• Advanced Photonics Nexus
  • Vol. 2, Issue 3, 036013 (2023)
Nian Zhang1、2、3、4, Baoxing Xiong1、2、3、4, Xiang Zhang1、2、3、4, and Xiao Yuan1、2、3、4、*
Author Affiliations
  • 1Soochow University, School of Optoelectronic Science and Engineering, Suzhou, China
  • 2Soochow University, Collaborative Innovation Center of Suzhou Nano Science and Technology, Suzhou, China
  • 3Soochow University, Key Lab of Advanced Optical Manufacturing Technologies of Jiangsu Province, Suzhou, China
  • 4Soochow University, Key Lab of Modern Optical Technologies of Education Ministry of China, Suzhou, China
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    DOI: 10.1117/1.APN.2.3.036013 Cite this Article Set citation alerts
    Nian Zhang, Baoxing Xiong, Xiang Zhang, Xiao Yuan. Multiparameter encrypted orbital angular momentum multiplexed holography based on multiramp helicoconical beams[J]. Advanced Photonics Nexus, 2023, 2(3): 036013 Copy Citation Text show less
    (a1)–(a3) Phase distributions of the MHC beams. (b1)–(b3) Simulation of the spatial frequency distributions of the MHC beams. (c) Relationship between the TC and sampling constant d. (d) Principle of the MHC-OAM holography.
    Fig. 1. (a1)–(a3) Phase distributions of the MHC beams. (b1)–(b3) Simulation of the spatial frequency distributions of the MHC beams. (c) Relationship between the TC and sampling constant d. (d) Principle of the MHC-OAM holography.
    MHC-OAM mode selectivity. (a) Mode selectivity of the constant K. (b) Mode selectivity of the multiramp mixed screw-edge dislocations. (c) Relationship between the reconstructed normalized peak intensity and normalized factor r0. (d) Interference field distribution of the encoded MHC beam with r0=1 mm and decoded MHC beams with r0=0.8 mm, r0=0.95 mm, r0=1 mm, and r0=1.5 mm, respectively.
    Fig. 2. MHC-OAM mode selectivity. (a) Mode selectivity of the constant K. (b) Mode selectivity of the multiramp mixed screw-edge dislocations. (c) Relationship between the reconstructed normalized peak intensity and normalized factor r0. (d) Interference field distribution of the encoded MHC beam with r0=1  mm and decoded MHC beams with r0=0.8  mm, r0=0.95  mm, r0=1  mm, and r0=1.5  mm, respectively.
    (a) SNR as a function of the number of multiramp mixed screw-edge dislocations. (b) SNR as a function of the normalized factor.
    Fig. 3. (a) SNR as a function of the number of multiramp mixed screw-edge dislocations. (b) SNR as a function of the normalized factor.
    (a) Schematic diagram of the experimental setup of MHC-OAM holography. L1 and L2, lens; A, aperture; P, polarizer; BS, beam splitter; and SLM, spatial light modulator. (b) The hologram loaded into the SLM contains the decoded phase and OAM hologram.
    Fig. 4. (a) Schematic diagram of the experimental setup of MHC-OAM holography. L1 and L2, lens; A, aperture; P, polarizer; BS, beam splitter; and SLM, spatial light modulator. (b) The hologram loaded into the SLM contains the decoded phase and OAM hologram.
    Schematic diagram of MHC-OAM-multiplexed holography designed with key m. (a) Design process. (b)–(e) Experimental reconstruction results based on the m-dependence of the incident MHC beams with m=4, 5, 6, and 7, respectively. (f) Reconstruction holographic image by a planar wave.
    Fig. 5. Schematic diagram of MHC-OAM-multiplexed holography designed with key m. (a) Design process. (b)–(e) Experimental reconstruction results based on the m-dependence of the incident MHC beams with m=4, 5, 6, and 7, respectively. (f) Reconstruction holographic image by a planar wave.
    Schematic diagram of MHC-OAM-multiplexed holography designed with key r0. (a) Design process. (b)–(e) Experimental reconstruction results based on the r0-dependence of the incident MHC beams with r0=0.5, 0.6, 0.7, and 0.8 mm, respectively.
    Fig. 6. Schematic diagram of MHC-OAM-multiplexed holography designed with key r0. (a) Design process. (b)–(e) Experimental reconstruction results based on the r0-dependence of the incident MHC beams with r0=0.5, 0.6, 0.7, and 0.8 mm, respectively.
    Experimental reconstruction results of the α-K-encrypted MHC-OAM multiplexed holography. (a) The design process and (b)–(e) experimental reconstruction results.
    Fig. 7. Experimental reconstruction results of the α-K-encrypted MHC-OAM multiplexed holography. (a) The design process and (b)–(e) experimental reconstruction results.
    The experimental reconstruction results of the m-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Fig. 8. The experimental reconstruction results of the m-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Experimental reconstruction results of the r0-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Fig. 9. Experimental reconstruction results of the r0-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Experimental reconstruction results of the α-m-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Fig. 10. Experimental reconstruction results of the α-m-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b)–(e) experimental reconstruction results.
    Experimental reconstruction results of the α-m-r0-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b) experimental reconstruction results.
    Fig. 11. Experimental reconstruction results of the α-m-r0-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b) experimental reconstruction results.
    Experimental reconstruction results of the α-m-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b) experimental reconstruction results.
    Fig. 12. Experimental reconstruction results of the α-m-K-encrypted MHC-OAM-multiplexed holography. (a) Design process and (b) experimental reconstruction results.
    The encrypted images are encoded by the parameters α, m, r0, and K.
    Fig. 13. The encrypted images are encoded by the parameters α, m, r0, and K.
    Experimental reconstruction results of the α-m-r0-K-encrypted MHC-OAM-multiplexed holography.
    Fig. 14. Experimental reconstruction results of the α-m-r0-K-encrypted MHC-OAM-multiplexed holography.
    Nian Zhang, Baoxing Xiong, Xiang Zhang, Xiao Yuan. Multiparameter encrypted orbital angular momentum multiplexed holography based on multiramp helicoconical beams[J]. Advanced Photonics Nexus, 2023, 2(3): 036013
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