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Table A.1.

Best-fit parameters to the size–mass equation for each redshift bin that we fit for.

Redshift Parameter F115W F150W F200W F277W F356W F410M F444W
α 0.204 0.203 0.204 0.181 0.142 0.116 0.105
σα 0.012 0.011 0.010 0.009 0.009 0.009 0.009
3 ≤ z < 4 log10A 0.070 0.083 0.087 0.092 0.085 0.085 0.092
(zmedian = 3.21) σlog10A 0.006 0.005 0.005 0.004 0.004 0.004 0.004
σlogREFF 0.232 0.217 0.199 0.189 0.186 0.180 0.178
α 0.213 0.220 0.218 0.231 0.200 0.159 0.151
σα 0.015 0.014 0.013 0.012 0.012 0.012 0.012
4 ≤ z < 5 log10A -0.035 -0.031 -0.012 -0.012 -0.002 0.005 0.014
(zmedian = 4.43) σlog10A 0.007 0.007 0.006 0.005 0.005 0.006 0.006
σlogREFF 0.225 0.211 0.191 0.174 0.171 0.171 0.168
α 0.303 0.294 0.288 0.259 0.231 0.170 0.173
σα 0.033 0.031 0.030 0.028 0.028 0.029 0.029
5 ≤ z < 6 log10A -0.115 -0.109 -0.105 -0.082 -0.070 -0.023 -0.025
(zmedian = 5.28) σlog10A 0.015 0.014 0.013 0.012 0.013 0.013 0.013
σlogREFF 0.227 0.214 0.210 0.197 0.193 0.188 0.191
α 0.215 0.215 0.215 0.215 0.215 0.215 0.215
σα
6 ≤ z < 9 log10A -0.176 -0.184 -0.170 -0.153 -0.149 -0.133 -0.120
(zmedian = 6.42) σlog10A 0.028 0.027 0.024 0.019 0.017 0.019 0.018
σlogREFF 0.259 0.247 0.222 0.178 0.158 0.165 0.163

Notes. The best-fit parameters to the size–mass equation: logREFF = αlog(M*/M0)+logA. Here α is the slope, logA is the intercept at the turn-over stellar mass M0 = 109M, and σlogREFF is the intrinsic scatter. Due to low number statistics, the slope of the 6 ≤ z < 9 size–mass relation is fixed (see Section 2).

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