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We study the shape coexistence of differently deformed states within Si using shell-model and beyond-mean-field techniques. Experimentally, Si exhibits shape coexistence between an oblate ground state and an excited prolate structure. The oblate rotational band is described well within the shell using the USDB interaction. However, for the prolate band, a modification of this interaction is required, lowering the single-particle energy of the orbit. Furthermore, we explore the possibility of a superdeformed configuration in Si. Our calculations, spanning both the and shells, rule out the existence of a superdeformed bandhead within an excitation energy range of 10-20 MeV.

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