Optics Express · 2023 · 17 citations · 37 references
Natural SciencesPhysicsOpticsOptoelectronicsPhotonicsDiffractionFourier OpticsPhysical OpticsTopological MaterialsWave DiffractionWave OpticsBeam DiffractionDiffraction GratingsDiffraction In Periodic StructuresGaussian Beam OpticsGaussian Beam PropagationOptical VorticesOrthogonal Arrays
In this work, by providing comprehensive theoretical foundations, we revisit and improve a simple and efficient method that has been used for generation of 2D orthogonal arrays of optical vortices with components having different topological charges (TCs). This method has been implemented by the diffraction of a plane wave from 2D gratings where the gratings’ profiles are determined by iterative computational process. Here, based on the theoretical predictions, specifications of the diffraction gratings can be easily adjusted in a way to generate experimentally a heterogeneous vortex array with the desired power shares among different elements of the array. We use the diffraction of a Gaussian beam from a class of pure phase 2D orthogonal periodic structures having sinusoidal or binary profiles possessing a phase singularity, calling pure phase 2D fork-shaped gratings (FSGs). The transmittance of each of the introduced gratings is obtained by multiplying the transmittance of two pure phase 1D FSGs along x and y directions, having topological defect numbers l x and l y and phase variation amplitudes γ x and γ y , respectively. By solving the Fresnel integral, we show that the diffraction of a Gaussian beam from a pure phase 2D FSG leads to generation of a 2D array of vortex beams having different TCs and power shares. The power distribution among the generated optical vortices over the different diffraction orders can be adjusted by γ x and γ y , and it strongly depends on the profile of the grating. Meanwhile the TCs of the generated vortices depend on l x and l y and the corresponding diffraction orders, namely l m , n = −( ml x + nl y ) presents the TC of ( m , n )th diffraction order. We recorded the intensity patterns of the experimentally generated vortex arrays which are fully consistent with the theoretically predicted results. Furthermore, the TCs of the experimentally generated vortices are measured individually by the diffraction of each of them through a pure amplitude quadratic curved-line (parabolic-line) grating. The absolute values and signs of the measured TCs are consistent with the theoretical prediction. The generated configuration of vortices with adjustable TC and power sharing features might find many applications such as non-homogeneous mixing of a solution consisting trapped particles.
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