Abstract
Two new absolute transition rates are reported for the nucleus144Sm following an (α, α′) Coulomb excitation study. They are B(E3; 3−→ 0+)=(38±3) W.u. and B(E1;3− → 2+)=(2.8±0.4)×10−3 W.u. This large E1 matrix element, along with the previously known B(E1; 1− →+) value support the interpretation of the 1− state in this nucleus as 2-phonon 2+ × 3− excitation. In the frame of the IBM-1 +f-boson model we show the need for a two-body term in the E1 transition operator. Estimates for the strengths of the one and two-body parts of the E1 transition operator are obtained from these experimental data.
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The authors thank R.F. Casten, A. Gelberg, F. Iachello, Dao Tien Khoa, K. Heyde, C. Wesselborg and H. Harter for valuable discussions and S. Harissopulos for his help during the experiments. NVZ thanks Institut für Kernphysik in Köln and AFB thanks both Institut für Kernphysik in Köln and the Kernfysisch Versneller Institut in Groningen for their hospitality during the course of this work. This work has been partially funded by the German Minister of Research and Technology (BMFT) under contract number 060K272.
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Barfield, A.F., von Brentano, P., Dewald, A. et al. Evidence for the two-body nature of theE1 transition operator in the sdf-interacting boson model. Z. Physik A - Atomic Nuclei 332, 29–32 (1989). https://doi.org/10.1007/BF01292577
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DOI: https://doi.org/10.1007/BF01292577