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Table 1.

Structural properties of the fitted dark matter haloes.

Halo log(M200) log(c200) log(M200)MLE log(c200)MLE V2 kpc Vmax Rmax BIC
[log(M)] [log(M)] [km/s] [km/s] [kpc]
CDM, CORENFW, Case 1 9 . 36 0.31 + 0.37 $ 9.36^{+0.37}_{-0.31} $ 0 . 44 0.27 + 0.39 $ 0.44^{+0.39}_{-0.27} $ 9.21 0.40 11 . 1 1.6 + 1.6 $ 11.1^{+1.6}_{-1.6} $ 19 . 6 3.5 + 6.0 $ 19.6^{+6.0}_{-3.5} $ 21 . 4 11.8 + 29.4 $ 21.4^{+29.4}_{-11.8} $ 11 . 13 1.05 + 2.51 $ 11.13^{+2.51}_{-1.05} $
CDM, CORENFW, Case 2 10 . 06 0.07 + 0.13 $ 10.06^{+0.13}_{0.07} $ 0 . 08 0.06 + 0.10 $ 0.08^{+0.10}_{-0.06} $ 9.99 0.02 11 . 3 0.8 + 1.0 $ 11.3^{+1.0}_{-0.8} $ 33 . 6 2.0 + 3.7 $ 33.6^{+3.7}_{-2.0} $ 84 . 4 18.2 + 14.9 $ 84.4^{+14.9}_{-18.2} $ 11 . 32 0.53 + 1.67 $ 11.32^{+1.67}_{-0.53} $
CDM, DPL, Case 1 ( * ) 9 . 24 0.29 + 0.35 $ 9.24^{+0.35}_{-0.29} $ 0 . 57 0.24 + 0.15 $ 0.57^{+0.15}_{-0.24} $ 9.20 0.63 6 . 8 2.9 + 3.4 $ 6.8^{+3.4}_{-2.9} $ 13 . 0 5.7 + 4.4 $ 13.0^{+4.4}_{-5.7} $ 13 . 7 5.8 + 20.5 $ 13.7^{+20.5}_{-5.8} $ 12 . 99 1.39 + 3.17 $ 12.99^{+3.17}_{-1.39} $
CDM, DPL, Case 2 ( * ) 10 . 16 0.15 + 0.39 $ 10.16^{+0.39}_{-0.15} $ 0 . 18 0.12 + 0.13 $ 0.18^{+0.13}_{-0.12} $ 10.03 0.19 4 . 3 1.1 + 1.5 $ 4.3^{+1.5}_{-1.1} $ 19 . 9 5.2 + 8.8 $ 19.9^{+8.8}_{-5.2} $ 71 . 5 24.5 + 40.0 $ 71.5^{+40.0}_{-24.5} $ 17 . 20 3.48 + 4.38 $ 17.20^{+4.38}_{-3.48} $
SIDM, Case 1 9 . 21 0.22 + 0.25 $ 9.21^{+0.25}_{-0.22} $ 0 . 61 0.19 + 0.16 $ 0.61^{+0.16}_{-0.19} $ 9.17 0.63 12 . 0 2.4 + 2.2 $ 12.0^{+2.2}_{-2.4} $ 19 . 0 2.7 + 3.5 $ 19.0^{+3.5}_{-2.7} $ 11 . 1 4.5 + 10.2 $ 11.1^{+10.2}_{-4.5} $ 9 . 81 1.41 + 2.97 $ 9.81^{+2.97}_{-1.41} $
SIDM, Case 2 10 . 08 0.09 + 0.21 $ 10.08^{+0.21}_{-0.09} $ 0 . 17 0.11 + 0.14 $ 0.17^{+0.14}_{-0.11} $ 10.01 0.10 7 . 5 0.9 + 1.4 $ 7.5^{+1.4}_{-0.9} $ 35 . 1 2.5 + 6.7 $ 35.1^{+6.7}_{-2.5} $ 65 . 6 21.9 + 26.4 $ 65.6^{+26.4}_{-21.9} $ 17 . 50 1.49 + 2.44 $ 17.50^{+2.44}_{-1.49} $
FDM, Case 1 8 . 99 0.57 + 0.41 $ 8.99^{+0.41}_{-0.57} $ 0 . 58 0.42 0.60 $ 0.58^{0.60}_{-0.42} $ 9.09 0.09 9 . 7 2.1 + 2.8 $ 9.7^{+2.8}_{-2.1} $ 18 . 8 2.2 + 2.6 $ 18.8^{+2.6}_{-2.2} $ 7 . 0 1.8 + 10.9 $ 7.0^{+10.9}_{-1.8} $ 16 . 26 1.37 + 2.03 $ 16.26^{+2.03}_{-1.37} $
FDM, Case 2 10 . 04 0.06 + 0.11 $ 10.04^{+0.11}_{-0.06} $ 0 . 08 0.06 + 0.10 $ 0.08^{+0.10}_{-0.06} $ 9.99 0.02 9 . 1 1.5 + 2.1 $ 9.1^{+2.1}_{1.5} $ 33 . 3 1.7 + 3.0 $ 33.3^{+3.0}_{-1.7} $ 84 . 1 18.6 + 12.8 $ 84.1^{+12.8}_{-18.6} $ 18 . 95 1.08 + 1.70 $ 18.95^{+1.70}_{-1.08} $

Notes. The first column lists the corresponding mass model. Case 1 considers a broad log(M200) prior, while for Case 2 a lower limit on log(M200) was imposed. The second and third columns give the halo mass and concentration parameters. The values and uncertainties in log(M200) and log(c200) come from the 16th, 50th, and 84th percentiles of the posterior distributions shown in Appendix D. The fourth and fifth columns provide the maximum-likelihood estimation (MLE) of log(M200) and log(c200) (the remaining MLE parameters are given in the corresponding figures of each mass model). The sixth, seventh, and eighth columns give V2 kpc, Vmax, and Rmax, respectively. These values are obtained by reconstructing and sampling the MCMC chains of each mass model and obtaining the distribution of those parameters. Finally, the last column gives the BIC of each model computed from the posterior distributions. ( * )The DPL (double power-law) fits are shown in Appendix C and included here for completeness.

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