Fig. 10.
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Comparison of the parameter posteriors of the dynamical modeling performed with JWST-NIRSpec-only data (red), Keck-KCWI-only data (blue), and both combined (black). The four free parameters in our dynamical model are the ratio of the tangential and radial velocity dispersion σt/σr ≡ (1 − βani)1/2 with βani being the amplitude of a spatially constant anisotropy profile, the MST parameter λmst, the main deflector’s Einstein radius θE, the power-law mass profile’s logarithmic slope γ, and the super-massive black hole’s Einstein radius θE, bh. We have imposed a prior on the total Einstein radius (θE2 + θE, bh2)1/2 based on the lens model posterior of Suyu et al. (2013), which dominates the θE posterior illustrated here. All of them are consistent at ≲1σ confidence levels. The JWST NIRSpec’s superior spatial resolution also allows for the exclusion of a large fraction of the prior volume in the anisotropy parameter (σt/σr) that is largely unconstrained by the Keck-KCWI measurements.
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