Excitations of the α cluster in A=6 and 7 nuclei

T. Yamagata, S. Nakayama, H. Akimune, M. Fujiwara, K. Fushimi, M. B. Greenfield, K. Hara, K. Y. Hara, H. Hashimoto, K. Ichihara, K. Kawase, M. Kinoshita, Y. Matsui, K. Nakanishi, M. Tanaka, H. Utsunomiya, and M. Yosoi
Phys. Rev. C 69, 044313 – Published 21 April 2004

Abstract

The isovector giant dipole resonance (GDR) of an α cluster in Li6 and Li7, and its analogs in Be6,7 and He6,7 were searched for by using the Li6,7(p,p), Li6,7(He3,t), and Li6,7(Li7,Be7) reactions at the incident energies of 300, 450, and 455MeV, respectively. New dipole resonances were found at Ex=27.0±1.5MeV in Li6 and at Ex=29.0±1.5MeV in Li7, both with widths (full width at half maximum) of 12±2MeV. In He6, Be6, He7, and Be7, the dipole resonances with a width of 12±2MeV were observed at Ex=24.0±1.5,23.5±1.5,18.0±1.5, and 28.0±1.5MeV, respectively. The resonance shapes were reproduced well with the GDR shape observed in the He4(γ,n) reactions. The averaged value for the ratios of the resonance cross section in A=6 to that in A=7 for each element was 1.2±0.3. The averaged value for the ratios of the resonance cross section to the GDR cross section in the respective target nuclei was 0.44±0.08, which was consistent with the ratios of the GDR cross section in He4 to that in Li6,7 reported in the photonuclear reactions. The excitation energies for the dipole resonances in A=6 and 7 nuclei relative to the separation energies of an α particle in Li6 and Li7, respectively, agreed well with the excitation energy for the GDR in He4(26MeV). We conclude that the resonances observed in Li6,7 are consistent with the GDR of the α cluster and the resonances in He6,7 and Be6,7 are consistent with the analogs of the GDR in the α cluster. The Q value for the excitation of the GDR of the α cluster in A=7 nuclei is deeper by 1.6±0.3MeV on the average than that in A=6.

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  • Received 25 December 2003

DOI:https://doi.org/10.1103/PhysRevC.69.044313

©2004 American Physical Society

Authors & Affiliations

T. Yamagata1,*, S. Nakayama2, H. Akimune1, M. Fujiwara3,4, K. Fushimi2, M. B. Greenfield5, K. Hara3, K. Y. Hara1, H. Hashimoto3, K. Ichihara2, K. Kawase3, M. Kinoshita1, Y. Matsui2, K. Nakanishi3, M. Tanaka6, H. Utsunomiya1, and M. Yosoi7

  • 1Department of Physics, Konan University, Kobe 658-8501, Japan
  • 2Department of Physics, University of Tokushima, Tokushima 770-8502, Japan
  • 3Research Center for Nuclear Physics, Osaka University, Osaka 567-0047, Japan
  • 4Advance Science Research Center, JAERI, Ibaragi 319-1195, Japan
  • 5Department of Physics, International Christian University, Tokyo 113-0033, Japan
  • 6Kobe Tokiwa College, Kobe 654-0838, Japan
  • 7Department of Physics, Kyoto University, Kyoto 606-8502, Japan

  • *Electronic address: yamagata@center.konan-u.ac.jp

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Vol. 69, Iss. 4 — April 2004

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