• Chinese Optics Letters
  • Vol. 16, Issue 11, 110502 (2018)
Feili Wang1, Cibo Lou1,*, and Yi Liang2,**
Author Affiliations
  • 1Institute of Photonics, Faculty of Science, Ningbo University, Ningbo 315211, China
  • 2Guangxi Key Laboratory for Relativistic Astrophysics, School of Physics Science and Technology, Guangxi University, Nanning 530004, China
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    DOI: 10.3788/COL201816.110502 Cite this Article Set citation alerts
    Feili Wang, Cibo Lou, Yi Liang, "Propagation dynamics of ring Airy Gaussian beams with cosine modulated optical vortices," Chin. Opt. Lett. 16, 110502 (2018) Copy Citation Text show less
    (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. 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.
    Intensity and phase patterns of RAGB with CMOV with the parameters C0=1,m=0,n=3, and φ0=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. 2. Intensity and phase patterns of RAGB with CMOV with the parameters C0=1,m=0,n=3, and φ0=0 during propagation. (a1)–(a5) The intensity distributions of the RAGB with CMOV for various propagation distances z=0m, 0.04 m, 0.08 m, 0.12 m, 0.16 m, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12 m when C0=1,m=0, and φ0=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. 3. Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12m when C0=1,m=0, and φ0=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).
    Intensity and phase patterns of RAGB with CMOV for various φ0 at the distance z=0.12 m when C0=1,m=0, and n=3. (a1)–(a5) are the beam spots for φ0=0,π2,π,3π2,2π, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    Fig. 4. Intensity and phase patterns of RAGB with CMOV for various φ0 at the distance z=0.12m when C0=1,m=0, and n=3. (a1)–(a5) are the beam spots for φ0=0,π2,π,3π2,2π, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    (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. 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.
    Intensity and phase patterns of the RAGB with CMOV with the parameters m=1,n=2, and φ0=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. 6. Intensity and phase patterns of the RAGB with CMOV with the parameters m=1,n=2, and φ0=0 during propagation. (a1)–(a5) The intensity distributions of the RAGB with CMOV for various propagation distances z=0m, 0.04 m, 0.08 m, 0.12 m, 0.16 m, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    The modulation phase distributions and the intensity distributions at z=0 m and z=0.12 m versus the spiral phase θ when C0=1,φ0=0 for different factors m and n. (a) m=0,n=3; (b) m=1,n=2.
    Fig. 7. The modulation phase distributions and the intensity distributions at z=0m and z=0.12m versus the spiral phase θ when C0=1,φ0=0 for different factors m and n. (a) m=0,n=3; (b) m=1,n=2.
    Intensity and phase patterns of RAGB with CMOV for various φ0 at the distance z=0.12 m when C0=1,m=1, and n=2. (a1)–(a5) The beam spots for φ0=0,π2,π,3π2,2π, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    Fig. 8. Intensity and phase patterns of RAGB with CMOV for various φ0 at the distance z=0.12m when C0=1,m=1, and n=2. (a1)–(a5) The beam spots for φ0=0,π2,π,3π2,2π, respectively; (b1)–(b5) are the corresponding phase distributions of (a1)–(a5).
    Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12 m when C0=1,m=1, and φ0=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. 9. Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12m when C0=1,m=1, and φ0=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).
    (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. 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.
    Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12 m when C0=1,m=2, and φ0=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. 11. Intensity and phase patterns of RAGB with CMOV for various n at the distance z=0.12m when C0=1,m=2, and φ0=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).
    (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.
    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.
    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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