Coulomb energy differences in T = 1 mirror rotational bands in 50Fe and 50Cr
- D. Bazzacco
- B. Rubio
- J. Sanchez-Solano
- F. Brandolini
- G. de Angelis
- M. A. Bentley
- Andrea Vitturi
- R. Menegazzo
- C. Chandler
- T. Martinez
- Andrés P. Zuker
- S. M. Lenzi
- W. von Oertzen
- E. Farnea
- C. A. Kalfas
- C. A. Ur
- J. Garces-Narro
- H Eberth
- Roberto Vicençotto Ribas
- P. G. Bizzeti
- Roberto Isocrate
- Johan Nyberg
- M. Axiotis
- O. Thelen
- S. Lunardi
- T. Klug
- Gabriel Martínez-Pinedo
- D. R. Napoli
- Matthias Weiszflog
- H. Grawe
- P. von Brentano
- A. M. Bizzeti-Sona
- D. Bucurescu
- A. Gadea
- P. Spolaore
- Alejandro Algora
- Zs. Podolyák
- D. T. Joss
- T. J. Lampman
- N. Marginean
- Alfredo Poves
- J. A. Cameron
- M. De Poli
- T. Steinhardt
- W. Gelletly
- C. Rossi Alvarez
- Dimitar Tonev
- A. Dewald
- N. Belcari
DOIAbstract
Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground state band up to the state J(pi) = 11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations, incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model space
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