2022
DOI: 10.1088/2040-8986/ac6960
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Orbital angular momentum sidebands in second harmonic generation of a vortex beam by a nonlinear crystal with inhomogeneous refractive index

Abstract: The manipulation of the orbital angular momentum (OAM) spectrum in new wavelengths generated by frequency conversion has a wide range of applications in quantum information technology and modern communications. Here, the second harmonic generation (SHG) of a vortex beam in a nonlinear crystal with an inhomogeneous refractive index is considered. It is shown that by using a segmented oven and generating a controllable temperature gradient along the thickness of the nonlinear crystal, a transverse phase mismatch… Show more

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Cited by 3 publications
(2 citation statements)
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“…The fork element should be an array of positive numbers in the range of [0, 1] and be able to produce superposed vortex beams with high fidelity. First of all, the hologram h(x, y) of each LG basis mode of a superposition, is designed in the form of [31]: (8) where, a(x, y) is the normalized amplitude distribution, and (u 0 , v 0 ) are the spatial frequencies of the periodic grating. Secondly, to associate the phase of modal coefficient θ ℓ with the related basis LG mode, we develop equation (8) which is given by:…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The fork element should be an array of positive numbers in the range of [0, 1] and be able to produce superposed vortex beams with high fidelity. First of all, the hologram h(x, y) of each LG basis mode of a superposition, is designed in the form of [31]: (8) where, a(x, y) is the normalized amplitude distribution, and (u 0 , v 0 ) are the spatial frequencies of the periodic grating. Secondly, to associate the phase of modal coefficient θ ℓ with the related basis LG mode, we develop equation (8) which is given by:…”
Section: Resultsmentioning
confidence: 99%
“…They carry orbital angular momentum (OAM) with a phase of the form e iℓφ , where φ is the azimuthal angle, and ℓ is the helicity or topological charge [3,4]. They have found numerous applications in a variety of optical systems, such as material processing [5], optical tweezers [6], micromanipulation [7], nonlinear frequencyconversion processes [8,9], and optical communications [10,11]. Multiplexing OAM modes enables high-capacity optical communication.…”
Section: Introductionmentioning
confidence: 99%