Table 2.

Virial mass, associated uncertainty, and radius of the spectroscopic groups in the field of HE 0435−1223 identified in Sluse et al. (2017). The last column shows our weak-lensing detection limit in terms of virial mass for haloes at each of the group redshifts. The limit is obtained according to equation (19).

|$\bar{z}_{\mathrm{ group}}$|log(Mvir/M)Rvir (Mpc)log(Mvir/M)limit
0.050313.32 ± 0.610.63515.52
0.174413.81 ± 0.401.07114.57
0.184113.65 ± 0.460.95414.57
0.320213.83 ± 0.361.25914.37
0.418513.18 ± 0.480.87314.37
0.454713.72 ± 0.361.38514.42
0.505913.72 ± 0.361.37314.42
0.565013.33 ± 0.430.97114.52
0.701912.49 ± 0.630.65414.72
|$\bar{z}_{\mathrm{ group}}$|log(Mvir/M)Rvir (Mpc)log(Mvir/M)limit
0.050313.32 ± 0.610.63515.52
0.174413.81 ± 0.401.07114.57
0.184113.65 ± 0.460.95414.57
0.320213.83 ± 0.361.25914.37
0.418513.18 ± 0.480.87314.37
0.454713.72 ± 0.361.38514.42
0.505913.72 ± 0.361.37314.42
0.565013.33 ± 0.430.97114.52
0.701912.49 ± 0.630.65414.72
Table 2.

Virial mass, associated uncertainty, and radius of the spectroscopic groups in the field of HE 0435−1223 identified in Sluse et al. (2017). The last column shows our weak-lensing detection limit in terms of virial mass for haloes at each of the group redshifts. The limit is obtained according to equation (19).

|$\bar{z}_{\mathrm{ group}}$|log(Mvir/M)Rvir (Mpc)log(Mvir/M)limit
0.050313.32 ± 0.610.63515.52
0.174413.81 ± 0.401.07114.57
0.184113.65 ± 0.460.95414.57
0.320213.83 ± 0.361.25914.37
0.418513.18 ± 0.480.87314.37
0.454713.72 ± 0.361.38514.42
0.505913.72 ± 0.361.37314.42
0.565013.33 ± 0.430.97114.52
0.701912.49 ± 0.630.65414.72
|$\bar{z}_{\mathrm{ group}}$|log(Mvir/M)Rvir (Mpc)log(Mvir/M)limit
0.050313.32 ± 0.610.63515.52
0.174413.81 ± 0.401.07114.57
0.184113.65 ± 0.460.95414.57
0.320213.83 ± 0.361.25914.37
0.418513.18 ± 0.480.87314.37
0.454713.72 ± 0.361.38514.42
0.505913.72 ± 0.361.37314.42
0.565013.33 ± 0.430.97114.52
0.701912.49 ± 0.630.65414.72
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