Отрывок: Eq. (5) is simplified significantly for α = pi/4 and z = 2f, since zx → ∞ and zy → ∞ for these values: ( ) ( ) 1 2 2 2 2 2 2 2 2 2 , , 2 2 exp , 4 2y x E z f i ik ik f w w f −ξ η = = − γ ×  ξ η ξη × ξ + η − − + γ γ γ   (7) where 1/2 2 2 2 2 161 x y f k w w   γ = +     . (8) It is seen in Eq. (7) that at the distance z = 2f the ellip- tic Gaussian beam (1) is rotated by 90 degrees and wid- ened since γ > 1...
Полная запись метаданных
Поле DC Значение Язык
dc.contributor.authorKotlyar, V.V.-
dc.contributor.authorKovalev, A.A.-
dc.date.accessioned2017-10-25 12:07:46-
dc.date.available2017-10-25 12:07:46-
dc.date.issued2017-08-
dc.identifierDspace\SGAU\20171020\65764ru
dc.identifier.citationKotlyar VV, Kovalev AA. Vortex-free laser beam with an orbital angular momentum. Computer Optics 2017; 41(4): 573-576ru
dc.identifier.urihttps://dx.doi.org/10.18287/2412-6179-2017-41-4-573-576-
dc.identifier.urihttp://repo.ssau.ru/handle/Zhurnal-Komputernaya-optika/Vortexfree-laser-beam-with-an-orbital-angular-momentum-65764-
dc.description.abstractWe show that if one cylindrical lens is placed in the Gaussian beam waist and another cylindrical lens is placed at some distance from the first one and rotated by some angle, then the laser beam after the second lens has an orbital angular momentum (OAM). An explicit analytical expression for the OAM of such a beam is obtained. Depending on the inter-lens distance, the OAM can be positive, negative, or zero. Such a laser beam has no isolated intensity nulls with a singular phase and it is not an optical vortex, but has an OAM. By choosing the radius of the beam waist of the source Gaussian beam, the focal lengths of the lenses and the distance between them, it is possible to generate a vortex-free laser beam equivalent to an optical vortex with a topological charge of several hundreds.ru
dc.description.sponsorshipThis work was funded by the Russian Science Foundation grant # 17-19-01186ru
dc.language.isoenru
dc.publisherСамарский университетru
dc.relation.ispartofseries41;4-
dc.subjectelliptic Gaussian beamru
dc.subjectcylindrical lensru
dc.subjectorbital angular momentumru
dc.titleVortex-free laser beam with an orbital angular momentumru
dc.typeArticleru
dc.textpartEq. (5) is simplified significantly for α = pi/4 and z = 2f, since zx → ∞ and zy → ∞ for these values: ( ) ( ) 1 2 2 2 2 2 2 2 2 2 , , 2 2 exp , 4 2y x E z f i ik ik f w w f −ξ η = = − γ ×  ξ η ξη × ξ + η − − + γ γ γ   (7) where 1/2 2 2 2 2 161 x y f k w w   γ = +     . (8) It is seen in Eq. (7) that at the distance z = 2f the ellip- tic Gaussian beam (1) is rotated by 90 degrees and wid- ened since γ > 1...-
dc.classindex.scsti29.31.15-
Располагается в коллекциях: Журнал "Компьютерная оптика"

Файлы этого ресурса:
Файл Описание Размер Формат  
410416.pdf368.5 kBAdobe PDFПросмотреть/Открыть



Все ресурсы в архиве электронных ресурсов защищены авторским правом, все права сохранены.