Florida 32306, USA
  • 3Heavy Ion Laboratory, University of Warsaw, ul. Pasteura 5a, 02-093, Warsaw, Poland

  • *nicholas.keeley@ncbj.gov.pl

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Vol. 92, Iss. 5 — November 2015

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