Sharp focusing of a light field with polarization and phase singularities of an arbitrary order

Using the Richards-Wolf formalism, we obtain general expressions for all components of the electric and magnetic strength vectors near the sharp focus of an optical vortex with the topological charge m and nth-order azimuthal polarization. From these equations, simple consequences are derived for di...

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Main Authors: Victor Kotlyar, Sergey Stafeev, Alexey Kovalev
Format: Article
Language:English
Published: Samara National Research University 2019-06-01
Series:Компьютерная оптика
Subjects:
Online Access:http://computeroptics.smr.ru/KO/PDF/KO43-3/430301.pdf
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spelling doaj-e82b7e16f3b8415da8de9bb949ccd13a2020-11-25T00:42:28ZengSamara National Research UniversityКомпьютерная оптика0134-24522412-61792019-06-0143333734610.18287/2412-6179-2019-43-3-337-346Sharp focusing of a light field with polarization and phase singularities of an arbitrary orderVictor Kotlyar0Sergey Stafeev1Alexey Kovalev 2IPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, 443001, Samara, Russia; Samara National Research University, Moskovskoye shosse, 34, 443086, Samara, RussiaIPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, 443001, Samara, Russia; Samara National Research University, Moskovskoye shosse, 34, 443086, Samara, RussiaIPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, 443001, Samara, Russia; Samara National Research University, Moskovskoye shosse, 34, 443086, Samara, RussiaUsing the Richards-Wolf formalism, we obtain general expressions for all components of the electric and magnetic strength vectors near the sharp focus of an optical vortex with the topological charge m and nth-order azimuthal polarization. From these equations, simple consequences are derived for different values of m and n. If m=n>1, there is a non-zero intensity on the optical axis, like the one observed when focusing a vortex-free circularly polarized light field. If n=m+2, there is a reverse flux of light energy near the optical axis in the focal plane. The derived expressions can be used both for simulating the sharp focusing of optical fields with the double singularity (phase and polarization) and for a theoretical analysis of focal distributions of the intensity and the Poynting vector, allowing one to reveal the presence of rotational symmetry or the on-axis reverse energy flux, as well as the focal spot shape (a circle or a doughnut).http://computeroptics.smr.ru/KO/PDF/KO43-3/430301.pdfsharp focusingRichards-Wolf formulaeoptical vortextopological chargephase singularitypolarization singularityPoynting vectorreverse flux of energyfocal spot symmetry Citation
collection DOAJ
language English
format Article
sources DOAJ
author Victor Kotlyar
Sergey Stafeev
Alexey Kovalev
spellingShingle Victor Kotlyar
Sergey Stafeev
Alexey Kovalev
Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
Компьютерная оптика
sharp focusing
Richards-Wolf formulae
optical vortex
topological charge
phase singularity
polarization singularity
Poynting vector
reverse flux of energy
focal spot symmetry Citation
author_facet Victor Kotlyar
Sergey Stafeev
Alexey Kovalev
author_sort Victor Kotlyar
title Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
title_short Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
title_full Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
title_fullStr Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
title_full_unstemmed Sharp focusing of a light field with polarization and phase singularities of an arbitrary order
title_sort sharp focusing of a light field with polarization and phase singularities of an arbitrary order
publisher Samara National Research University
series Компьютерная оптика
issn 0134-2452
2412-6179
publishDate 2019-06-01
description Using the Richards-Wolf formalism, we obtain general expressions for all components of the electric and magnetic strength vectors near the sharp focus of an optical vortex with the topological charge m and nth-order azimuthal polarization. From these equations, simple consequences are derived for different values of m and n. If m=n>1, there is a non-zero intensity on the optical axis, like the one observed when focusing a vortex-free circularly polarized light field. If n=m+2, there is a reverse flux of light energy near the optical axis in the focal plane. The derived expressions can be used both for simulating the sharp focusing of optical fields with the double singularity (phase and polarization) and for a theoretical analysis of focal distributions of the intensity and the Poynting vector, allowing one to reveal the presence of rotational symmetry or the on-axis reverse energy flux, as well as the focal spot shape (a circle or a doughnut).
topic sharp focusing
Richards-Wolf formulae
optical vortex
topological charge
phase singularity
polarization singularity
Poynting vector
reverse flux of energy
focal spot symmetry Citation
url http://computeroptics.smr.ru/KO/PDF/KO43-3/430301.pdf
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