Fig. 1

Comparison of the magnitude of convergence, shear, first and second flexion due to a dark matter halo of mass M200 = 1 × 1012 h-1 M⊙, assuming that the mass distribution is described by Einasto, NFW, and SIS profiles and the Sérsic model. The lens and source planes are located at redshifts zL = 0.4 and zS = 0.92, respectively. The Einsten radius for the SIS is θE = 0.216″, indicating the angular distance when the weak lensing effects are relevant.
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