2020
DOI: 10.3390/app10061966
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Spatial Manipulation of a Supercontinuum Beam for the Study of Vortex Interference Effects

Abstract: In this work, we generate optical vortices from the supercontinuum output of an ultrafast laser interacting with a micro-structured fiber. Using a segmented spatial light modulator, multiple vortices are designed and dynamically generated and shifted in order to observe their superposition in the image plane. It is shown that single-color patterns of exquisite complexity can be generated across a wide frequency range. Multi-color interference patterns are experimentally generated and compared to the results of… Show more

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Cited by 2 publications
(7 citation statements)
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“…Since the angular derivative of Equation ( 7) is ∂E(r, ϕ, z)/∂ϕ = inE(r, ϕ, z), then, according to Equation (3), the TC of the superposition (7) with arbitrary colors is equal to the TC of each beam: TC = n. This result is simple, but practical generation of the superposition (7) is challenging, since it requires that, in the waist planes of each colored Gaussian beam, different SPPs be placed, the maximal relief depth h s of which is matched with the wavelength λ s of the incident light: 2πh s (n 0 − 1) = nλ s , with n 0 being the refractive index of the SPP material (we suppose that there is no dispersion of the refractive index). However, if an amplitude fork grating is used, as in [9,18], then all spectral components of the beam have the same TC. However, due to diffraction by the grating, monochromatic beam components diffract by different angles.…”
Section: Topological Charge Of a Two-color Superposition Of Optical V...mentioning
confidence: 99%
See 4 more Smart Citations
“…Since the angular derivative of Equation ( 7) is ∂E(r, ϕ, z)/∂ϕ = inE(r, ϕ, z), then, according to Equation (3), the TC of the superposition (7) with arbitrary colors is equal to the TC of each beam: TC = n. This result is simple, but practical generation of the superposition (7) is challenging, since it requires that, in the waist planes of each colored Gaussian beam, different SPPs be placed, the maximal relief depth h s of which is matched with the wavelength λ s of the incident light: 2πh s (n 0 − 1) = nλ s , with n 0 being the refractive index of the SPP material (we suppose that there is no dispersion of the refractive index). However, if an amplitude fork grating is used, as in [9,18], then all spectral components of the beam have the same TC. However, due to diffraction by the grating, monochromatic beam components diffract by different angles.…”
Section: Topological Charge Of a Two-color Superposition Of Optical V...mentioning
confidence: 99%
“…However, due to diffraction by the grating, monochromatic beam components diffract by different angles. Therefore, in [18], light rings of different colors are shifted relative to each other. This shift can be compensated by a prism.…”
Section: Topological Charge Of a Two-color Superposition Of Optical V...mentioning
confidence: 99%
See 3 more Smart Citations