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Constraining Dark Matter Substructure With Gaia Wide Binaries

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arxiv 2209.08100 v1 pith:JR2IFZNP submitted 2022-09-16 hep-ph astro-ph.GA

classification hep-phastro-ph.GA
keywords widebinariessubhalosconstraintsdarkdensitymatterprofiles
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abstract

We use a catalogue of stellar binaries with wide separations (up to 1 pc) identified by the Gaia satellite to constrain the presence of extended substructure within the Milky Way galaxy. Heating of the binaries through repeated encounters with substructure results in a characteristic distribution of binary separations, allowing constraints to be placed independent of the formation mechanism of wide binaries. Across a wide range of subhalo density profiles, we show that subhalos with masses $\gtrsim 65 \ M_\odot$ and characteristic length scales similar to the separation of these wide binaries cannot make up 100% of the Galaxy's dark matter. Constraints weaken for subhalos with larger length scales and are dependent on their density profiles. For such large subhalos, higher central densities lead to stronger constraints. Subhalos with density profiles similar to those expected from cold dark matter must be at least $\sim 5,000$ times denser than predicted by simulation to be constrained by the wide binary catalogue.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Probing the fate of large primordial perturbations with exoplanets

    astro-ph.CO 2026-06 conditional novelty 6.5 of 10

    Observed ultra-wide exoplanets already constrain the amplitude and scale of primordial power-spectrum peaks that produce ultra-compact minihalos, with misalignment signatures as a future probe.

  2. Wide binaries in ultra-faint dwarf galaxies as a probe of extended dark objects

    hep-ph 2026-07 conditional novelty 5.0 of 10

    Wide binaries in Boötes I exclude dark-matter fractions down to ~10^-3 to 10^-2 for extended dark objects between 0.1 and 3000 solar masses with radii up to 10^7 solar radii, implying P_R ≲ 5×10^-6 at k ≈ 4×10^2-3×10^...

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