We investigate the influence of density, interaction and harmonic confinement on the superfluid to insulator transition (SIT) in disordered fermionic superfluids described by the one-dimensional Hubbard model. We quantify the ground-state single-site entanglement via density-functional theory calculations of the linear entropy. We analyze the critical concentration at which the fully-localized state a special type of localization, with null entanglement emerges. We find that is independent on the interaction, but demands a minimum disorder strength to occur. We then derive analytical relations for as a function of the average particle density for attractive and repulsive disorder. Our results reveal that weak harmonic confinement does not impact the properties of the fully-localized state, which occurs at the same , but stronger confinements may lead the system from the fully-localized state to the ordinary localization.

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