In this paper, we study the linear stability of self-interacting boson stars in the nonrelativistic limit of the Einstein-Klein-Gordon theory. For this purpose, based on a combination of analytic and numerical methods, we determine the behavior of general linear perturbations around the stationary and spherically symmetric solutions of the Gross-Pitaevskii-Poisson system. In particular, we conclude that ground state configurations are linearly stable if the self-interaction is repulsive, whereas there exists a state of maximum mass that divides the stable and the unstable branches in case the self-interaction is attractive. Regarding the excited states, they are in general unstable under generic perturbations, although we identify a stability band in the first excited states of the repulsive theory. This result is independent of the mass of the scalar field and the details of the self-interaction potential, and it is in contrast to the situation of vanishing self-interaction, in which excited states are always unstable.
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Nambo et al. (2024) studied this question.
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