Figure 5
From: Absorption-assisted mode transformation in butterfly compound eyes

Impact of conformally extended absorption.
(a) The setting of the conformally extended absorption which starts from z = zt with a t μm-thick buffer. (b,c) The amplitude and phase profiles obtained at the Rh entrance when t = 0.35 μm. LP01 profiles are also superimposed for comparison. (b) For zt = 65 μm, i.e., 3 μm-long conformal absorption, the output becomes indistinguishable from LP01. The inset shows how the increase in the conformal absorption reduces the mismatch in the output amplitude profile, especially near ρ = 2 μm. (c) The conformal absorption also improves the wavefront flatness within the radial extent of CS. (d) The minimum phase and shape errors for various (zt, t) combinations. Note that δp and δs minimize simultaneously near (zt, t) = (65 ~ 66, 0.2 ~ 0.35) μm. (e) The change in the mode power along the propagation through CC and CS. CP/CC: The interface between CP and CC.