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Table 2.

Summary of the observational constraints of FBQ 0951+2635.

Parameter (units) Constraint Reference
zs 1.249 1
zl 0.260 2
APS 1
xA (″) 0.000 ± 0.001 3
yA (″) 0.000 ± 0.001 3
xB (″) −0.892 ± 0.001 3
yB (″) −0.628 ± 0.001 3
xG (″) −0.750 ± 0.002 3
yG (″) −0.459 ± 0.002 3
eG 0.25 ± 0.04 3
θeG (°) 22 ± 4 3
RG (″) 0.09 ± 0.02 3
APS 2
xA (″) 0.0000 ± 0.0001 4
yA (″) 0.0000 ± 0.0001 4
xB (″) −0.8983 ± 0.0012 4
yB (″) −0.6336 ± 0.0012 4
xG (″) −0.7521 ± 0.0028 4
yG (″) −0.4603 ± 0.0028 4
eG 0.47 ± 0.03 4
θeG (°) 12.8 ± 2.2 4
RG (″) 0.78 ± 0.01 4
M 0.23 ± 0.02 5
Δt (d) 13.5 ± 1.6 This paper
κext 0.23 6
γext 0.04 6
θγext (°) −44 6

Notes. zs and zl are the redshifts of the double quasar (images A and B) and the main lensing galaxy G, respectively. Additionally, regarding the two astro-photometric solutions APS 1 and APS 2, the brightest image A is located at the origin of coordinates, and the positive direction of x is defined by west, while the positive direction of y is defined by north. Some astrometric errors were also made symmetric (σx = σy). The morphology of G (De Vaucouleurs brightness profile) is given by three parameters: the ellipticity (eG), the position angle of the major axis (θeG; it is measured east of north), and the effective radius (RG). We also include the macro-magnification ratio M and time delay Δt with respect to the image A. All astro-photometric, magnification, and delay constraints are 1σ confidence intervals. The last three rows correspond to the external convergence, the external shear strength, and the position angle of the external shear. We also assumed a flat ΛCDM cosmology (see main text). (1) Momcheva et al. (2015); (2) Eigenbrod et al. (2007); (3) Jakobsson et al. (2005); (4) Sluse et al. (2012a); (5) Sluse et al. (2012b); (6) Wilson et al. (2017).

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