Figure 2
From: Generation of flower high-order Poincaré sphere laser beams from a spatial light modulator
(a)–(e) Numerical results of the superposed LG modes represented by Eq. (1). (a) LG(1, 3, 0, −4, 1), (b) LG(1, 4, 0, −5, 2), (c) LG(2, 1, 0, 6, 1), (d) LG(0, 10, 9, −11, 1), (e) LG(3, 16, 0, −18, 2). (a’)–(e’) Phase distribution corresponding to (a)–(e).
