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Bayesian Constraints on Bosonic Dark Matter in Neutron Stars within a Covariant Density-Functional Equation-of-State Ensemble

Published 29 Sep 2026 in nucl-th and astro-ph.HE | (2609.38055v1)

Abstract: We investigate neutron stars admixed with repulsively self-interacting bosonic dark matter (DM) using current multi-messenger observations. The dark component is modeled as a complex scalar field coupled to baryonic matter only through gravity, allowing dark-core and dark-halo configurations. To quantify baryonic equation-of-state (EOS) uncertainties, we combine a three-dimensional scan over (mχ,λ,Fχ)(m_χ,λ,F_χ) with 27 DDME2-based covariant density-functional EOSs spanning Lsym=30,50,70L_{\rm sym}=30,50,70 MeV and −600≤Qsat≤1000-600\le Q_{\rm sat}\le 1000 MeV. The models are confronted in a Bayesian framework with NICER mass--radius measurements from the Amsterdam and Maryland/Illinois analyses and the GW170817 tidal-deformability constraint. After Bayesian evidence weighting over the EOS ensemble, the EOS-relevant dark-sector scale μ<em>χ≡m</em>χ/λ<sup>1/4μ<em>χ\equiv m</em>χ/λ<sup>{1/4} is localized around 250 MeV for both NICER data sets. In the (mχ,λ)(m_χ,λ) parameterization, the marginalized boson-mass posterior peaks at mχ≃300m_χ\simeq300--$330$ MeV, while λλ remains broadly distributed. Since the bosonic EOS depends on mχm_χ and λλ only through μ<em>χμ<em>χ, their separate marginals are conditional on the adopted independent priors. The inferred DM fraction is more data-set dependent, with posterior modes near 4% for Maryland/Illinois and 12% for Amsterdam. Bosonic DM also shifts the inferred Q</em>satQ</em>{\rm sat} from negative toward intermediate and positive values, whereas the response of LsymL_{\rm sym} is weaker. This indicates a model-dependent trade-off between DM-induced compactification and the high-density stiffness of baryonic matter. These constraints remain conditional on the selected EOS family and the assumption of a common effective FχF_χ for all sources.

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