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Table 3.

Parameter estimation results for the BMP parameterization.

BMP Priors: [1.0, 3.0] [0.1, 20.0] [0.1, 2.0]
Redshift Mass c500 P0 β χr2
z ∈ [0.0, 0.4] M500c ∈ [1014.0,1014.3] M 2 . 28 0.04 + 0.05 Mathematical equation: $ 2.28^{+0.05}_{-0.04} $ 5 . 8 0.3 + 0.4 Mathematical equation: $ 5.8^{+0.4}_{-0.3} $ 1 . 07 0.03 + 0.03 Mathematical equation: $ 1.07^{+0.03}_{-0.03} $ 0.07
z ∈ [0.0, 0.4] M500c ∈ [1014.3,1014.6] M 2 . 42 0.03 + 0.03 Mathematical equation: $ 2.42^{+0.03}_{-0.03} $ 6 . 0 0.3 + 0.3 Mathematical equation: $ 6.0^{+0.3}_{-0.3} $ 1 . 08 0.02 + 0.02 Mathematical equation: $ 1.08^{+0.02}_{-0.02} $ 1.02
z ∈ [0.0, 0.4] M500c ∈ [1014.6,1015.1] M 2 . 49 0.03 + 0.03 Mathematical equation: $ 2.49^{+0.03}_{-0.03} $ 8 . 1 0.5 + 0.5 Mathematical equation: $ 8.1^{+0.5}_{-0.5} $ 1 . 29 0.03 + 0.03 Mathematical equation: $ 1.29^{+0.03}_{-0.03} $ 0.11
z ∈ [0.0, 0.4] All masses 2 . 52 0.02 + 0.02 Mathematical equation: $ 2.52^{+0.02}_{-0.02} $ 6 . 7 0.3 + 0.3 Mathematical equation: $ 6.7^{+0.3}_{-0.3} $ 1 . 10 0.02 + 0.02 Mathematical equation: $ 1.10^{+0.02}_{-0.02} $ 0.45

z ∈ [0.4, 0.8] M500c ∈ [1014.0,1014.3] M 2 . 49 0.04 + 0.04 Mathematical equation: $ 2.49^{+0.04}_{-0.04} $ 5 . 0 0.4 + 0.4 Mathematical equation: $ 5.0^{+0.4}_{-0.4} $ 0 . 99 0.03 + 0.03 Mathematical equation: $ 0.99^{+0.03}_{-0.03} $ 0.38
z ∈ [0.4, 0.8] M500c ∈ [1014.3,1014.6] M 2 . 08 0.02 + 0.02 Mathematical equation: $ 2.08^{+0.02}_{-0.02} $ 4 . 6 0.2 + 0.2 Mathematical equation: $ 4.6^{+0.2}_{-0.2} $ 1 . 18 0.02 + 0.02 Mathematical equation: $ 1.18^{+0.02}_{-0.02} $ 1.73
z ∈ [0.4, 0.8] M500c ∈ [1014.6,1015.1] M 2 . 18 0.03 + 0.03 Mathematical equation: $ 2.18^{+0.03}_{-0.03} $ 5 . 4 0.3 + 0.3 Mathematical equation: $ 5.4^{+0.3}_{-0.3} $ 1 . 19 0.02 + 0.02 Mathematical equation: $ 1.19^{+0.02}_{-0.02} $ 2.29
z ∈ [0.4, 0.8] All masses 2 . 11 0.02 + 0.02 Mathematical equation: $ 2.11^{+0.02}_{-0.02} $ 4 . 9 0.2 + 0.2 Mathematical equation: $ 4.9^{+0.2}_{-0.2} $ 1 . 18 0.02 + 0.02 Mathematical equation: $ 1.18^{+0.02}_{-0.02} $ 1.76

z ∈ [0.8, 2.0] M500c ∈ [1014.0,1014.3] M 2 . 50 0.04 + 0.04 Mathematical equation: $ 2.50^{+0.04}_{-0.04} $ 3 . 8 0.6 + 0.7 Mathematical equation: $ 3.8^{+0.7}_{-0.6} $ 0 . 90 0.06 + 0.06 Mathematical equation: $ 0.90^{+0.06}_{-0.06} $ 0.41
z ∈ [0.8, 2.0] M500c ∈ [1014.3,1014.6] M 2 . 28 0.03 + 0.03 Mathematical equation: $ 2.28^{+0.03}_{-0.03} $ 4 . 2 0.3 + 0.3 Mathematical equation: $ 4.2^{+0.3}_{-0.3} $ 1 . 08 0.03 + 0.03 Mathematical equation: $ 1.08^{+0.03}_{-0.03} $ 0.57
z ∈ [0.8, 2.0] M500c ∈ [1014.6,1015.1] M 2 . 64 0.04 + 0.04 Mathematical equation: $ 2.64^{+0.04}_{-0.04} $ 7 . 6 0.9 + 1.0 Mathematical equation: $ 7.6^{+1.0}_{-0.9} $ 1 . 18 0.05 + 0.05 Mathematical equation: $ 1.18^{+0.05}_{-0.05} $ 0.92
z ∈ [0.8, 2.0] All masses 2 . 50 0.02 + 0.02 Mathematical equation: $ 2.50^{+0.02}_{-0.02} $ 4 . 5 0.4 + 0.4 Mathematical equation: $ 4.5^{+0.4}_{-0.4} $ 1 . 00 0.03 + 0.03 Mathematical equation: $ 1.00^{+0.03}_{-0.03} $ 0.65

All redshifts M500c ∈ [1014.0,1014.3] M 2 . 36 0.03 + 0.03 Mathematical equation: $ 2.36^{+0.03}_{-0.03} $ 4 . 8 0.4 + 0.4 Mathematical equation: $ 4.8^{+0.4}_{-0.4} $ 1 . 00 0.03 + 0.03 Mathematical equation: $ 1.00^{+0.03}_{-0.03} $ 0.16
All redshifts M500c ∈ [1014.3,1014.6] M 2 . 01 0.01 + 0.01 Mathematical equation: $ 2.01^{+0.01}_{-0.01} $ 4 . 5 0.2 + 0.2 Mathematical equation: $ 4.5^{+0.2}_{-0.2} $ 1 . 19 0.02 + 0.02 Mathematical equation: $ 1.19^{+0.02}_{-0.02} $ 1.01
All redshifts M500c ∈ [1014.6,1015.1] M 2 . 37 0.02 + 0.02 Mathematical equation: $ 2.37^{+0.02}_{-0.02} $ 7 . 1 0.4 + 0.4 Mathematical equation: $ 7.1^{+0.4}_{-0.4} $ 1 . 26 0.03 + 0.03 Mathematical equation: $ 1.26^{+0.03}_{-0.03} $ 0.07
All redshifts All masses 2 . 16 0.01 + 0.01 Mathematical equation: $ 2.16^{+0.01}_{-0.01} $ 5 . 2 0.3 + 0.3 Mathematical equation: $ 5.2^{+0.3}_{-0.3} $ 1 . 17 0.02 + 0.02 Mathematical equation: $ 1.17^{+0.02}_{-0.02} $ 0.27

Notes. The table quotes the best-fit estimates for the BMP parameters as obtained from the multistage fit. Uncertainties are quoted at the 68% confidence level; for c500, the error bars have been rescaled using a Fisher-matrix correction as discussed in Sec. 6.1.

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