Optical vortices with an infinite number of screw dislocations

In optical data transmission with using vortex laser beams, data can be encoded by the topological charge, which is theoretically unlimited. However, the topological charge of a single separate vortex (screw dislocation) is limited by possibilities of its generating. Therefore, we investigate here t...

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Main Author: A.A. Kovalev
Format: Article
Language:English
Published: Samara National Research University 2021-07-01
Series:Компьютерная оптика
Subjects:
Online Access:http://computeroptics.ru/eng/KO/Annot/KO45-4/450403e.html
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spelling doaj-a4baa2dabbdf45a1831f893e501ed71d2021-08-04T18:16:09ZengSamara National Research UniversityКомпьютерная оптика0134-24522412-61792021-07-0145449750510.18287/2412-6179-CO-866Optical vortices with an infinite number of screw dislocationsA.A. Kovalev0IPSI RAS – Branch of the FSRC "Crystallography and Photonics" RAS, 443001, Samara, Russia, Molodogvardeyskaya 151; Samara National Research University, 443086, Samara, Russia, Moskovskoye Shosse 34In optical data transmission with using vortex laser beams, data can be encoded by the topological charge, which is theoretically unlimited. However, the topological charge of a single separate vortex (screw dislocation) is limited by possibilities of its generating. Therefore, we investigate here three examples of multivortex Gaussian light fields (two beams are form-invariant and one beam is astigmatic) with an unbounded (countable) set of screw dislocations. As a result, such fields have an infinite topological charge. The first beam has the complex amplitude of the Gaussian beam, but multiplied by the cosine function with a squared vortex argument. Phase singularity points of such a beam reside in the waist plane on the Cartesian axes and their density grows with increasing distance from the optical axis. The transverse intensity distribution of such a beam has a shape of a four-pointed star. All the optical vortices in this beam has the same topological charge of +1. The second beam also has the complex amplitude of the Gaussian beam, multiplied by the vortex-argument cosine function, but the cosine is raised to an arbitrary power. This beam has a countable number of the optical vortices, which reside in the waist plane uniformly on one Cartesian axis and the topological charge of each vortex equals to power, to which the cosine function is raised. The transverse intensity distribution of such beam consists of two light spots residing on a straight line, orthogonal to a straight line with the optical vortices. Finally, the third beam is similar to the first one in many properties, but it is generated with a tilted cylindrical lens from a 1D parabolic-argument cosine grating.http://computeroptics.ru/eng/KO/Annot/KO45-4/450403e.htmloptical vortexscrew dislocationtopological chargeform-invariant beammultivortex beamorbital angular momentum
collection DOAJ
language English
format Article
sources DOAJ
author A.A. Kovalev
spellingShingle A.A. Kovalev
Optical vortices with an infinite number of screw dislocations
Компьютерная оптика
optical vortex
screw dislocation
topological charge
form-invariant beam
multivortex beam
orbital angular momentum
author_facet A.A. Kovalev
author_sort A.A. Kovalev
title Optical vortices with an infinite number of screw dislocations
title_short Optical vortices with an infinite number of screw dislocations
title_full Optical vortices with an infinite number of screw dislocations
title_fullStr Optical vortices with an infinite number of screw dislocations
title_full_unstemmed Optical vortices with an infinite number of screw dislocations
title_sort optical vortices with an infinite number of screw dislocations
publisher Samara National Research University
series Компьютерная оптика
issn 0134-2452
2412-6179
publishDate 2021-07-01
description In optical data transmission with using vortex laser beams, data can be encoded by the topological charge, which is theoretically unlimited. However, the topological charge of a single separate vortex (screw dislocation) is limited by possibilities of its generating. Therefore, we investigate here three examples of multivortex Gaussian light fields (two beams are form-invariant and one beam is astigmatic) with an unbounded (countable) set of screw dislocations. As a result, such fields have an infinite topological charge. The first beam has the complex amplitude of the Gaussian beam, but multiplied by the cosine function with a squared vortex argument. Phase singularity points of such a beam reside in the waist plane on the Cartesian axes and their density grows with increasing distance from the optical axis. The transverse intensity distribution of such a beam has a shape of a four-pointed star. All the optical vortices in this beam has the same topological charge of +1. The second beam also has the complex amplitude of the Gaussian beam, multiplied by the vortex-argument cosine function, but the cosine is raised to an arbitrary power. This beam has a countable number of the optical vortices, which reside in the waist plane uniformly on one Cartesian axis and the topological charge of each vortex equals to power, to which the cosine function is raised. The transverse intensity distribution of such beam consists of two light spots residing on a straight line, orthogonal to a straight line with the optical vortices. Finally, the third beam is similar to the first one in many properties, but it is generated with a tilted cylindrical lens from a 1D parabolic-argument cosine grating.
topic optical vortex
screw dislocation
topological charge
form-invariant beam
multivortex beam
orbital angular momentum
url http://computeroptics.ru/eng/KO/Annot/KO45-4/450403e.html
work_keys_str_mv AT aakovalev opticalvorticeswithaninfinitenumberofscrewdislocations
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