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AbstractAbstract
[en] The nucleus 141Gd was investigated at high spins for the first time via the reactions 112Sn(32S,2pn)141Gd at 155 MeV and 112Sn(33S,2p2n)141Gd at 170 MeV. The methods of in-beam γ-ray spectroscopy were used to establish a number of different structures. These include a band assigned as the νi13/2[660]1/2+ intruder in the Nilsson scheme. This is the heaviest nucleus thus far in which this type of intruder band has been identified, and is the first case in which the 13/2+ bandhead has been clearly observed. Cranked shell model (CSM) calculations predict the occurrence of backbends due to h11/2 proton and h9/2 neutron band crossings. Gradual upbends are observed in the experimental alignments, which suggests the interaction strengths are stronger than those predicted by the CSM
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BARYONS, BETA DECAY RADIOISOTOPES, CATIONS, CHARGED PARTICLES, DEFORMATION, ELECTRON CAPTURE RADIOISOTOPES, ELEMENTARY PARTICLES, ENERGY LEVELS, ENERGY RANGE, ENERGY-LEVEL TRANSITIONS, EVEN-ODD NUCLEI, EXCITATION, FERMIONS, GADOLINIUM ISOTOPES, HADRONS, HEAVY ION REACTIONS, HYDROGEN IONS, HYDROGEN IONS 1 PLUS, INTERMEDIATE MASS NUCLEI, IONS, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, MATHEMATICAL MODELS, MEV RANGE, NUCLEAR MODELS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, RADIOISOTOPES, RARE EARTH NUCLEI, SECONDS LIVING RADIOISOTOPES, SPECTROSCOPY, TARGETS
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