Table 6.
Weak lensing mass constraints derived from the fit of the tangential reduced shear profiles around the X-ray centres using spherical NFW models assuming the c(M) relation from Diemer & Kravtsov (2015) with updated parameters from Diemer & Joyce (2019) for two different over-densities Δ ∈ {200c, 500c}.
| Cluster |
 |
 |
σ(ln b200c, WL) |
 |
 |
σ(ln b500c, WL) |
|---|---|---|---|---|---|---|
| SPT-CL J0156−5541 |
 |
0.88 ± 0.02 | 0.35 ± 0.03 |
 |
0.92 ± 0.03 | 0.28 ± 0.05 |
| SPT-CL J0205−5829 |
 |
0.76 ± 0.03 | 0.41 ± 0.05 |
 |
0.79 ± 0.03 | 0.41 ± 0.04 |
| SPT-CL J0313−5334 |
 |
0.86 ± 0.03 | 0.44 ± 0.04 |
 |
0.83 ± 0.03 | 0.37 ± 0.05 |
| SPT-CL J0459−4947 |
 |
0.85 ± 0.05 | 0.51 ± 0.08 |
 |
0.79 ± 0.05 | 0.43 ± 0.10 |
| SPT-CL J0607−4448 |
 |
0.86 ± 0.03 | 0.46 ± 0.04 |
 |
0.82 ± 0.04 | 0.45 ± 0.06 |
| SPT-CL J0640−5113 |
 |
0.93 ± 0.03 | 0.27 ± 0.08 |
 |
0.85 ± 0.04 | 0.37 ± 0.05 |
| SPT-CL J2040−4451 |
 |
0.89 ± 0.04 | 0.44 ± 0.06 |
 |
0.74 ± 0.04 | 0.48 ± 0.06 |
| SPT-CL J2341−5724 |
 |
0.88 ± 0.03 | 0.35 ± 0.04 |
 |
0.87 ± 0.03 | 0.25 ± 0.05 |
Notes. The maximum likelihood mass estimates 
are given in 1014 M⊙, where errors correspond to statistical 68% uncertainties from shape noise (asymmetric errors), followed by uncorrelated large-scale structure projections, the calibration of the UHIGH band, and variations in the redshift distribution between different lines of sight (for systematic uncertainties see Table 3). Statistical corrections for mass modelling biases have not yet been applied for 
. They are characterised by 
and σ(ln bΔ, WL), which relate to the mean and the width of the estimated mass bias distribution (see Sect. 6.3).
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