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Table 2.

Modeling of the deflector total mass distribution using the extended source modeling.

Multiple images A, B
PIEMD
x [″] y [″] q θ [rad] θE [″] rcore [″]
0.24 −0.14 0.79 0.14 10.9 [0.0]
Shear γext ϕext [rad]
0.25 1.45
Nobs = 5831 d.o.f. = 4576

SPEMD
x [″] y [″] q θ [rad] θE [″] rcore [″] γ
0.18 −0.14 0.75 0.09 3.9 [0.0] 1.57
Shear γext ϕext [rad]
0.06 1.07
Nobs = 5831 d.o.f. = 4571

Multiple images A, B, C
SPEMD
x [″] y [″] q θ [rad] θE [″] rcore [″] γ
0.05 −0.17 0.62 0.04 4.2 [0.0] 1.58
Shear γext ϕext [rad]
0.08 0.28
Source Dds/Ds = 0.543 (equals to zC = 1.69)
Nobs = 7195 d.o.f. = 5396

PIEMD+rc
x [″] y [″] q θ [rad] θE [″] rcore [″]
0.09 −0.12 0.84 0.15 18.7 3.4
Shear γext ϕext [rad]
0.09 1.25
Source Dds/Ds = 0.590 (equals to zC = 2.04)
Nobs = 7195 d.o.f. = 5583

Notes. The two upper models were optimized by exploting the double-peak source AB, while the two bottom models also include source C. The parameters are defined as in Table 1.

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