Abstract
The level structure of the 143Sm and 145Gd nuclei has been studied using the 142Nd (α, 3nγ) 143Sm and 144Sm(α, 3nγ) 145Gd reactions. Singles γ-ray, γ-γ coincidence spectra, angular and time distributions with respect to the beam burst have been measured. Gamma transitions between excited states with spin values up to 29 2 in 143Sm and up to 21 2 in 145Gd have been observed. The observed level structure in both nuclei can be explained if the neutron-hole is coupled to the doubly even core excitations. The coupling of the h 11 2 neutron-hole with the 2 + and 3 − vibrations is calculated in the weak and intermediate coupling models. The results obtained in these calculations are in reasonably good agreement with the experimental data. The energies of the three-particle states, being the result of the coupling of the h 11/2 neutron-hole with the two-proton excitations in the core, are nicely reproduced in the calculations. Empirical values of the two-body interaction matrix elements have been used. However, the three-particle calculation does not explain the existence of the 30 ms 23 2 − isomeric level in the 143Sm nucleus.
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