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Table 2.

MCMC results from each considered case.

σ8 CUE24a As CUE24a AsPlanck AsPlanck (σ = 0.1) As CUE24a (no G15)
α 0 . 69 0.46 + 0.30 ( 0.60 ) $ 0.69^{+0.30}_{-0.46}\,(0.60) $ > 0.79 (−) > 1.17 (−) > 1.09 (−) 0 . 89 0.26 + 0.18 ( 0.81 ) $ 0.89^{+0.18}_{-0.26}\,(0.81) $
log Mmin 11 . 64 0.12 + 0.17 ( 11.68 ) $ 11.64^{+0.17}_{-0.12}\,(11.68) $ 11 . 47 0.11 + 0.14 ( 11.50 ) $ 11.47^{+0.14}_{-0.11}\,(11.50) $ 11 . 49 0.16 + 0.14 ( 11.50 ) $ 11.49^{+0.14}_{-0.16}\,(11.50) $ 11 . 53 0.14 + 0.15 ( 11.54 ) $ 11.53^{+0.15}_{-0.14}\,(11.54) $ 11 . 46 0.16 + 0.27 ( 11.53 ) $ 11.46^{+0.27}_{-0.16}\,(11.53) $
log M1 13 . 39 0.92 + 0.71 ( 13.34 ) $ 13.39^{+0.71}_{-0.92}\,(13.34) $ 12 . 89 0.41 + 0.56 ( 13.01 ) $ 12.89^{+0.56}_{-0.41}\,(13.01) $ 12 . 52 0.25 + 0.36 ( 12.61 ) $ 12.52^{+0.36}_{-0.25}\,(12.61) $ 12 . 59 0.34 + 0.50 ( 12.71 ) $ 12.59^{+0.50}_{-0.34}\,(12.71) $ 12 . 43 0.46 + 0.70 ( 12.68 ) $ 12.43^{+0.70}_{-0.46}\,(12.68) $
Ωm 0 . 28 0.08 + 0.04 ( 0.25 ) $ 0.28^{+0.04}_{-0.08}\,(0.25) $ 0 . 18 0.02 + 0.02 ( 0.18 ) $ 0.18^{+0.02}_{-0.02}\,(0.18) $ 0 . 16 0.02 + 0.01 ( 0.16 ) $ 0.16^{+0.01}_{-0.02}\,(0.16) $ 0 . 17 0.03 + 0.01 ( 0.16 ) $ 0.17^{+0.01}_{-0.03}\,(0.16) $ 0 . 34 0.03 + 0.02 ( 0.33 ) $ 0.34^{+0.02}_{-0.03}\,(0.33) $
h < 0.70 (−) > 0.77 (−) > 0.82 (−) > 0.83 (−) 0 . 72 0.06 + 0.07 ( 0.73 ) $ 0.72^{+0.07}_{-0.06}\,(0.73) $
mν (eV) − (−) < 0.22 (−) < 0.36 (−) < 0.46 (−) − (−)
β 2 . 91 0.04 + 0.04 ( 2.91 ) $ 2.91^{+0.04}_{-0.04}\,(2.91) $ 2 . 91 0.02 + 0.03 ( 2.91 ) $ 2.91^{+0.03}_{-0.02}\,(2.91) $ 2 . 92 0.04 + 0.04 ( 2.92 ) $ 2.92^{+0.04}_{-0.04}\,(2.92) $ 2 . 92 0.04 + 0.04 ( 2.92 ) $ 2.92^{+0.04}_{-0.04}\,(2.92) $ 2 . 90 0.03 + 0.04 ( 2.90 ) $ 2.90^{+0.04}_{-0.03}\,(2.90) $

Notes. The mean and 68% credible intervals for each parameter are stated, along with the marginalized maximum a posteriori value in parenthesis. Dashes indicate unconstrained distributions or unmeaningful maximum a posteriori values. Halo masses are expressed in M/h.

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