Figure E1.
The lensing rate, defined as the ratio of the number of observable lenses to the parent ETGs used to simulate them, is plotted as a function of velocity dispersion. Solid lines in the left and right panels represent results from our Monte Carlo simulations for single-source and double-source strong lensing, respectively. The dashed line in the right panel corresponds to a ‘pseudo’ double-source lensing rate obtained by squaring the curve from the left panel. The solid line in the right panel exhibits a counter-trend drop in the largest velocity dispersion bin due to significant Poisson counting noise.

The lensing rate, defined as the ratio of the number of observable lenses to the parent ETGs used to simulate them, is plotted as a function of velocity dispersion. Solid lines in the left and right panels represent results from our Monte Carlo simulations for single-source and double-source strong lensing, respectively. The dashed line in the right panel corresponds to a ‘pseudo’ double-source lensing rate obtained by squaring the curve from the left panel. The solid line in the right panel exhibits a counter-trend drop in the largest velocity dispersion bin due to significant Poisson counting noise.

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