2022
DOI: 10.37188/lam.2022.024
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Review of engineering techniques in chaotic coded aperture imagers

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Cited by 22 publications
(24 citation statements)
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“…For vortex-beam generation, the optical modulator is a spiral Fresnel lens with a phase of , where L is the topological charge and θ is the azimuthal angle given as [ 43 , 44 ]. For the generation of a scattered beam, the optical modulator is a quasi-random lens with a phase given as , where Φ R is the random phase matrix with a particular scattering degree synthesized using Gerchberg–Saxton algorithm (GSA) [ 2 , 15 , 26 ]. For the generation of accelerating Airy beams, the optical modulator is a cubic phase mask with a phase given as [ 45 ].…”
Section: Methodsmentioning
confidence: 99%
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“…For vortex-beam generation, the optical modulator is a spiral Fresnel lens with a phase of , where L is the topological charge and θ is the azimuthal angle given as [ 43 , 44 ]. For the generation of a scattered beam, the optical modulator is a quasi-random lens with a phase given as , where Φ R is the random phase matrix with a particular scattering degree synthesized using Gerchberg–Saxton algorithm (GSA) [ 2 , 15 , 26 ]. For the generation of accelerating Airy beams, the optical modulator is a cubic phase mask with a phase given as [ 45 ].…”
Section: Methodsmentioning
confidence: 99%
“…The noninterferometric indirect-imaging methods include transport of intensity equations-based imaging [ 11 , 12 ], ghost imaging [ 13 ] and coded-aperture imaging (CAI) [ 14 , 15 ]. In this review, only CAI is considered.…”
Section: Introductionmentioning
confidence: 99%
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“…For vortex-beam generation, the optical modulator is a spiral Fresnel lens with a phase of exp −j Lθ + πR 2 /λ (1/u + 1/v ) , where L is the topological charge and θ is the azimuthal angle given as θ = tan −1 (y/x) [43,44]. For the generation of a scattered beam, the optical modulator is a quasi-random lens with a phase given as exp −j πR 2 /λ (1/u + 1/v ) + Φ R , where Φ R is the random phase matrix with a particular scattering degree synthesized using Gerchberg-Saxton algorithm (GSA) [2,15,26]. For the generation of accelerating Airy beams, the optical modulator is a cubic phase mask with a phase given as exp −j(2π/λ)ζ x 3 + y 3 [45].…”
Section: Methodsmentioning
confidence: 99%
“…The noninterferometric indirect-imaging methods include transport of intensity equationsbased imaging [11,12], ghost imaging [13] and coded-aperture imaging (CAI) [14,15]. In this review, only CAI is considered.…”
Section: Introductionmentioning
confidence: 99%