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ABSTRACT The free-streaming length of dark matter depends on fundamental dark matter physics, and determines the abundance and concentration of dark matter haloes on sub-galactic scales. Using the image positions and flux ratios from eight quadruply imaged quasars, we constrain the free-streaming length of dark matter and the amplitude of the subhalo mass function (SHMF). We model both main deflector subhaloes and haloes along the line of sight, and account for warm dark matter free-streaming effects on the mass function and mass–concentration relation. By calibrating the scaling of the SHMF with host halo mass and redshift using a suite of simulated haloes, we infer a global normalization for the SHMF. We account for finite-size background sources, and marginalize over the mass profile of the main deflector. Parametrizing dark matter free-streaming through the half-mode mass mhm, we constrain the thermal relic particle mass mDM corresponding to mhm. At 95 \, per\, cent CI: mhm 107. 8 M⊙ (m ₃₌ 5. 2 \ keV). We disfavour m ₃₌ = 4. 0 \, keV and m ₃₌ = 3. 0 \, keV with likelihood ratios of 7: 1 and 30: 1, respectively, relative to the peak of the posterior distribution. Assuming cold dark matter, we constrain the projected mass in substructure between 106 and 109 M⊙ near lensed images. At 68 \, per\, cent CI, we infer 2. 0-6. 1 10^7\, { M }\, kpc^{-2}, corresponding to mean projected mass fraction f ₒₔ₁ = 0. 035-₀. ₀₁₇^+0. 021. At 95 \, per\, cent CI, we obtain a lower bound on the projected mass of 0. 6 10^7 \, { M }\, kpc^{-2}, corresponding to f ₒₔ₁ 0. 005. These results agree with the predictions of cold dark matter.
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Daniel Gilman
University of Chicago
Simon Birrer
Stony Brook University
Anna Nierenberg
University of California, Merced
Monthly Notices of the Royal Astronomical Society
University of California, Los Angeles
Jet Propulsion Laboratory
Carnegie Observatories
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Gilman et al. (Tue,) studied this question.
synapsesocial.com/papers/6a0eec75b7cc3b883f22e3c2 — DOI: https://doi.org/10.1093/mnras/stz3480