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In physics, a deformed nucleus refers to a nucleus that is not perfectly spherical. Instead, it has a shape that is elongated, resembling a cigar or a football. This deformation occurs in nuclei that are far from the stable "doubly magic" regions.1

The collective model explains this phenomenon by suggesting that nucleons within the nucleus can interact in a way that collectively alters the nuclear shape. These cigar-shaped nuclei are commonly found in specific atomic mass ranges. The collective model has been successful in predicting and correlating the properties of these deformed nuclei, including their rotational excitations.1

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