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    Testing bosonic dark matter through white dwarf mass measurements

    Jorge Castelo Mourelle1,2, Nicolas Sanchis-Gual1, José A. Font1,3, and Juan Calderón Bustillo4,5

    • 1Departamento de Astronomía y Astrofísica, Universitat de València, Doctor Moliner 50, 46100 Burjassot (València), Spain
    • 2Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Circuito Exterior Ciudad Universitaria, Apartado Postal 70-543, México Distrito Federal 04510, México
    • 3Observatori Astronòmic, Universitat de València, Calle Catedrático Josè Beltrán 2, 46980, Paterna (València), Spain
    • 4Departamento de Física de Partículas, Universidad de Santiago de Compostela and Instituto Galego de Física de Altas Enerxias (IGFAE), E-15782 Santiago de Compostela, Spain
    • 5Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong

    Phys. Rev. D 113, 023049 – Published 26 January, 2026

    DOI: https://doi.org/10.1103/ktdz-dhjp

    Abstract

    Mass estimates of white dwarfs via electromagnetic methods, often differ from those obtained through gravitational redshift measurements, in some cases with discrepancies ranging in 5%–15% across independent datasets. Although many of the discrepancies reported in large spectroscopic surveys and confirmed by high-precision techniques such as astrometric microlensing and wide-binary analyses may be attributable to thermal effects, model uncertainties or measurement errors prevent a complete description of some of the observations. Here, we explore an alternative explanation based on the presence of a gravitationally coupled bosonic scalar field that contributes to the stellar mass while remaining electromagnetically invisible. We construct stationary, static mixed configurations consisting of a white dwarf that presents a bosonic scalar field (dark matter) component, forming a composite white dwarf–boson star system. We explore families of solutions showing that a scalar field fraction of fDM∼5%–15% to the mass contribution can account for the observed redshift excess. Our models provide a physically motivated explanation for the mass bias, might offer new observational signatures, and allow us to place preliminary constraints on the mass and compactness of the scalar field configuration. Finally, using our theoretical framework in combination with Bayesian model selection we provide plausible bounds for the mass of the constituent (ultralight) bosonic particle.

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