Geometric phase in beating of light waves

Beating is a simple physical phenomenon known for long in the context of sound waves but remained surprisingly unexplored for light waves. When two monochromatic optical beams of different frequencies and states of polarization interfere, the polarization state of the superposition field exhibits te...

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Main Authors: Antti Hannonen, Kimmo Saastamoinen, Lasse-Petteri Leppänen, Matias Koivurova, Andriy Shevchenko, Ari T Friberg, Tero Setälä
Format: Article
Language:English
Published: IOP Publishing 2019-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ab3740
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author Antti Hannonen
Kimmo Saastamoinen
Lasse-Petteri Leppänen
Matias Koivurova
Andriy Shevchenko
Ari T Friberg
Tero Setälä
author_facet Antti Hannonen
Kimmo Saastamoinen
Lasse-Petteri Leppänen
Matias Koivurova
Andriy Shevchenko
Ari T Friberg
Tero Setälä
author_sort Antti Hannonen
collection DOAJ
description Beating is a simple physical phenomenon known for long in the context of sound waves but remained surprisingly unexplored for light waves. When two monochromatic optical beams of different frequencies and states of polarization interfere, the polarization state of the superposition field exhibits temporal periodic variation—polarization beating. In this work, we reveal a foundational and elegant phase structure underlying such polarization beating. We show that the phase difference over a single beating period decomposes into the Pancharatnam–Berry geometric phase and a dynamical phase of which the former depends exclusively on the intensities and polarization states of the interfering beams whereas the sum of the phases is determined solely by the beam frequencies. Varying the intensity and polarization characteristics of the beams, the relative contributions of the geometric and dynamical phases can be adjusted. The geometric phase inherent in polarization beating is governed by a compact expression containing only the Stokes parameters of the interfering waves and can alternatively be obtained from the individual beam intensities and the amplitude of the intensity beats. We demonstrate both approaches experimentally by using an interferometer with a fast detector and a specific polarimetric arrangement. Polarization beating has a unique character that the geometric and dynamical phases are entangled, i.e. variation in one unavoidably leads to a change in the other. Our work expands geometric phases into a new domain and offers important novel insight into the role of polarization in interference of electromagnetic waves.
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spelling doaj.art-afa1058bb4ca4dea90a29394963392ea2023-08-08T15:40:07ZengIOP PublishingNew Journal of Physics1367-26302019-01-0121808303010.1088/1367-2630/ab3740Geometric phase in beating of light wavesAntti Hannonen0Kimmo Saastamoinen1Lasse-Petteri Leppänen2Matias Koivurova3https://orcid.org/0000-0001-6100-6316Andriy Shevchenko4Ari T Friberg5Tero Setälä6Institute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandInstitute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandInstitute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandInstitute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandDepartment of Applied Physics, Aalto University , PO Box 13500, FI-00076 Aalto, FinlandInstitute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandInstitute of Photonics, University of Eastern Finland , PO Box 111, FI-80101 Joensuu, FinlandBeating is a simple physical phenomenon known for long in the context of sound waves but remained surprisingly unexplored for light waves. When two monochromatic optical beams of different frequencies and states of polarization interfere, the polarization state of the superposition field exhibits temporal periodic variation—polarization beating. In this work, we reveal a foundational and elegant phase structure underlying such polarization beating. We show that the phase difference over a single beating period decomposes into the Pancharatnam–Berry geometric phase and a dynamical phase of which the former depends exclusively on the intensities and polarization states of the interfering beams whereas the sum of the phases is determined solely by the beam frequencies. Varying the intensity and polarization characteristics of the beams, the relative contributions of the geometric and dynamical phases can be adjusted. The geometric phase inherent in polarization beating is governed by a compact expression containing only the Stokes parameters of the interfering waves and can alternatively be obtained from the individual beam intensities and the amplitude of the intensity beats. We demonstrate both approaches experimentally by using an interferometer with a fast detector and a specific polarimetric arrangement. Polarization beating has a unique character that the geometric and dynamical phases are entangled, i.e. variation in one unavoidably leads to a change in the other. Our work expands geometric phases into a new domain and offers important novel insight into the role of polarization in interference of electromagnetic waves.https://doi.org/10.1088/1367-2630/ab3740polarizationgeometric phasePancharatnam–Berry phaseinterferometry
spellingShingle Antti Hannonen
Kimmo Saastamoinen
Lasse-Petteri Leppänen
Matias Koivurova
Andriy Shevchenko
Ari T Friberg
Tero Setälä
Geometric phase in beating of light waves
New Journal of Physics
polarization
geometric phase
Pancharatnam–Berry phase
interferometry
title Geometric phase in beating of light waves
title_full Geometric phase in beating of light waves
title_fullStr Geometric phase in beating of light waves
title_full_unstemmed Geometric phase in beating of light waves
title_short Geometric phase in beating of light waves
title_sort geometric phase in beating of light waves
topic polarization
geometric phase
Pancharatnam–Berry phase
interferometry
url https://doi.org/10.1088/1367-2630/ab3740
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AT andriyshevchenko geometricphaseinbeatingoflightwaves
AT aritfriberg geometricphaseinbeatingoflightwaves
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