Neutron decay from the giant resonance via the B10(e,e'n) reaction

H. Ueno, T. Kawamura, T. Suzuki, H. Taneichi, T. Saito, T. Nakagawa, K. Kino, T. Nakagawa, Y. Matsuura, and M. Higuchi
Phys. Rev. C 80, 064609 – Published 16 December 2009

Abstract

The cross sections and angular correlations for neutron decay into various states in the residual nucleus following the B10(e,e'n) reaction have been measured over the excitation energy range of 18–33 MeV at an effective momentum transfer of 0.56 fm1. In the giant resonance, neutron emission leads to the population of two higher excited states in addition to the ground-state transition: 6.97 MeV 7/2(n5) and 11.70 MeV 7/2+12.06 MeV 3/2(n6,7). This is the first observation of the neutron population of these states. The angular correlations for n0 show a strong forward-backward asymmetry, which suggests interference from a transition with the opposite parity to E1. The angular correlations for n5 and n6,7 have a peak shift of about 50° at lower excitation energy and recover above about 24 and 25 MeV for n5 and n6,7, respectively. Their patterns are considerably different from that for n0. The angular correlations for each transition were fitted with a Legendre polynomial. The longitudinal-transverse interference coefficient C2/A0 is negligible for all populations. For n0 decay, all Legendre coefficients bi are positive, but b2 and b3 for the n5 and n6,7 decays are negative at lower excitation energy, and the latter causes a shift of the forward peak. The negative values may come from the signs of the phase differences of cosδ21 and cosδ20. The B10(e,e'n) cross section measured up to Ex~32 MeV agrees well with that of B10(γ,n), except for a peak at 23 MeV of the giant resonance. In comparison with shell-model calculations, the partial cross section for n0 is sizable up to higher excitation energy, and predicted large partial cross sections populating the 6.97 MeV 7/2 and 11.70 MeV 7/2+12.06 MeV 3/2 states in the giant resonance were not observed.

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  • Received 27 August 2009

DOI:https://doi.org/10.1103/PhysRevC.80.064609

©2009 American Physical Society

Authors & Affiliations

H. Ueno, T. Kawamura*, T. Suzuki, and H. Taneichi

  • Department of Physics, Yamagata University, Kojirakawa, Yamagata 990-8560, Japan

T. Saito, T. Nakagawa§, and K. Kino

  • Laboratory of Nuclear Science, Tohoku University, Mikamine, Taihaku-ku, Sendai 982-0826, Japan

T. Nakagawa

  • Department of Physics, Tohoku University, Aramaki, Aoba-ku, Sendai 980-8578, Japan

Y. Matsuura and M. Higuchi

  • Faculty of Engineering, Tohoku Gakuin University, Chuo, Tagajo 985-8537, Japan

  • *Current Address: Iwanuma City Office, Sakura, Iwanuma 989-2480, Japan.
  • Current Address: Research Center for Nuclear Physics, Osaka University, Ibaraki 567-0047, Japan.
  • Current address: Department of Physics, Yamagata University, Kojirakawa, Yamagata 990-8560, Japan.
  • §Current address: Toshiba Corporation, Shinsugita, Isogo-ku, Yokohama 235-8532, Japan.
  • Current address: Graduate School of Engineering, Hokkaido University, Kita 13 Nishi 8, Sapporo 060-8628, Japan.
  • Current address: Rise Corporation, 3-9-15, Tsutsujigaoka, Miyagino-ku, Sendai 983-0852, Japan.

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Issue

Vol. 80, Iss. 6 — December 2009

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