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Observation of replica symmetry breaking in disordered nonlinear wave propagation

Author

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  • Davide Pierangeli

    (Università di Roma “La Sapienza”)

  • Andrea Tavani

    (Università di Roma “La Sapienza”)

  • Fabrizio Di Mei

    (Università di Roma “La Sapienza”)

  • Aharon J. Agranat

    (Hebrew University of Jerusalem)

  • Claudio Conti

    (Università di Roma “La Sapienza”
    Institute for Complex Systems, ISC-CNR)

  • Eugenio DelRe

    (Università di Roma “La Sapienza”
    Institute for Complex Systems, ISC-CNR)

Abstract

A landmark of statistical mechanics, spin-glass theory describes critical phenomena in disordered systems that range from condensed matter to biophysics and social dynamics. The most fascinating concept is the breaking of replica symmetry: identical copies of the randomly interacting system that manifest completely different dynamics. Replica symmetry breaking has been predicted in nonlinear wave propagation, including Bose-Einstein condensates and optics, but it has never been observed. Here, we report the experimental evidence of replica symmetry breaking in optical wave propagation, a phenomenon that emerges from the interplay of disorder and nonlinearity. When mode interaction dominates light dynamics in a disordered optical waveguide, different experimental realizations are found to have an anomalous overlap intensity distribution that signals a transition to an optical glassy phase. The findings demonstrate that nonlinear propagation can manifest features typical of spin-glasses and provide a novel platform for testing so-far unexplored fundamental physical theories for complex systems.

Suggested Citation

  • Davide Pierangeli & Andrea Tavani & Fabrizio Di Mei & Aharon J. Agranat & Claudio Conti & Eugenio DelRe, 2017. "Observation of replica symmetry breaking in disordered nonlinear wave propagation," Nature Communications, Nature, vol. 8(1), pages 1-7, December.
  • Handle: RePEc:nat:natcom:v:8:y:2017:i:1:d:10.1038_s41467-017-01612-2
    DOI: 10.1038/s41467-017-01612-2
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