• Photonics Research
  • Vol. 5, Issue 3, 251 (2017)
Shiyao Fu1, Tonglu Wang2, Shikun Zhang1, Zheyuan Zhang1, Yanwang Zhai1, and Chunqing Gao1、*
Author Affiliations
  • 1School of Opto-Electronics, Beijing Institute of Technology, Beijing 100081, China
  • 2School of Physics, Beijing Institute of Technology, Beijing 100081, China
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    DOI: 10.1364/PRJ.5.000251 Cite this Article Set citation alerts
    Shiyao Fu, Tonglu Wang, Shikun Zhang, Zheyuan Zhang, Yanwang Zhai, Chunqing Gao. Non-probe compensation of optical vortices carrying orbital angular momentum[J]. Photonics Research, 2017, 5(3): 251 Copy Citation Text show less
    Concept of the GS-based non-probe pre-compensation of distorted optical vortices.
    Fig. 1. Concept of the GS-based non-probe pre-compensation of distorted optical vortices.
    Computing the pre-compensation phase mask C(x,y) based on GS algorithm. (a) Flow chart. (b) C(x,y) can be obtained through subtracting the iteration output φ(x,y) from the initial helical phase of the transmitted optical vortices S(x,y).
    Fig. 2. Computing the pre-compensation phase mask C(x,y) based on GS algorithm. (a) Flow chart. (b) C(x,y) can be obtained through subtracting the iteration output φ(x,y) from the initial helical phase of the transmitted optical vortices S(x,y).
    Experimental setup. Col., collimator; L, convex lens; CCD, infrared CCD camera; ID, iris diaphragm; PM, power meter.
    Fig. 3. Experimental setup. Col., collimator; L, convex lens; CCD, infrared CCD camera; ID, iris diaphragm; PM, power meter.
    Observed intensity profiles of optical vortices. (a) No turbulence. (b) With turbulence r0=1 mm. (c) With turbulence r0=3 mm.
    Fig. 4. Observed intensity profiles of optical vortices. (a) No turbulence. (b) With turbulence r0=1  mm. (c) With turbulence r0=3  mm.
    Received power of diverse OAM channels with or without pre-compensation when |+2⟩ is transmitted. (a) Case of strong turbulence with Fried parameter r0=1 mm and d/r0=3.46. (b) Case of weak turbulence with Fried parameter r0=3 mm and d/r0=1.15. The number of iterations of the GS algorithm is 100.
    Fig. 5. Received power of diverse OAM channels with or without pre-compensation when |+2 is transmitted. (a) Case of strong turbulence with Fried parameter r0=1  mm and d/r0=3.46. (b) Case of weak turbulence with Fried parameter r0=3  mm and d/r0=1.15. The number of iterations of the GS algorithm is 100.
    Mode purity of vortex beams (|+2⟩, |+3⟩) with and without compensation for various turbulence realizations (r0=1 mm for |+2⟩, d/r0=3.46 and |+3⟩, d/r0=4; r0=3 mm for |+2⟩, d/r0=1.15 and |+3⟩, d/r0=1.33). The number of iterations of the GS algorithm under all turbulence realizations is 100.
    Fig. 6. Mode purity of vortex beams (|+2, |+3) with and without compensation for various turbulence realizations (r0=1  mm for |+2, d/r0=3.46 and |+3, d/r0=4; r0=3  mm for |+2, d/r0=1.15 and |+3, d/r0=1.33). The number of iterations of the GS algorithm under all turbulence realizations is 100.
    Mode purities of a beam with topological charge l=2, as a function of number of iterations, at two turbulence values of different strength (Fried parameter r0=1 mm and r0=3 mm).
    Fig. 7. Mode purities of a beam with topological charge l=2, as a function of number of iterations, at two turbulence values of different strength (Fried parameter r0=1  mm and r0=3  mm).
    Shiyao Fu, Tonglu Wang, Shikun Zhang, Zheyuan Zhang, Yanwang Zhai, Chunqing Gao. Non-probe compensation of optical vortices carrying orbital angular momentum[J]. Photonics Research, 2017, 5(3): 251
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