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Table 2.

Flux ratio compared to candidate counterimages and the derived magnification factor.

f/f4.4 (Continuum) f/f4.4 (O I 8449Å) μ (P21) μ (S22)
Godzilla 7.6 ± 0.38 35 ± 5.1 570 100 + 100 $ 570^{+100}_{-100} $ 550 120 + 92 $ 550^{+92}_{-120} $
P1 1.2 ± 0.077 1.2 ± 0.20 20 3.9 + 3.8 $ 20^{+3.8}_{-3.9} $ 19 4.5 + 3.5 $ 19^{+3.5}_{-4.5} $
P2 1.7 ± 0.099 1.6 ± 0.25 26 5.0 + 4.9 $ 26^{+4.9}_{-5.0} $ 25 5.9 + 4.4 $ 25^{+4.4}_{-5.9} $

f/f4.9 (Continuum) f/f4.9 (O I 8449Å) μ (P21) μ (S22)

Godzilla 9.5 ± 0.55 94 ± 22 6700 1700 + 1700 $ 6700^{+1700}_{-1700} $ 2900 740 + 1100 $ 2900^{+1100}_{-740} $
P1 1.5 ± 0.10 3.3 ± 0.8 230 60 + 61 $ 230^{+61}_{-60} $ 100 26 + 40 $ 100^{+40}_{-26} $
P2 2.1 ± 0.14 4.3 ± 1.0 310 78 + 80 $ 310^{+80}_{-78} $ 130 34 + 50 $ 130^{+50}_{-34} $

Notes. Top row shows the comparison with image 4.4, and the bottom row shows the comparison with image 4.9. The continuum flux is calculated as the average of the flux ratios from 6 NIRCam filters (F115W, F150W, F200W, F277W, F356W, F444W), weighted with the inverse square of the error. The O I flux was calculated from each clump’s 1D spectrum. The magnification factor was determined by comparing the values for images 4.4 and 4.9 given in Pignataro et al. (2021) and Sharon et al. (2022), denoted as P21 and S22, respectively.

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