Feili Wang, Cibo Lou, Yi Liang, "Propagation dynamics of ring Airy Gaussian beams with cosine modulated optical vortices," Chin. Opt. Lett. 16, 110502 (2018)

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- Chinese Optics Letters
- Vol. 16, Issue 11, 110502 (2018)

Fig. 1. (a1) The side-view propagation of a common RAG beam; (a2) the intensity profile at the focus plane marked by the dashed line in (a1); (a3) the distribution of | u | 2 marked by the dashed line in (a2); (a4) the phase pattern of the common RAG beam at the focus plane; (b1)–(b4) are the corresponding properties of the RAGB.

Fig. 2. Intensity and phase patterns of RAGB with CMOV with the parameters C 0 = 1 , m = 0 , n = 3 , and φ 0 = 0 during propagation. (a1)–(a5) The intensity distributions of the RAGB with CMOV for various propagation distances z = 0 m , 0.04 m, 0.08 m, 0.12 m, 0.16 m, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 3. Intensity and phase patterns of RAGB with CMOV for various n at the distance z = 0.12 m when C 0 = 1 , m = 0 , and φ 0 = 0 . (a1)–(a5) are the beam spots for n = 0 , 1 , 2 , 3 , 4 , respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 4. Intensity and phase patterns of RAGB with CMOV for various φ 0 at the distance z = 0.12 m when C 0 = 1 , m = 0 , and n = 3 . (a1)–(a5) are the beam spots for φ 0 = 0 , π 2 , π , 3 π 2 , 2 π , respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 5. (a) The peak intensity distributions of the RAGB with CMOV during propagation for m = 0 , n = 0 , 1 , 2 , 3 , 4 , respectively; (b) the max peak intensities of (a) for various n .

Fig. 6. Intensity and phase patterns of the RAGB with CMOV with the parameters m = 1 , n = 2 , and φ 0 = 0 during propagation. (a1)–(a5) The intensity distributions of the RAGB with CMOV for various propagation distances z = 0 m , 0.04 m, 0.08 m, 0.12 m, 0.16 m, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 7. The modulation phase distributions and the intensity distributions at z = 0 m and z = 0.12 m versus the spiral phase θ when C 0 = 1 , φ 0 = 0 for different factors m and n . (a) m = 0 , n = 3 ; (b) m = 1 , n = 2 .

Fig. 8. Intensity and phase patterns of RAGB with CMOV for various φ 0 at the distance z = 0.12 m when C 0 = 1 , m = 1 , and n = 2 . (a1)–(a5) The beam spots for φ 0 = 0 , π 2 , π , 3 π 2 , 2 π , respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 9. Intensity and phase patterns of RAGB with CMOV for various n at the distance z = 0.12 m when C 0 = 1 , m = 1 , and φ 0 = 0 . (a1)–(a5) are the beam spots for n = 0 , 1 , 2 , 3 , 4 , respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 10. (a) Peak intensity distributions of the RAGB with CMOV during propagation for m = 1 , n = 0 , 1 , 2 , 3 , 4 , respectively; (b) the max peak intensities of (a) for various n .

Fig. 11. Intensity and phase patterns of RAGB with CMOV for various n at the distance z = 0.12 m when C 0 = 1 , m = 2 , and φ 0 = 0 . (a1)–(a5) are the beam spots for n = 0 , 1 , 2 , 3 , 4 , respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).

Fig. 12. (a) Peak intensity distributions of the RAGB with CMOV during propagation for m = 2 , n = 0 , 1 , 2 , 3 , 4 , respectively; (b) the max peak intensity of (a) for various n .

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