• Chinese Optics Letters
  • Vol. 22, Issue 2, 020501 (2024)
Shang Gao1,*, María del Mar Sánchez-López1,2,**, and Ignacio Moreno1,3
Author Affiliations
  • 1Instituto de Bioingeniería, Universidad Miguel Hernández, Elche 03202, Spain
  • 2Departamento de Física Aplicada, Universidad Miguel Hernández, Elche 03202, Spain
  • 3Departamento de Ciencia de Materiales, Óptica y Tec. Electrónica, Universidad Miguel Hernández, Elche 03202, Spain
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    DOI: 10.3788/COL202422.020501 Cite this Article Set citation alerts
    Shang Gao, María del Mar Sánchez-López, Ignacio Moreno, "Experimental implementation of phase triplicator gratings in a spatial light modulator," Chin. Opt. Lett. 22, 020501 (2024) Copy Citation Text show less
    Experimental setup. At, variable attenuator; P1, P2, P3, linear polarizers; L1, L2, convergent lenses; QWP, quarter-wave plate; SF, spatial filter; Ap, circular aperture.
    Fig. 1. Experimental setup. At, variable attenuator; P1, P2, P3, linear polarizers; L1, L2, convergent lenses; QWP, quarter-wave plate; SF, spatial filter; Ap, circular aperture.
    Binary phase grating. (a) Normalized intensity of diffraction orders versus phase level; (b) experimental diffraction patterns for different phase values.
    Fig. 2. Binary phase grating. (a) Normalized intensity of diffraction orders versus phase level; (b) experimental diffraction patterns for different phase values.
    Sinusoidal phase grating. (a) Normalized intensity versus parameter a; (b) experimental diffraction patterns.
    Fig. 3. Sinusoidal phase grating. (a) Normalized intensity versus parameter a; (b) experimental diffraction patterns.
    Gori’s optimum triplicator. (a) Phase profile for a = 1, a = 2.65, and a = 8; (b) theoretical and experimental normalized intensity of the 0th and ±1st orders versus a; (c) experimental diffraction patterns for different values of a.
    Fig. 4. Gori’s optimum triplicator. (a) Phase profile for a = 1, a = 2.65, and a = 8; (b) theoretical and experimental normalized intensity of the 0th and ±1st orders versus a; (c) experimental diffraction patterns for different values of a.
    Quantized phase profile. Inset, for N = 20 versus Gori’s.
    Fig. 5. Quantized phase profile. Inset, for N = 20 versus Gori’s.
    Calculated diffraction efficiency of the quantized triplicator as a function of N. (a) η0±1; (b) η±2 and η±3; (c) experimental diffraction patterns with N = 2, 3, 5, and 20.
    Fig. 6. Calculated diffraction efficiency of the quantized triplicator as a function of N. (a) η0±1; (b) η±2 and η±3; (c) experimental diffraction patterns with N = 2, 3, 5, and 20.
    (a) Illustration of the gray-level image addressed to the SLM and (b) the corresponding experimental diffraction patterns for a uniform phase, a positive and a negative blazed gratings, and the random triplicator generated by randomly addressing to 4 × 4 macropixels the phase of either the uniform grating or that of the positive or the negative blazed grating.
    Fig. 7. (a) Illustration of the gray-level image addressed to the SLM and (b) the corresponding experimental diffraction patterns for a uniform phase, a positive and a negative blazed gratings, and the random triplicator generated by randomly addressing to 4 × 4 macropixels the phase of either the uniform grating or that of the positive or the negative blazed grating.
    Shang Gao, María del Mar Sánchez-López, Ignacio Moreno, "Experimental implementation of phase triplicator gratings in a spatial light modulator," Chin. Opt. Lett. 22, 020501 (2024)
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