Fig. B.1.
Radial dependence on the projected velocity dispersion measurement for an Osipkov–Merritt anisotropy profile (Eq. (51)). Top to bottom: increase in the half light radius of the deflector. Left to right: change in the mass profile slope (https://github.com/TDCOSMO/hierarchy_analysis_2020_public/blob/6c293af582c398a5c9de60a51cb0c44432a3c598/MST_impact/anisotropy_ifu.ipynb).
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