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Phys. Rev. C 80, 044317 (2009) [7 pages]

Proton decay from the isoscalar giant dipole resonance in 58Ni

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M. Hunyadi1,2, H. Hashimoto3, T. Li1, H. Akimune4, H. Fujimura3, M. Fujiwara3, Z. Gácsi2, U. Garg1, K. Hara3, M. N. Harakeh5,6, J. Hoffman1, M. Itoh3, T. Murakami7, K. Nakanishi3, B. K. Nayak1, S. Okumura3, H. Sakaguchi7, S. Terashima7, M. Uchida7, Y. Yasuda7, and M. Yosoi7
1University of Notre Dame, Notre Dame, Indiana 46556, USA
2Institute of Nuclear Research of the Hungarian Academy of Sciences, H-4001 Debrecen, Hungary
3Research Center for Nuclear Physics, Osaka University, Mihogaoka 10-1, Ibaraki, 567-0047 Osaka, Japan
4Department of Physics, Konan University, Kobe 658-8501, Japan
5Kernfysisch Versneller Instituut, University of Groningen, 9747 AA Groningen, The Netherlands
6GANIL, CEA/DSM CNRS/IN2P3, F-14076 Caen, France
7Department of Physics, Kyoto University, Kyoto 606-8502, Japan

Received 24 June 2009; published 15 October 2009

Proton decay from the 3ω isoscalar giant dipole resonance (ISGDR) in 58Ni has been measured using the (α,α'p) reaction at a bombarding energy of 386 MeV to investigate its decay properties. We have extracted the ISGDR strength under the coincidence condition between inelastically scattered α particles at forward angles and decay protons emitted at backward angles. Branching ratios for proton decay to low-lying states of 57Co have been determined, and the results compared with predictions of recent continuum-RPA calculations. The final-state spectra of protons decaying to the low-lying states in 57Co were analyzed for a more detailed understanding of the structure of the ISGDR. It is found that there are differences in the structure of the ISGDR as a function of excitation energy.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.80.044317
DOI:
10.1103/PhysRevC.80.044317
PACS:
24.30.Cz, 23.50.+z, 25.55.Ci, 27.40.+z