Photonics Research, Volume. 13, Issue 2, 468(2025)

Rotational Doppler effect using ultra-dense vector perfect vortex beams

Jianbo Gao1, Xingyuan Lu1,5、*, Xuechun Zhao1, Zhuoyi Wang1, Junan Zhu1, Zhiquan Hu1, Jingjing He1, Qiwen Zhan2, Yangjian Cai3,4, and Chengliang Zhao1,6、*
Author Affiliations
  • 1School of Physical Science and Technology, Jiangsu Key Laboratory of Frontier Material Physics and Devices, Soochow University, Suzhou 215006, China
  • 2School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
  • 3Shandong Provincial Engineering and Technical Center of Light Manipulations & Shandong Provincial Key Laboratory of Optics and Photonic Device, School of Physics and Electronics, Shandong Normal University, Jinan 250358, China
  • 4Shandong Joint Research Center of Light Manipulation Science and Photonics Integrated Chip of East China Normal University and Shandong Normal University, East China Normal University, Shanghai 200241, China
  • 5e-mail: xylu@suda.edu.cn
  • 6e-mail: zhaochengliang@suda.edu.cn
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    Figures & Tables(8)
    Schematic diagram of the generation of ultra-dense vector perfect vortex beam and rotational Doppler frequency shift measurement. The setup comprises a spatial light modulator (SLM); two lenses (L1 and L2) with focal length 250 mm used to construct a 4-f system; polarizers (X-LP and Y-LP) with polarization along the x-axis and y-axis, respectively; a Ronchi grating (RG) used to synthesize x- and y-polarization components; a rotating object for detection (Rotor); and a photodetector (PD). Simulated beam intensities: (b) l=±6, (c) l=±(5,8,12) (from inner to outer), (d) l=±(3:3:36), (e) l=±(6,9,12,15) at multiple axes, (f) l=±(2:2:12) for detecting rotation radius, and (g) l=±(2:2:12) for detecting object size.
    Experimentally captured intensities and corresponding crosslines with l=6 and N=2, 4, 6, 8, 10, and 12: (a1)–(f2) scalar multi-ring perfect vortex beams, and (a3)–(f4) ultra-dense vector perfect vortex beams.
    Simulated and experimental intensities and corresponding crosslines of ultra-dense vector perfect vortex beams with l=6 and ω=0.15 mm, 0.10 mm, and 0.05 mm. (a1)–(c2) Simulation results. (d1)–(f2) Corresponding experimental results.
    Frequency spectra of rotational Doppler frequency shift of ultra-dense vector perfect vortex beams: (a) N=2, (b) N=4, (c) N=6, (d) N=8, (e) N=12. Insets show intensities. (f) Signal-to-noise ratio (SNR) of 20 datasets with error bar in red.
    Experimental generation of frequency combs. (a1)–(c1) Intensity distributions; (a2)–(c2) time-domain intensity fluctuations; and (a3)–(c3) frequency-domain signals.
    Simulation and experimental results of object size and location perception. Intensity used for detection: (a) simulated; (b) experimental. The TCs used to generate petal-like intensities are l=±(2:2:12) with radius interval Δr=0.25 mm. Object location sensing of ball object: (c) simulated; (d) experimental. Size detection of rectangular object: (e) simulated; (f) experimental.
    Simulation results of misalignment issues. Frequency combs of coaxial nested ultra-dense vector perfect vortex beam: (a) aligned and (b) misaligned. TCs of each ring are ±(6,9,12,15), located at radius 1.2, 1.8, 2.4, and 3.0 mm, respectively. Frequency combs of non-coaxial nested beam for misalignment issues. From the inner to the outer rings, shift is 0.1 mm in positive x-, positive y-, negative x-, and negative y-directions, and object rotation axis shifts 0.052 mm diagonally to (c) first quadrant, (d) second quadrant, (e) third quadrant, and (f) fourth quadrant, respectively. The red dashed line is the fitted envelope.
    Experimental results of error margin. (a) Frequency domain results with 100 s sampling time. (b) Mean peak value and error bar with different sampling times.
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    Jianbo Gao, Xingyuan Lu, Xuechun Zhao, Zhuoyi Wang, Junan Zhu, Zhiquan Hu, Jingjing He, Qiwen Zhan, Yangjian Cai, Chengliang Zhao, "Rotational Doppler effect using ultra-dense vector perfect vortex beams," Photonics Res. 13, 468 (2025)

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    Paper Information

    Category: Physical Optics

    Received: Aug. 5, 2024

    Accepted: Dec. 2, 2024

    Published Online: Feb. 10, 2025

    The Author Email: Xingyuan Lu (xylu@suda.edu.cn), Chengliang Zhao (zhaochengliang@suda.edu.cn)

    DOI:10.1364/PRJ.538590

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