Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity
Using Jones matrices and vectors, we show that an optical metasurface composed of a set of subwavelength binary diffraction gratings and characterized by an anisotropic transmittance described by a polarization rotation matrix by the angle mφ, where φ is the polar angle, forms an m-th order azimutha...
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doaj-9781bcd5487c4bcfa472e280473bdd892020-11-25T01:20:32ZengSamara National Research UniversityКомпьютерная оптика0134-24522412-61792019-04-0143217418310.18287/2412-6179-2019-43-2-174-183Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularityVictor Kotlyar0Anton Nalimov1Sergey Stafeev2IPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, Samara, Russia, Samara National Research University, Moskovskoye shosse, 34, Samara, RussiaIPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, Samara, Russia, Samara National Research University, Moskovskoye shosse, 34, Samara, RussiaIPSI RAS – Branch of the FSRC “Crystallography and Photonics” RAS, Molodogvardeyskaya 151, Samara, Russia, Samara National Research University, Moskovskoye shosse, 34, Samara, RussiaUsing Jones matrices and vectors, we show that an optical metasurface composed of a set of subwavelength binary diffraction gratings and characterized by an anisotropic transmittance described by a polarization rotation matrix by the angle mφ, where φ is the polar angle, forms an m-th order azimuthally or radially polarized beam when illuminated by linearly polarized light, generating an optical vortex with the topological charge m upon illumination by circularly polarized light. Such a polarization-phase converter (PPC) performs a spin-orbit transformation, similar to that performed by liquid-crystal q-plates. Using a FDTD method, it is numerically shown that when illuminating the PPC by a uniformly (linearly or circularly) polarized field with topological charge m = 2 and then focusing the output beam with a binary zone plate, a reverse on-axis light flow is formed, being comparable in magnitude with the direct optical flow. Moreover, the reverse flows obtained when focusing the circularly polarized optical vortex with the topological charge m = 2 and the second-order polarization vortex are shown to be the same in magnitude.http://computeroptics.ru/KO/PDF/KO43-2/430203.pdfoptical vortexpolarizationbackward fluxmetalens |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Victor Kotlyar Anton Nalimov Sergey Stafeev |
spellingShingle |
Victor Kotlyar Anton Nalimov Sergey Stafeev Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity Компьютерная оптика optical vortex polarization backward flux metalens |
author_facet |
Victor Kotlyar Anton Nalimov Sergey Stafeev |
author_sort |
Victor Kotlyar |
title |
Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
title_short |
Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
title_full |
Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
title_fullStr |
Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
title_full_unstemmed |
Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
title_sort |
comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity |
publisher |
Samara National Research University |
series |
Компьютерная оптика |
issn |
0134-2452 2412-6179 |
publishDate |
2019-04-01 |
description |
Using Jones matrices and vectors, we show that an optical metasurface composed of a set of subwavelength binary diffraction gratings and characterized by an anisotropic transmittance described by a polarization rotation matrix by the angle mφ, where φ is the polar angle, forms an m-th order azimuthally or radially polarized beam when illuminated by linearly polarized light, generating an optical vortex with the topological charge m upon illumination by circularly polarized light. Such a polarization-phase converter (PPC) performs a spin-orbit transformation, similar to that performed by liquid-crystal q-plates. Using a FDTD method, it is numerically shown that when illuminating the PPC by a uniformly (linearly or circularly) polarized field with topological charge m = 2 and then focusing the output beam with a binary zone plate, a reverse on-axis light flow is formed, being comparable in magnitude with the direct optical flow. Moreover, the reverse flows obtained when focusing the circularly polarized optical vortex with the topological charge m = 2 and the second-order polarization vortex are shown to be the same in magnitude. |
topic |
optical vortex polarization backward flux metalens |
url |
http://computeroptics.ru/KO/PDF/KO43-2/430203.pdf |
work_keys_str_mv |
AT victorkotlyar comparisonofbackwardflowvaluesinthesharpfocusoflightfieldswithpolarizationandphasesingularity AT antonnalimov comparisonofbackwardflowvaluesinthesharpfocusoflightfieldswithpolarizationandphasesingularity AT sergeystafeev comparisonofbackwardflowvaluesinthesharpfocusoflightfieldswithpolarizationandphasesingularity |
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