2021
DOI: 10.1002/asna.202113941
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Stability of multistate configurations of fuzzy dark matter

Abstract: We study the stability properties of multistate configurations of the Schrödinger-Poisson system without self-interaction, with monopolar and first dipolar components (1,0,0) + (2,1,0). We show that these studied configurations are stable using numerical simulations and using criteria of stationarity, unitarity, and time dependence consistency. The study covers a range of states with a monopolar to dipolar mass ratio of between 47 and 0.17. The astrophysical implication of this result is that this type of conf… Show more

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Cited by 5 publications
(2 citation statements)
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“…An excited monopole scalar BS, which is unstable against decaying to a fundamental BS [20], is stabilized by adding a sufficiently large fundamental monopole BS of a second field [21] (see also [22][23][24]). In the same spirit, for the non-relativistic BSs of the Schrödinger-Poisson system, a dipole configuration is stabilized by adding a sufficiently large fundamental monopole [25] (see also [26]). These examples turn out to be illustrations of a stabilization mechanism, as we shall discuss.…”
mentioning
confidence: 99%
“…An excited monopole scalar BS, which is unstable against decaying to a fundamental BS [20], is stabilized by adding a sufficiently large fundamental monopole BS of a second field [21] (see also [22][23][24]). In the same spirit, for the non-relativistic BSs of the Schrödinger-Poisson system, a dipole configuration is stabilized by adding a sufficiently large fundamental monopole [25] (see also [26]). These examples turn out to be illustrations of a stabilization mechanism, as we shall discuss.…”
mentioning
confidence: 99%
“…The stability of self-gravitating scalar field configurations have been widely studied as it is an important characteristic to determine their viability as astrophysical objects. In [40,41] and [42,43] it was shown that there exist stable -boson stars with n = + 1, under radial perturbations, in the relativistic and Newtonian limit respectively. On the other hand, -boson stars are unstable under 3D perturbations, however it is possible to stabilize them by adding a sufficiently large fundamental, n = 1, = 0 boson star [44].…”
Section: Jcap09(2023)031mentioning
confidence: 99%