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...
Название : Vortex-free laser beam with an orbital angular momentum
Авторы/Редакторы : Kotlyar, V.V.
Kovalev, A.A.
Ключевые слова : elliptic Gaussian beam
cylindrical lens
orbital angular momentum
Дата публикации : Авг-2017
Издательство : Самарский университет
Библиографическое описание : Kotlyar VV, Kovalev AA. Vortex-free laser beam with an orbital angular momentum. Computer Optics 2017; 41(4): 573-576
Серия/номер : 41;4
Аннотация : We 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.
URI (Унифицированный идентификатор ресурса) : https://dx.doi.org/10.18287/2412-6179-2017-41-4-573-576
http://repo.ssau.ru/handle/Zhurnal-Komputernaya-optika/Vortexfree-laser-beam-with-an-orbital-angular-momentum-65764
Другие идентификаторы : Dspace\SGAU\20171020\65764
ГРНТИ: 29.31.15
Располагается в коллекциях: Журнал "Компьютерная оптика"

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