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Suppression of Gamow-Teller and M1 transitions in deformed mirror nuclei 25Mg and 25Al
Authors:Y Shimbara  Y Fujita  T Adachi  G P A Berg  H Fujita  K Fujita  I Hamamoto  K Hatanaka  J Kamiya  K Nakanishi  Y Sakemi  Y Shimizu  M Uchida  T Wakasa  M Yosoi
Institution:(1) Department of Physics, Osaka University, 560-0043 Osaka, Toyonaka, Japan;(2) Research Center for Nuclear Physics, Osaka University, 567-0047 Osaka, Ibaraki, Japan;(3) Kernfysisch Versneller Instituut, Zernikelaan 25, 9747 AA Groningen, The Netherlands;(4) Division of Mathematical Physics, LTH, University of Lund, P.O. Box 118, S-22100 Lund, Sweden;(5) Department of Physics, Kyoto University, 606-8502 Kyoto, Sakyo, Japan
Abstract:The mirror nuclei 25Mg and 25Al are expected to have very similar structures. The Gamow-Teller (GT) transitions from the $J^{\pi} = 5/2^{ + }$ ground state of 25Mg to the excited states in 25Al were studied by high-resolution measurements of the 25Mg( $^3{\rm He},t$ ) charge-exchange reaction at $0^{\circ}$ and at 140 MeV/nucleon. Assuming the usual $\Delta J^{\pi} = 1^{ + }$ selection rule for the spin-isospin-type GT transitions, the states with $J^{\pi} = 3/2^{ + }, 5/2^{ + }$ , and 7/2 + should be excited. However, of the more than ten states with these $J^{\pi}$ values below 6 MeV excitation energy, only the 5/2 + ground state and the 7/2 + , 1.613 MeV state in 25Al were strongly populated, while all other states were strongly suppressed. The analysis of M1 transitions in 25Mg also suggested a very similar feature for the analogous M1 transitions. Both 25Mg and 25Al are known to be largely deformed, and most low-lying states can be interpreted in terms of one-particle quantum numbers in the deformed potential and the associated rotational spectra. The observed suppression can be explained in terms of the K quantum number selection rules that are inherent to axially deformed nuclei.-1Received: 18 July 2003, Published online: 18 December 2003PACS: 21.10.Re Collective levels - 21.60.Ev Collective models - 25.55.Kr Charge-exchange reactions - 27.30. + t $20 \leq A \leq 38$ H. Fujita: Present address: Research Center for Nuclear Physics, Osaka University, Ibaraki, Osaka 567-0047, Japan.J. Kamiya: Present address: Japan Atomic Energy Research Institute, Tokai, Ibaraki 319-1195, Japan.T. Wakasa: Present address: Department of Physics, Kyushu University, Higashi, Fukuoka 812-8581, Japan.
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