Figure 5
From: The upper limit of the in-plane spin splitting of Gaussian beam reflected from a glass-air interface
The changes of the SDDs Δ+ (a) and Δ− (b) as functions of the incident angle θ i and the initial amplitude ratio t, when Δδ = π/2. (c) The corresponding energy ratio between the RCP and LCP components 10 log(W +/W −). Insets in (a) and (b) zoom in the ranges of t between −1.1 and −0.9 and 0.9 and 1.1, respectively.
