Table 4.
Model parameter estimates, as the median values, with 68% CL (i.e., 1σ) uncertainties and the adopted prior ranges.
Profile | Parameter | Prior | Median ±1σ |
---|---|---|---|
1st Halo | xH [″] | [ − 60, 60] | −0.5 ± 0.3 |
yH [″] | [ − 60, 60] |
![]() |
|
qH | [0.2, 1] |
![]() |
|
ϕH [rad] | ( −∞, +∞) | 0.60 ± 0.02 | |
θE,H [″] | [0, +∞) |
![]() |
|
rc,H [″] | [0, +∞) |
![]() |
|
2nd Halo | xH [″] | [ − 60, 60] |
![]() |
yH [″] | [ − 60, 60] |
![]() |
|
qH | [0.2, 1] |
![]() |
|
ϕH [rad] | ( −∞, +∞) |
![]() |
|
θE,H [″] | [0, +∞) |
![]() |
|
rc,H [″] | [0, +∞) | 7.1 ± 1.8 | |
3rd Halo | xH [″] | [ − 60, 60] |
![]() |
yH [″] | [ − 60, 60] |
![]() |
|
qH | [0.2, 1] |
![]() |
|
ϕH [rad] | ( −∞, +∞) | 0.60 ± 0.04 | |
θE,H [″] | [0, +∞) | 9.8 ± 0.9 | |
rc,H [″] | [0, +∞) |
![]() |
|
4th Halo (H4N) | xH [″] | [0, 60] |
![]() |
yH [″] | [0, 60] |
![]() |
|
θE,H [″] | [0, +∞) | 4.5 ± 0.5 | |
Scaling relation | θE,BCG [″] | [0, +∞) | 1.57 ± 0.24 |
rt,BCG [″] | [0, +∞) |
![]() |
|
1st member | q | [0.2, 1] |
![]() |
ϕ [rad] | ( −∞, +∞) |
![]() |
|
θE [″] | [0, +∞) |
![]() |
|
rt [″] | [0, +∞) |
![]() |
|
2nd member | q | [0.2, 1] | 0.6 ± 0.3 |
ϕ [rad] | ( −∞, +∞) |
![]() |
|
θE [″] | [0, +∞) |
![]() |
|
rt [″] | [0, +∞) |
![]() |
|
photo-z | z6 | [0, 6] |
![]() |
z7 | [0, 6] | 2.74 ± 0.06 | |
z8 | [0, 6] |
![]() |
Notes. The positions are given relative to the BCG, Einstein radii are given for a source redshift of infinity, and all position angle values, measured counterclockwise from the positive x-axis, are converted to the range [0, π]. For the prior ranges, square brackets indicates bounds included in the prior range, while round brackets indicate bounds excluded. The median values and 1σ uncertainties are computed by excluding the first 20 000 accepted iterations as burn-in points.
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