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A Kerr polarization controller

Author

Listed:
  • N. Moroney

    (Max Planck Institute for the Science of Light
    QOLS, Blackett Laboratory, Imperial College London)

  • L. Del Bino

    (Max Planck Institute for the Science of Light)

  • S. Zhang

    (Max Planck Institute for the Science of Light)

  • M. T. M. Woodley

    (Max Planck Institute for the Science of Light
    QOLS, Blackett Laboratory, Imperial College London
    SUPA and Department of Physics, Heriot-Watt)

  • L. Hill

    (Max Planck Institute for the Science of Light
    SUPA and Department of Physics, University of Strathclyde)

  • T. Wildi

    (Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY)

  • V. J. Wittwer

    (Laboratoire Temps-Fréquence, Université de Neuchâtel)

  • T. Südmeyer

    (Laboratoire Temps-Fréquence, Université de Neuchâtel)

  • G.-L. Oppo

    (SUPA and Department of Physics, University of Strathclyde)

  • M. R. Vanner

    (QOLS, Blackett Laboratory, Imperial College London)

  • V. Brasch

    (Swiss Center for Electronics and Microtechnology (CSEM), Time and Frequency)

  • T. Herr

    (Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY
    Physics Department, Universität Hamburg)

  • P. Del’Haye

    (Max Planck Institute for the Science of Light
    Department of Physics, Friedrich Alexander University Erlangen-Nuremberg)

Abstract

Kerr-effect-induced changes of the polarization state of light are well known in pulsed laser systems. An example is nonlinear polarization rotation, which is critical to the operation of many types of mode-locked lasers. Here, we demonstrate that the Kerr effect in a high-finesse Fabry-Pérot resonator can be utilized to control the polarization of a continuous wave laser. It is shown that a linearly-polarized input field is converted into a left- or right-circularly-polarized field, controlled via the optical power. The observations are explained by Kerr-nonlinearity induced symmetry breaking, which splits the resonance frequencies of degenerate modes with opposite polarization handedness in an otherwise symmetric resonator. The all-optical polarization control is demonstrated at threshold powers down to 7 mW. The physical principle of such Kerr effect-based polarization controllers is generic to high-Q Kerr-nonlinear resonators and could also be implemented in photonic integrated circuits. Beyond polarization control, the spontaneous symmetry breaking of polarization states could be used for polarization filters or highly sensitive polarization sensors when operating close to the symmetry-breaking point.

Suggested Citation

  • N. Moroney & L. Del Bino & S. Zhang & M. T. M. Woodley & L. Hill & T. Wildi & V. J. Wittwer & T. Südmeyer & G.-L. Oppo & M. R. Vanner & V. Brasch & T. Herr & P. Del’Haye, 2022. "A Kerr polarization controller," Nature Communications, Nature, vol. 13(1), pages 1-8, December.
  • Handle: RePEc:nat:natcom:v:13:y:2022:i:1:d:10.1038_s41467-021-27933-x
    DOI: 10.1038/s41467-021-27933-x
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    References listed on IDEAS

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    1. L. E. Sadler & J. M. Higbie & S. R. Leslie & M. Vengalattore & D. M. Stamper-Kurn, 2006. "Spontaneous symmetry breaking in a quenched ferromagnetic spinor Bose–Einstein condensate," Nature, Nature, vol. 443(7109), pages 312-315, September.
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    Cited by:

    1. Stéphane Coen & Bruno Garbin & Gang Xu & Liam Quinn & Nathan Goldman & Gian-Luca Oppo & Miro Erkintalo & Stuart G. Murdoch & Julien Fatome, 2024. "Nonlinear topological symmetry protection in a dissipative system," Nature Communications, Nature, vol. 15(1), pages 1-11, December.

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