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Fig. 6.

image

Comparison of the inferred Dd, Ds/Dds, DΔt, and λint in different cases. Case 1 (orange): The distance measurements directly from single time-delay mock lens without assuming any cosmological model. Case 2 (blue): The distance measurements under the assumption of the flat wCDM model with Ωm = [0.05, 1.0], Ωde = 1 − Ωm, w = [ − 2.5, 0.5], and H0 uniform in [0,150] km s−1 Mpc−1. Case 3 (black): The distance measurements under the assumption of the ΛCDM model with Ωm = [0.05, 1.0], ΩΛ = 1 − Ωm, and H0 uniform in [0,150] km s−1 Mpc−1 Case 4: (green): The distance measurements from single time-delay mock lens, Pantheon dataset, and BAO dataset by using splines with free Ωk. Case 5 (red): The distance measurements from single time-delay mock lens, Pantheon dataset, and BAO dataset by using splines with Ωk = 0. For the cases (green and red) that do not assume a particular cosmological model, the constraining power on λint is comparable to the cases (blue and black) with an assumption of having a underlying cosmological model.

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