• Advanced Photonics Nexus
  • Vol. 3, Issue 1, 016005 (2024)
Tian Xia1, Zhenwei Xie1、*, and Xiaocong Yuan1、2、*
Author Affiliations
  • 1Shenzhen University, Institute of Microscale Optoelectronics, Nanophotonics Research Centre, State Key Laboratory of Radio Frequency Heterogeneous Integration, Shenzhen, China
  • 2Research Institute of Intelligent Sensing, Research Center for Humanoid Sensing, Zhejiang Lab, Hangzhou, China
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    DOI: 10.1117/1.APN.3.1.016005 Cite this Article Set citation alerts
    Tian Xia, Zhenwei Xie, Xiaocong Yuan. Multidimensional multiplexing holography based on optical orbital angular momentum lattice multiplexing[J]. Advanced Photonics Nexus, 2024, 3(1): 016005 Copy Citation Text show less
    Schematic diagrams of two types of holograms: (a) an OAM-preserved hologram and (b) an OAM-selective hologram. These holograms are designed to transfer the OAM property from an incident OAM beam to a holographic image and to reconstruct specific OAM channels, respectively. Top: the conventional OAM beam. Bottom: the proposed VL beam. {a1}* and {β1}* are the equivalent values of α2 and β1 for the conjugate phase of the encoded phase, respectively.
    Fig. 1. Schematic diagrams of two types of holograms: (a) an OAM-preserved hologram and (b) an OAM-selective hologram. These holograms are designed to transfer the OAM property from an incident OAM beam to a holographic image and to reconstruct specific OAM channels, respectively. Top: the conventional OAM beam. Bottom: the proposed VL beam. {a1}* and {β1}* are the equivalent values of α2 and β1 for the conjugate phase of the encoded phase, respectively.
    OAML mode selectivity. (a) Design concept for an OAM-preserved hologram and an OAM-selective hologram. (b) Mode selectivity of the constant l. (c) Mode selectivity of α. (d) Mode selectivity of β.
    Fig. 2. OAML mode selectivity. (a) Design concept for an OAM-preserved hologram and an OAM-selective hologram. (b) Mode selectivity of the constant l. (c) Mode selectivity of α. (d) Mode selectivity of β.
    (a) Schematic diagram of the experimental setup of OAML hologram. (b) The hologram loaded into the SLM consists of two components: the decoded phase and the OAM hologram.
    Fig. 3. (a) Schematic diagram of the experimental setup of OAML hologram. (b) The hologram loaded into the SLM consists of two components: the decoded phase and the OAM hologram.
    Schematic diagram of OAML multiplexed holography designed with key l. (a) Design process. (b)–(e) Experimental reconstruction results based on the l-dependence of the incident VL beams with (l=−1, −11, −21, −31, {α}*=−0.2π/2, −0.2π/2, −0.2π/2, −0.2π/2, {β}*=−0.001, −0.001, −0.001, −0.001), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Fig. 4. Schematic diagram of OAML multiplexed holography designed with key l. (a) Design process. (b)–(e) Experimental reconstruction results based on the l-dependence of the incident VL beams with (l=1, 11, 21, 31, {α}*=0.2π/2, 0.2π/2, 0.2π/2, 0.2π/2, {β}*=0.001, 0.001, 0.001, 0.001), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Schematic diagram of OAML multiplexed holography designed with key α. (a) Design process. (b)–(e) Experimental reconstruction results based on the α-dependence of the incident VL beams with (l=−1, −1, −1, −1, {α}*=−0.1π/2, −0.2π/2, −0.3π/2, −0.4π/2, {β}*=−0.001, −0.001, −0.001, −0.001), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Fig. 5. Schematic diagram of OAML multiplexed holography designed with key α. (a) Design process. (b)–(e) Experimental reconstruction results based on the α-dependence of the incident VL beams with (l=1, 1, 1, 1, {α}*=0.1π/2, 0.2π/2, 0.3π/2, 0.4π/2, {β}*=0.001, 0.001, 0.001, 0.001), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Schematic diagram of OAML multiplexed holography designed with key β. (a) Design process. (b)–(e) Experimental reconstruction results based on the β-dependence of the incident VL beams with (l=−1, −1, −1, −1, {α}*=−0.1π/2, −0.1π/2, −0.1π/2, −0.1π/2, {β}*=−0.001, −0.002, −0.003, −0.004), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Fig. 6. Schematic diagram of OAML multiplexed holography designed with key β. (a) Design process. (b)–(e) Experimental reconstruction results based on the β-dependence of the incident VL beams with (l=1, 1, 1, 1, {α}*=0.1π/2, 0.1π/2, 0.1π/2, 0.1π/2, {β}*=0.001, 0.002, 0.003, 0.004), respectively. (f)–(i) Capture intensity distributions of the above VL beams, respectively. (j) Experimental reconstruction results of the OAML-preserved holography.
    Tian Xia, Zhenwei Xie, Xiaocong Yuan. Multidimensional multiplexing holography based on optical orbital angular momentum lattice multiplexing[J]. Advanced Photonics Nexus, 2024, 3(1): 016005
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