Abstract
We have described the positive parity rotational-like band structure J π = 1 2 +, 3 2 +, 5 2 + … , persisting in most odd-mass In nuclei (107 ≦ A ≦ 119), in both a deformed representation (Nilsson model) with extensive band-mixing calculations as well as in a spherical representation (particle-anharmonic-core coupling). Also, electromagnetic properties (static, dynamic) are described in both representations. The results from both types of calculation are compared extensively and possible numerical and analytic equivalences are pointed out (i.e. energy spectra, E2 transition rates and quadrupole moments, spectroscopic factors).
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