• Opto-Electronic Advances
  • Vol. 4, Issue 12, 210027-1 (2021)
Yonglei Liu, Yahong Chen, Fei Wang*, Yangjian Cai*, Chunhao Liang*, and Olga Korotkova
DOI: 10.29026/oea.2021.210027 Cite this Article
Yonglei Liu, Yahong Chen, Fei Wang, Yangjian Cai, Chunhao Liang, Olga Korotkova. Robust far-field imaging by spatial coherence engineering[J]. Opto-Electronic Advances, 2021, 4(12): 210027-1 Copy Citation Text show less
Variation of the modulus of DOC |μ| of a CGCSM beam with the propagation distance z after the focusing lens, with the CP strength factor (a1−a4) u = 0 mm−2, (b1−b4) u = 2 mm−2, (c1−c4) u = 10 mm−2, and (d1−d4) u = 70 mm−2. The parameters are set as λ = 532 nm, δ0 =0.5 mm and n=1.
Fig. 1. Variation of the modulus of DOC |μ| of a CGCSM beam with the propagation distance z after the focusing lens, with the CP strength factor (a1a4) u = 0 mm−2, (b1b4) u = 2 mm−2, (c1c4) u = 10 mm−2, and (d1d4) u = 70 mm−2. The parameters are set as λ = 532 nm, δ0 =0.5 mm and n=1.
Theoretical results of the modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2. The inserted letter “S” in (a) is adopted as the power spectral density P(v) function.
Fig. 2. Theoretical results of the modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2. The inserted letter “S” in (a) is adopted as the power spectral density P(v) function.
Schematic diagram of the experiment setup for generation of Schell-model beams with a controllable CP structure, measurement of the modulus of the DOC in the far field propagation in free space as well as in turbulent atmosphere. Laser, a Nd:YAG laser with wavelength 532nm; M, mirror; BE, beam expander; SLM1, SLM2, spatial light modulator; RGGD, rotating ground glass disk; L1, L2, L3, L4, L5, L6, thin lenses with the identical focal length f=250mm; GAF, Gaussian amplitude filter; BS, beam splitter; CA, circular aperture; SP, source plane; CCD, charge-coupled device; HP, hot plate; PC1, PC2, PC3, personal computers.
Fig. 3. Schematic diagram of the experiment setup for generation of Schell-model beams with a controllable CP structure, measurement of the modulus of the DOC in the far field propagation in free space as well as in turbulent atmosphere. Laser, a Nd:YAG laser with wavelength 532nm; M, mirror; BE, beam expander; SLM1, SLM2, spatial light modulator; RGGD, rotating ground glass disk; L1, L2, L3, L4, L5, L6, thin lenses with the identical focal length f=250mm; GAF, Gaussian amplitude filter; BS, beam splitter; CA, circular aperture; SP, source plane; CCD, charge-coupled device; HP, hot plate; PC1, PC2, PC3, personal computers.
(a−d) Experimental results of the modulus of the DOC |μ| in the focal plane with different strength factors u. (e−h) The modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2.
Fig. 4. (ad) Experimental results of the modulus of the DOC |μ| in the focal plane with different strength factors u. (eh) The modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2.
Experimental results of the modulus of the DOC |μ| in the focal plane at different temperatures of the HP. The strength factor of the CP is u=−60 mm−2. T=0 °C stands for the free space case.
Fig. 5. Experimental results of the modulus of the DOC |μ| in the focal plane at different temperatures of the HP. The strength factor of the CP is u=−60 mm−2. T=0 °C stands for the free space case.
Experimental results of the dependence of the quality of the recovered image on the strength factor u in the focal plane in free space.
Fig. 6. Experimental results of the dependence of the quality of the recovered image on the strength factor u in the focal plane in free space.
(a−c) Simulation results of the reconstructed image in turbulence of different strength and with different CP strength factor u. (d−f) Experimental results of the reconstructed image at different temperatures with u=−60 mm−2.
Fig. 7. (ac) Simulation results of the reconstructed image in turbulence of different strength and with different CP strength factor u. (df) Experimental results of the reconstructed image at different temperatures with u=−60 mm−2.
(a) A typical instantaneous intensity captured by the CCD. (b) Experimental results of the recovered image through the area surrounded by the yellow dashed square shown in subplot (a) covering 1440×1440 pixels. (c) The recovered image through the area surrounded by the red dashed square shown in subplot (a) covering 500×500 pixels.
Fig. 8. (a) A typical instantaneous intensity captured by the CCD. (b) Experimental results of the recovered image through the area surrounded by the yellow dashed square shown in subplot (a) covering 1440×1440 pixels. (c) The recovered image through the area surrounded by the red dashed square shown in subplot (a) covering 500×500 pixels.
Yonglei Liu, Yahong Chen, Fei Wang, Yangjian Cai, Chunhao Liang, Olga Korotkova. Robust far-field imaging by spatial coherence engineering[J]. Opto-Electronic Advances, 2021, 4(12): 210027-1
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